JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass...

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Data Bank ISBN 978-92-64-99087-6 The JEFF-3.1/-3.1.1 radioactive decay data and fission yields sub-libraries JEFF Report 20 M.A. Kellett International Atomic Energy Agency O. Bersillon Commissariat à l’énergie atomique R.W. Mills National Nuclear Laboratory © OECD 2009 NEA No. 6287 NUCLEAR ENERGY AGENCY Organisation for Economic Co-operation and Development

Transcript of JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass...

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Data Bank ISBN 978-92-64-99087-6

The JEFF-3.1/-3.1.1 radioactive decay data and fission yields sub-libraries

JEFF Report 20

M.A. Kellett International Atomic Energy Agency

O. Bersillon Commissariat à l’énergie atomique

R.W. Mills National Nuclear Laboratory

© OECD 2009 NEA No. 6287

NUCLEAR ENERGY AGENCY Organisation for Economic Co-operation and Development

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ORGANISATION FOR ECONOMIC CO-OPERATION AND DEVELOPMENT The OECD is a unique forum where the governments of 30 democracies work together to address the

economic, social and environmental challenges of globalisation. The OECD is also at the forefront of efforts to understand and to help governments respond to new developments and concerns, such as corporate governance, the information economy and the challenges of an ageing population. The Organisation provides a setting where governments can compare policy experiences, seek answers to common problems, identify good practice and work to co-ordinate domestic and international policies.

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This work is published on the responsibility of the Secretary-General of the OECD. The opinions expressed and arguments employed herein do not necessarily reflect the official views of the Organisation or of the governments of its member countries.

NUCLEAR ENERGY AGENCY The OECD Nuclear Energy Agency (NEA) was established on 1st February 1958 under the name of the

OEEC European Nuclear Energy Agency. It received its present designation on 20th April 1972, when Japan became its first non-European full member. NEA membership today consists of 28 OECD member countries: Australia, Austria, Belgium, Canada, the Czech Republic, Denmark, Finland, France, Germany, Greece, Hungary, Iceland, Ireland, Italy, Japan, Luxembourg, Mexico, the Netherlands, Norway, Portugal, Republic of Korea, the Slovak Republic, Spain, Sweden, Switzerland, Turkey, the United Kingdom and the United States. The Commission of the European Communities also takes part in the work of the Agency.

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FOREWORD

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 3

Foreword

The Joint Evaluated Fission and Fusion (JEFF) Project [formed following the merger of the Joint Evaluated File (JEF) and the European Fusion File (EFF) Projects in 1995] is a collaborative effort among NEA Data Bank member countries to develop a reference nuclear data library for use in different energy applications. The first version of the JEF series of libraries, JEF-1, was issued in 1985, followed in 1993 by a second version, JEF-2.2. In 2005, a completely revised third version, JEFF-3.1, was made available. In 2007, the updated JEFF-3.1.1 Radioactive Decay Data and Fission Yields Sub-libraries were also released.

This report describes the development, contents and initial validation of the JEFF-3.1 Radioactive Decay Data and Fission Yields Sub-libraries, including the 2007 update, JEFF-3.1.1, of these sub-libraries.

Many laboratories throughout Europe have engaged in the data evaluation, processing and validation phase. The main contributors to the decay and fission yields files were: CEA and LNHB, France; BNFL, UKAEA and Serco Assurance, United Kingdom; and the IAEA, Austria. Further support was received from the following national industries: COGEMA, Électricité de France and Framatome-ANP from France and British Nuclear Fuels Ltd from the United Kingdom.

The authors acknowledge the dedication of many colleagues in the nuclear data community to the project, without whom such work would not have been possible, in particular: M-M. Bé, J. Blachot, C.J. Dean, R.A. Forrest, T.D. Huynh, C. Mounier, A.L. Nichols, R.J. Perry, B. Roque, O. Serot and J-M. Vidal.

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TABLE OF CONTENTS

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Table of contents

Foreword.......................................................................................................................................................... 3

Introduction .................................................................................................................................................... 7

1 Radioactive decay data sub-library production .................................................................................. 9

1.1 Basic data source – NUBASE ........................................................................................................... 9

1.2 JEFF-3.1 – additional data sources .................................................................................................. 9

1.3 JEFF-3.1.1 – additional data sources ............................................................................................... 10

1.4 Library verification and allocation of material number .............................................................. 11

2 Radioactive decay data sub-library contents ...................................................................................... 13

2.1 Summary of the major decay modes in JEFF-3.1/-3.1.1 ............................................................... 13

2.2 Radiation following decay to a metastable state ......................................................................... 13

2.3 Atomic weights and natural abundances ..................................................................................... 14

2.4 Inclusion of total absorption gamma-ray spectrometry (TAGS) measurements .................... 14

2.5 Total number of neutrons per fission )( totalυ ................................................................................ 14

2.6 Values in JEFF-3.1 updated in JEFF-3.1.1 ........................................................................................ 14

2.7 Listing of the main parameters of JEFF-3.1.1 ................................................................................ 14

3 Fission yields sub-library production .................................................................................................. 15

3.1 Introduction ...................................................................................................................................... 15

3.2 Definitions ......................................................................................................................................... 15

3.3 Evaluation ......................................................................................................................................... 16

3.3.1 Fissioning systems ................................................................................................................ 18

3.3.2 Databases and data collection ............................................................................................ 18

3.3.3 Evaluation method ............................................................................................................... 19

3.3.4 Interpolation and extrapolation to fill gaps ...................................................................... 20

3.3.5 Fitting to constraints ............................................................................................................ 23

3.3.6 Isomeric yields ...................................................................................................................... 23

3.3.7 The calculation of cumulative yields ................................................................................. 24

3.3.8 JEFF-3.1.1: A correction to the JEFF-3.1 fission yields ....................................................... 24

4 Library testing and validation ............................................................................................................... 25

4.1 Delayed neutron yields and total energy release from fission .................................................. 25

4.2 Fission pulse decay heat calculations ........................................................................................... 25

5 Conclusions............................................................................................................................................... 35

References ....................................................................................................................................................... 37

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TABLE OF CONTENTS

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List of figures

1 JEFF-3.1 fission product mass distributions for seven fissioning systems..................................... 22

2 The calculated total decay heat (β + γ) from fission products following a 235U fission pulse compared to the Tobias Standard (1989) and as a ratio ......................................................... 29

3 The calculated total decay heat (β + γ) from fission products following a 239Pu fission pulse compared to the Tobias Standard (1989) and as a ratio ......................................................... 30

4 The calculated beta decay heat from fission products following a 235U fission pulse compared to the Tobias Standard (1989) and as a ratio ......................................................... 31

5 The calculated beta decay heat from fission products following a 239Pu fission pulse compared to the Tobias Standard (1989) and as a ratio ......................................................... 32

6 The calculated gamma-ray decay heat from fission products following a 235U fission pulse compared to the Tobias Standard (1989) and as a ratio ......................................................... 33

7 The calculated gamma-ray decay heat from fission products following a 239Pu fission pulse compared to the Tobias Standard (1989) and as a ratio ......................................................... 34

List of tables

1.1 Additional nuclei taken from ENSDF .................................................................................................. 10

1.2 Source libraries for JEFF-3.1/-3.1.1 ....................................................................................................... 10

1.3 Nuclei updated using TAGS average energy values .......................................................................... 11

2.1 Decay modes in JEFF-3.1/-3.1.1............................................................................................................. 13

3.1 Changes to cumulative yields for 235U thermal neutron-induced fission resulting from using JEFF-3.1 and JEFF-3.1.1 Radioactive Decay Data Sub-libraries ..................................... 17

3.2 The 39 fissioning systems in JEF-2.2 and JEF-3.1,-3.1.1/UKFY3.6A .................................................. 18

4.1 Average delayed neutron yields following a single fission calculated using JEFF-3.1 and JEFF-3.1.1 ......................................................................................................................................... 27

4.2 Average delayed energy emission following a single fission calculated using JEFF-3.1 and JEFF-3.1.1 ......................................................................................................................................... 28

Main data tables

A Atomic weights and natural abundances included in JEFF-3.1.1 .................................................... 39 B Updated average energy values from TAGS measurements in JEFF-3.1.1 ..................................... 45

C Total number of neutrons per fission )( totalυ ..................................................................................... 46

D Original JEFF-3.1 data, updated in JEFF-3.1.1 ...................................................................................... 47 E Main parameters of the JEFF-3.1.1 Radioactive Decay Data Sub-library ........................................ 51

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INTRODUCTION

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 7

Introduction

Radioactive decay data forms an integral part of the nuclear data requirements for nuclear applications The JEF-2.2 sub-library has been extensively used over the past 15 years or more and contains high quality data for 2 345 nuclides covering the needs of most reactor-based calculations. However, as energy ranges increase and new applications and regulatory requests emerge, nuclear data requirements also evolve; hence the need for the release of a new sub-library containing many more nuclei. At the time of its initial release, in May 2005, JEFF-3.1 was the most extensive decay data library available.

Following initial validation studies with the JEFF-3.1 Radioactive Decay Data and Fission Yields Sub-libraries, further revisions were made resulting in the JEFF-3.1.1 Radioactive Decay Data and Fission Yields Sub-libraries, released in 2007.

The construction, contents and some initial validation of the JEFF-3.1/-3.1.1 Radioactive Decay Data and Fissions Yields Sub-libraries is described.

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RADIOACTIVE DECAY DATA SUB-LIBRARY PRODUCTION

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Chapter 1: Radioactive decay data sub-library production

The Decay Data Sub-group of the JEFF Project decided that post-JEF-2.2 a completely new approach to creating a radioactive decay data library was necessary in order to fulfil the increased scope required by such a library, given the new applications and increased energy ranges in many facilities. The philosophy was to base this new library on data which was seen as representing the actual measured decay properties of each individual nuclide as accurately as possible, without the contamination of global adjustments or theories.

1.1 Basic data source – NUBASE

The basic skeleton of data was taken from the NUBASE-2003 file (Audi, 2003), which contains basic nuclear properties; hence all known isomers were identified from here. This file contains data such as half-life, spin, parity, excitation energy (in the case of metastable states), decay branching ratios and Q-values for all nuclei having experimental evidence of their existence. If a nuclide was not present in this file then it was deemed as not being significantly important for inclusion in the JEFF library, since it had not actually been measured. This is a perfectly sound assumption, given that the goal was to produce a library which was suitable for applications calculations. This exercise resulted in 3 852 nuclei being selected, of which 226 are stable. With recently accepted extensions to the ENDF-6 format (Herman, 2005), stable nuclei can also be entered into a decay data sub-library, meaning that the basic nuclear properties for these stable nuclei can also be included. This had been specifically requested by members of the JEFF Project involved in validation work.

A second important assumption in deriving the nuclei to be included was to ensure that the decay daughter(s) from any given nuclei would also be present. Hence ensuring that complete decay chains could be formed throughout.1

NUBASE contains basic nuclear property information and, in order that the JEFF library would be able to meet modern-day requirements for decay heat calculations, spectroscopy and activation analysis, many nuclei needed much more data, specifically decay radiation spectra. A number of additional source libraries, as described below, were then used in order to flesh out the initial NUBASE skeleton.

1.2 JEFF-3.1 – additional data sources

Three fully evaluated libraries, from within Europe, were used to replace individual NUBASE files, for almost 600 nuclei in all, with the extensive decay data information contained therein. These files tend to be the most comprehensive in both content and quality. Two libraries already in the ENDF-6 format (Herman, 2005) came from the United Kingdom [UKPADD-6.4 and UKHEDD-2.4 (Nichols, 2005)] and the other from France through the Decay Data Evaluation Project (DDEP) (Bé, 2004) maintained at the Laboratoire National Henri Becquerel (LNHB). The latter project’s data are made available via their website (Bé, 2004) in tabular form, but were made available to the authors in the ENSDF format (Tuli, 1987), before being converted into the ENDF-6 format with the SDF2NDF code (Bersillon, 2009).

Further files were also selected from the ENSDF library (Tuli, 1987) – these files contain decay data derived from basic nuclear structure data. Approximately 900 nuclei were selected after verification that they contained sufficient data to allow calculation of their energy balance to a consistency of

1. It should also be noted that in the production procedure of the fission yields data, the condition was imposed that only nuclei which existed in the decay data file could be created following a fission event.

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RADIOACTIVE DECAY DATA SUB-LIBRARY PRODUCTION

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better than 2%. During the early construction and initial testing phase, a small number of additional nuclei, with an energy balance inconsistency of greater than 2%, (see Table 1.1) were additionally converted from the ENSDF file and included into the JEFF-3.1 release, since the need for their spectral data was seen as critical in certain applications.

Table 1.1: Additional nuclei taken from ENSDF

Nuclei Material number Energy balance 38-Sr-93 0968 ~8.6%

41-Nb-101 1105 ~2.2% 50-Sn-126 1562 ~4.0% 51-Sb-131 1619 ~2.5% 52-Te-123 1652 ~2.7% 56-Ba-142 1862 ~3.0%

In a large number of cases for important nuclei, particularly fission products, several evaluations were available from the different sources given above. As such, a qualitative choice was made based on the comparison of the depth of information available in each source library. In each case a complete isotopic evaluation file was taken from the most appropriate source, hence it should not be assumed that data, such as half-life, are identical to those contained in NUBASE, for all of the nuclei present.

A complete breakdown showing the number of nuclei taken from each available source is shown in Table 1.2.

Table 1.2: Source libraries for JEFF-3.1/-3.1.1

Source JEFF-3.1 JEFF-3.11 Change NUBASE 2 351 2 310 -41 ENSDF 909 892 -17 LNHB 116 115 -1 UKHEDD-2.x 116 116 0 UKPADD-6.x 360 419 59 Total 3 852 3 852 0

1.3 JEFF-3.1.1 – additional data sources

The initial decay heat benchmarking of JEFF-3.1, along with the work of the OECD/NEA Working Party on International Evaluation Co-operation Sub-group 25 (WPEC-25) (Kellet, 2007), highlighted some problems in the individual prediction of the gamma and beta decay heat components, the total decay heat prediction being satisfactory. It was suggested that average energy values as determined through Total Absorption Gamma-ray Spectroscopy (TAGS) experiments could help to alleviate this situation. Hence a limited number of 29 nuclei (see Table 1.3) had their average energies updated from the high quality work of Greenwood, et al. (1997). The nuclei updated were only those where a detailed evaluation was not available, and hence the nuclei measured by this group were considered. Further evaluation work is required before the inclusion of data from the remaining nuclei measured can be considered. The WPEC-25 subgroup concluded that further TAGS experiments are merited and a list of appropriate nuclei was formulated. The inclusion of such data into a future version of the library will be considered as and when data become available on a case by case basis.

Additional nuclei were also available from the updating that had been made of the two libraries from the United Kingdom (UKPADD-6.7 and UKHEDD-2.5) (Nichols, 2007) providing a further fifty high quality detailed evaluations.

Hence, following the May 2005 release of the JEFF-3.1 library, and as a consequence of the initial decay heat benchmarking a moderately revised version, JEFF-3.1.1, was released in November 2007.

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Table 1.3: Nuclei updated using TAGS average energy values2

Material number Nuclide Material

number Nuclide

0929 37-Rb-90 2006 59-Pr-148 0930 37-Rb-90M 2007 59-Pr-148M 0931 37-Rb-91 2008 59-Pr-149 0970 38-Sr- 95 2010 59-Pr-151 1812 55-Cs-139 2053 60-Nd-153 1814 55-Cs-141 2054 60-Nd-154 1863 56-Ba-143 2055 60-Nd-155 1864 56-Ba-144 2098 61-Pm-152 1865 56-Ba-145 2101 61-Pm-153 1908 57-La-142 2102 61-Pm-154 1909 57-La-143 2105 61-Pm-156 1910 57-La-144 2106 61-Pm-157 1911 57-La-145 2149 62-Sm-157 1960 58-Ce-148 2150 62-Sm-158 2005 59-Pr-147

1.4 Library verification and allocation of material number

The JEFF-3.1 libraries store all data in the internationally accepted ENDF-6 format (Herman, 2005). Recent enhancements allowing the storage of basic nuclear properties for stable nuclei (i.e. spin, parity, atomic weight) were adopted, being the first library to do so. Also the isotopic abundances for all appropriate nuclei (taken from NUBASE-2003) have been added as the last line in the Comments section (MF=1 MT=451) as a more appropriate place in the format is not yet available. The isotopic abundances and atomic weights are listed in Table A (see Main data tables).

Throughout the construction process the library has been constructed and checked with the standard ENDF Utility Codes STANEF, CHECKR and FIZCON (Dunford, n.d.). Significant enhancements, implemented by members of the JEFF project, were added to the official FIZCON code v7.00 for the verification of decay data (Perry, 2003) and also minor corrections to the official versions (7.00/7.01) of both CHECKR and FIZCON were also implemented following problems noted in checking the JEFF-3.1 sub-library, most notably the checking of the symbol field for metastable states and the inclusion of stable nuclei. Users should be warned that earlier versions of the checking codes should not be used in testing this library.

The current versions of the JEFF-3.1 Radioactive Decay Data Library pass through the CHECKR utility code (v7.01) without a single error, other than that pertaining to the material number allocated. This can be completely ignored as the standard procedure within the ENDF-6 format for material number assignment is too limited to be implemented in this library. The material number is limited to 4 figures, where normally the first 2 are the atomic number of the nuclei in question and by allowing for 2 metastable states, only 33 isotopes may be entered per element based on incrementing the second 2 figures by 3 per ground state nuclei.3 Due to this limitation the nuclei in the JEFF-3.1/ 3.1.1 Radioactive Decay Data and Fission Yields Sub-libraries are simply numbered sequentially from 1 to 3 852, as many elements have more than 33 isotopes and a small number of isotopes have 3 metastable states.

The FIZCON code generates a small number of warning messages, most of which can safely be ignored. For others the messages relate generally to the limits of current knowledge as available at the time of the library construction. Future enhancements could well reduce their number.

As far as possible appropriate authors, laboratory codes and evaluation dates have been included in the files for the benefit of the user.

2. For details of the average energy values before and after the addition of the TAGS values, see Table B in the final section of this report – Main data tables. 3. For example the lightest stable isotope of the element with atomic number ZZ is given the material number ZZ25, then ZZ28 for the next isotope etc., e.g. 92-U-234 (the lightest stable isotope of uranium) is given 9225; 92-U-235 is then 9228; 92-U-235M is 9229, and so on with 92-U-236 given 9231; 92-U-237 given 9234 and 92-U-238 given 9237, etc.

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Chapter 2: Radioactive decay data sub-library contents

The JEFF-3.1/-3.1.1 Radioactive Decay Data Sub-libraries contain data for 3 852 nuclei, ranging from the neutron (0-nn-1) to roentgenium 272 (111-Rg-272), and include data for all experimentally observed nuclei – as determined from the NUBASE-2003 evaluation of nuclear and decay properties (Audi, 2003). Spectral data are provided for 1 480 nuclei in the JEFF-3.1 release and for 1 521 nuclei in JEFF-3.1.1, i.e. an additional 41 nuclei. A total of 226 stable nuclei are also included, i.e. nuclei for which no finite half-life has been determined.

2.1 Summary of the major decay modes in JEFF-3.1/-3.1.1

A summary of the number of nuclei decaying via one dominant decay mode is given in Table 2.1. The table gives the number of nuclei which decay via only one decay mode, or where all other minor decay branches contribute less than 0.01% of the total decay.

Table 2.1: Decay modes in JEFF-3.1/-3.1.1

Decay mode* JEFF-3.1 JEFF-3.11 β – 892 892 β+ 822 823 Α 243 243

Stable 226 226 IT 222 224 P 069 069 N 025 025

2β– 018 018 2p 012 012 2β+ 011 011 SF 009 009 2n 004 004 β+,p 002 002 Β–,n 001 001 β+,n 001 001

* Note that decays to the ground and metastable states have been summed for the sake of simplicity.

2.2 Radiation following decay to a metastable state

The decay data files have been constructed such that radiation from the subsequent decay of the metastable state of a daughter nuclide, populated from the initial decay of the parent nuclide, are contained in a separate file for that metastable state – this may differ from certain other decay data libraries.

For example, in the case of the 661.657-keV γ-ray following the 55-Cs-137 β–-decay, this line arises from the subsequent 100% internal transition of daughter 55-Ba-137M, and hence the data are to be found in the 55-Ba-137M file.

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2.3 Atomic weights and natural abundances

Basic nuclear property data (spin, parity, atomic weight, etc.) for the 226 stable nuclei, including natural abundances, are taken from the NUBASE-2003 evaluation. Table A1 lists the atomic weights and the natural abundances for the 226 stable nuclei, and the 61 extremely long-lived nuclei, i.e. typically having a half-life of 109 years or more and having a measurable natural isotopic abundance, present in the JEFF-3.1.1 library.2 The natural abundances are not currently included as part of the ENDF-6 format and so are included as the final line of the Comments section of each evaluation (MF=1 MT=451).

2.4 Inclusion of total absorption gamma-ray spectrometry (TAGS) measurements

Following some initial decay heat benchmarking of the JEFF-3.1 sub-library it was noted that significant differences were observable at various decay times between the gamma and beta components of the decay heat when compared with evaluated experimental data. The total decay heat predictions, however, compared favourably with experimental data. Thus the JEFF-3.1.1 sub-library was released, which includes updated values for the average energy release components based on values obtained via the Total Absorption Gamma-Ray Spectrometry measurements of Greenwood et al. (1997). A total of 29 nuclei were updated (see Table 2.3) with the numerical values provided in Table B.

2.5 Total number of neutrons per fission ( totalυ )

The library contains (in MF=1 MT=452) data for the total number of neutrons from fission for the 27 major spontaneous fissioning systems and these are listed in Table C, many of which are taken from (Manero, 1972) or systematics (further details are given in the individual Comments section for each evaluation).

2.6 Values in JEFF-3.1 updated in JEFF-3.1.1

Although the JEFF-3.1 library has now been withdrawn, for reference purposes, Table D lists the main parameters of the JEFF-3.1 release for those nuclei which were updated in JEFF-3.1.1 – other than for those nuclei adjusted through the inclusion of data from TAGS measurements, which are given in Table B.

2.7 Listing of the main parameters of JEFF-3.1.1

A complete listing of the main parameters of the JEFF-3.1.1 Radioactive Decay Data Sub-library is given in Table E, i.e. the allocated material number (from 1 to 3 582), nuclide symbol (including both atomic and mass numbers, plus metastable state designation, e.g. 11-Na-24M), spin and parity, excitation energy (in eV) for the metastable states, half-life (with the percentage uncertainty), decay modes and branching fractions (expressed as a percentage), number of radiation spectra included in the library for that nuclide, average light-particle, electromagnetic and heavy-particle energies (in eV) and finally the original source library of the evaluation. The half-lives are all stored in the ENDF-6 format in seconds, but for convenience are given in this table in the most appropriate unit, where the number of seconds in a year is that used in NUBASE-2003, i.e. 1 year = 365.2422 days = 31 556 926 seconds.

1. Tables A, B, C, D and E are presented in the final section of this report – Main data tables. 2. Note that due to an incorrect conversion factor, the atomic weights given in the now-withdrawn JEFF-3.1 library are inaccurate and should not be used.

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FISSION YIELDS SUB-LIBRARY PRODUCTION

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Chapter 3: Fission yields sub-library production

This chapter summarises the methodology underlying the JEFF-3.1 fission product yield evaluation, which was adopted from the United Kingdom evaluation UKFY3.6A.

Note that the JEFF-3.1/-3.1.1 Fission Yields Sub-library is actually two distinct sub-libraries within the Evaluated Nuclear Data File (ENDF) format, one for neutron-induced fission (NFY) and the other for spontaneous fission (SFY). However, as these two distinct sub-libraries are evaluated within one unique system, and tend to be used simultaneously in most applications, they are generally referred to in the singular as the JEFF-3.1 (or JEFF-3.1.1) Fission Yields Sub-library.

3.1 Introduction

In the United Kingdom the evaluation of fission product yields for use in computer libraries was pioneered at Harwell in the 1960s (Crouch, 1977, 1985). Development of these has continued to the present day. The UKFY1 library (Banai, 1987) was adopted for JEF-1 after detailed review (James, 1987). Subsequent work produced UKFY2, which was adopted for JEF-2. The UKFY2 evaluation including methodology, experimental data and review of discrepancies is described in three reports (James, 1991, 1991a, 1991b). The UKFY3.6A library is a continuation of this work and is based upon UKFY3 (Mills, 1995). The library is in the ENDF-6 format. Both independent (pre-delayed neutron emission) and cumulative (post-delayed neutron emission) yields are available, together with their standard deviations.

3.2 Definitions

The atomic number and mass number of the fissioning nucleus are denoted by Zf and Af respectively. For the neutron-induced fission of a nuclide of mass number Atarget, Af = Atarget + 1, while for spontaneous fission, Af is the mass number of the fissioning nuclide. The subsequent fission product nuclide is specified symbolically by the triplet (A,Z,I), where A and Z are respectively the mass number and atomic number, and I indicates the isomeric state (I = 0 for the ground state, I = 1,2,… for the first, second,… metastable states). If a fission product has no isomers, or if we are referring to the sum of yields for all its isomers, we use the doublet (A,Z).

The independent yield y(A,Z,I) is the number of atoms of (A,Z,I) produced directly from one fission, after the emission of prompt neutrons (but before the emission of delayed neutrons). It can be written as the product of three factors:

y(A,Z,I) = Y(A) f(A,Z) R(A,Z,I)

where the sum yield Y(A) is the sum of independent yields (before delayed neutron emission) of all fission products of mass number A; f(A,Z) is the fractional independent yield of all isomers of (A,Z); and R(A,Z,I), the isomeric yield ratio, is the fraction of (A,Z) produced directly as isomer I.

From the definition, it follows that:

( )∑ =Z

AZf 1 for all A

and:

( )∑ =I

I,Z,AR 1 for all (A,Z)

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so that:

( ) ( )∑=ZI

I,Z,AyAY for all A

The usefulness of these formulae derives from the fact that, with the exception of delayed neutron (β–,n) emission and the few very long-lived α decays, all the radioactive decays of fission products are β– or β+, or isomeric transitions, and in none of these is A altered. Thus, to a very good approximation, the fission products can be considered as belonging to distinct mass chains.

The cumulative yield c(A,Z,I) of (A,Z,I) is the total number of atoms of that nuclide produced over all time after one fission. If the nuclide is stable and at the end of a mass chain, the cumulative yield is the total number of atoms remaining per fission, and is termed the chain yield Ch(A).

Similarly, for a nuclide with a much longer half-life than any of its precursors, c(A,Z,I) is very nearly equal to the amount of it produced at a time short compared to its half-life but long compared to those of its precursors. However, for a radioactive nuclide for which this is not the case, some atoms will have decayed before all have been produced, so that at no time will there actually be c(A,Z,I) atoms per fission present. An equivalent definition that is more useful is the following: immediately at the end of an “infinite” irradiation at the rate of 1 fission per second, c(A,Z,I) is the rate of decay of (A,Z,I) if that nuclide is radioactive, or its rate of production if it is stable. Consequently cumulative yields are useful in computing total fission product decay energies and delayed neutron emission rates.

The sum yield Y(A) and the chain yield Ch(A) for a mass chain A may differ by a few per cent, because the former applies before, and the latter after, delayed neutron emission. Tables of the calculated differences for each chain of some fissioning systems are provided in James (1991).

3.3 Evaluation

Many of the problems encountered in this work are found to a greater or lesser extent in any evaluation. To be generally useful, any data library must be as accurate and as complete as possible. Accuracy requires an up-to-date and complete compilation of experimental results, as well as a statistically sound method of treating the measurements and of considering the inevitable discrepancies between some of them. Completeness demands considerable care in interpolation and extrapolation to fill the equally inevitable gaps where there are no measured data at all. Since a user needs to know the accuracy of the data, it is also necessary to estimate as carefully as possible the standard deviations of the evaluated data. This last task is sometimes the longest and hardest. The database, evaluation methods and the interpolation of data and parameters are considered below.

Fission product yield nuclear data should satisfy some simple conditions arising from physical conservation laws of nucleon number and of charge. Different evaluating teams use these conditions differently: either to adjust the data, or, if they have not been used for adjustment, as tests subsequent to the evaluation process. There are essentially four such conditions applied to JEFF-3.1:

1) The complete independent yield distribution for all A and Z, apart from those of the relatively rare light products from ternary fission, should sum to 2.

2) There should be conservation of nucleon number; this must include the ternary products.

3) There should be overall conservation of charge, before beta decay. Again this must include the ternary products.

4) There should be detailed conservation of charge giving equal yields of complementary elements. The complementary element is the charge of the other fragment during an individual fission, due to conservation of charge, this is equal to Zf – Z.

These apply to the total independent yield of a nuclide, being the sum of all isomers. The experimental values of the ratios of independent yields of isomeric to ground states were reviewed and the method of Madland and England (1976) was used to calculate ratios for which there were no measurements.

The calculation of cumulative from independent yields requires data on branching ratios of radioactive decays, including all daughters. In this work, these were all obtained from the JEFF-3.1

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decay data library. It should be noted that some revisions in JEFF-3.1.1 changed a few of the decay paths. Table 3.1 contains a comparison of calculating cumulative yields calculated using the JEFF-3.1 independent fission product yields and the two decay data libraries for the thermal neutron induced fission of 235U. As can be seen very few nuclides have significant changes.

Table 3.1: Changes to cumulative yields for 235U thermal neutron-induced fission resulting from using JEFF-3.1 and JEFF-3.1.1 Radioactive Decay Data Sub-libraries

Nuclide JEFF-3.1

independent yield

JEFF-3.1 cumulative yield calculated with

the JEFF-3.1 decay data

JEFF-3.1 cumulative yield calculated with the JEFF-3.1.1

decay data

Ratio of cumulative yields

JEFF-3.1.1/ JEFF-3.1

29-Cu-70 4.2598E-10 3.4918E-09 3.6087E-09 1.033467 29-Cu-70M 4.7457E-09 6.1317E-09 6.6306E-09 1.081372 34-Se-81 8.5771E-06 1.9749E-03 1.9749E-03 0.999990 39-Y-89M 2.8162E-09 4.5232E-06 4.5236E-06 1.000096 40-Zr-90M 6.5152E-12 7.9587E-12 6.5152E-12 0.818627 40-Zr-96 2.6209E-03 6.3014E-02 6.3017E-02 1.000056 39-Y-97 6.1878E-03 2.0797E-02 2.0804E-02 1.000351

39-Y-97M 2.1091E-02 2.8144E-02 2.9187E-02 1.037051 40-Zr-97 9.3696E-03 5.9932E-02 5.9929E-02 0.999941 41-Nb-97 5.5298E-05 6.0001E-02 5.9997E-02 0.999941

41-Nb-97M 1.2786E-05 5.6977E-02 5.6974E-02 0.999941 42-Mo-97 3.4773E-08 6.0001E-02 5.9997E-02 0.999941 46-Pd-111 5.1161E-08 1.9679E-04 1.9700E-04 1.001081

46-Pd-111M 9.6149E-08 8.8367E-07 9.6149E-08 0.108807 47-Ag-111 6.1306E-12 1.9605E-04 1.9605E-04 0.999999

47-Ag-111M 4.0103E-11 1.9557E-04 1.9563E-04 1.000307 47-Ag-113 1.2008E-08 1.0456E-04 1.0500E-04 1.004160

47-Ag-113M 7.8549E-08 1.5279E-04 1.5158E-04 0.992092 48-Cd-113 5.7767E-12 1.5776E-04 1.5776E-04 0.999952

48-Cd-113M 1.8899E-11 1.8078E-06 1.8153E-06 1.004160 49-In-113 0.0000E+00 1.8053E-06 1.8128E-06 1.004160 49-In-119 9.1291E-07 5.6166E-05 5.6164E-05 0.999967

49-In-119M 2.1109E-07 9.9853E-05 9.9855E-05 1.000020 50-Sn-119M 1.0024E-09 5.0741E-05 5.0740E-05 0.999967 48-Cd-121 2.3876E-05 4.5842E-05 4.5718E-05 0.997299

48-Cd-121M 5.7641E-05 6.0204E-05 6.0328E-05 1.002056 49-In-121 1.5995E-05 9.2048E-05 9.1625E-05 0.995406

49-In-121M 3.6985E-06 3.4101E-05 3.4529E-05 1.012552 50-Sn-121 7.8096E-08 1.2363E-04 1.2364E-04 1.000087

50-Sn-121M 1.8853E-07 1.0616E-05 1.0568E-05 0.995487 50-Sn-129 1.7575E-03 2.3102E-03 2.3101E-03 0.999963 51-Sb-129 2.8285E-04 5.0887E-03 5.7823E-03 1.136310

51-Sb-129M 1.7285E-04 2.3204E-03 1.5044E-03 0.648318 52-Te-129 1.7810E-08 6.0359E-03 6.2439E-03 1.034461

52-Te-129M 4.2997E-08 2.7707E-03 2.2085E-03 0.797101 51-Sb-130 2.5080E-03 1.0810E-02 9.3231E-03 0.862423

51-Sb-130M 2.5080E-03 6.5646E-03 8.0519E-03 1.226558 66-Dy-158 0.0000E+00 1.5878E-13 1.6069E-13 1.012048

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3.3.1 Fissioning systems The selection of fission systems in the United Kingdom libraries is based on objective criteria. A series of calculations were made with the inventory code FISPIN, described by Burstall (1979), and its 1988 libraries for both thermal and fast reactors. For the former, initial fuelling by enriched uranium, recycled uranium, mixed plutonium/uranium and thorium/uranium, were individually considered. The ratings and irradiations applied to the calculations were greater than actually achieved in current reactors, but were values regarded as feasible in the future. Reactions were regarded as important if they contributed more than 0.1% of the fission rate at any time. Thus, it is thought that the derived list is more than adequate for some time to come. It does, of course, depend on the initial fuel compositions and on the assumed capture and fission cross-sections for the higher actinides; it is acknowledged that some of the latter may be considerably in error.

In addition, the library includes fission of 232Th, 233U, 235U and 238U by “high energy” (about 14 MeV) neutrons from fusion; these reactions were in the earlier United Kingdom libraries. We have also included the yields from the spontaneous fission of 242Cm and 244Cm which are important as sources of neutrons in reactors and in fuel handling, and of 252Cf, which is important as a standard.

The complete set is given in Table 3.2 below. The reactions considered by the reactor calculations are given in three sub-sets, in the three left-hand columns. These are distinguished by the value of the maximum fission rate percentage due to the nuclide in question at any time during the irradiation. (The range in which the percentage falls is indicated in the column heading.) Clearly, the required accuracy of yields is greater if the percentage fission rate is greater.

Table 3.2: The 39 fissioning systems in JEF-2.2 and JEFF-3.1,-3.1.1/UKFY3.6A

Maximum fraction of fission rate Spontaneous fission >10% 1-10% 0.1-1%

Nuclides: 5 2 12 3 233U* TFH 235U* TFH 238U* FH 239Pu TF 241Pu* TF

240Pu* F 245Cm TF

232Th* FH 234U F 236U F 237Np TF 238Np TF 238Pu TF 242Pu F 241Am TF 242mAm TF 243Am TF 243Cm TF 244Cm TF

252Cf Sp 242Cm Sp 244Cm Sp

* Nuclides in UKFY1 and previous United Kingdom libraries (James, 1991, 1991b). T Thermal fission. F Fast fission. H 14 MeV fission. Sp Spontaneous fission.

3.3.2 Databases and data collection The database used for the UKFY3.6A evaluation consisted of three files containing data measured absolutely, relatively, and by “ratio of ratio” methods. The most straightforward of these are the absolute measurements, in which the yield of a nuclide per fission is measured. However, this method requires knowledge of the number of fissions, which can be difficult to determine practically. In the second type, a nuclide with a yield that is assumed to be accurately known is used to estimate the number of fissions. Thus, the unknown yield is determined relative to the standard yield. The third type of measurement uses the “ratio of ratio” or “R-value” method. This assumes that the yields of both the fission product of interest and a monitor fission product are known from a reference fission reaction. Then, if the yield of the monitor is also known from the fission reaction of interest, the yield of the unknown yield from the reaction of interest can be found.

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The evaluation proceeded in iterative stages. In the first, only absolute measurements were used. In the subsequent steps, the two types of relative measurements were included as well, if they could be converted to absolute yields using the results of the previous step. Iterations were repeated until no further results could be converted.

Experimental fission yield data were collected from three computer readable sources:

1) Crouch’s fission yield database, which was used in the Crouch (1977) and the Banai, et al. (1987) evaluations.

2) A database of recent references, produced after a thorough search of recent literature 1993.

3) The international database EXFOR is described by Lemmel (1996); the last complete update for UKFY3 was received in June 1993. Some newer individual entries were added in 2005.

The combined UKFY3.6A database contains 12 109 absolute measurements, 1 342 relative measurements and 1 480 ratio of ratio measurements. The analysis resulted in 13 776 usable absolute measurements. This contains 85% more items of data than that used by Crouch (1977).

As in previous work the measurements were examined to remove duplications and to ensure consistency of isomeric states. In the evaluation, discrepant data were extensively examined to remove entry errors and to increase some unacceptably low estimates of error.

3.3.3 Evaluation method

General treatment of measurements

The experimentalists’ uncertainties were adjusted, in the previous United Kingdom evaluations, to be always greater than 5% (Crouch, 1977), unless significant justification was present in the reference. Throughout this work all uncertainties are quoted at the 1 standard deviation level. Considering the more accurate measurements now possible, this limit has been reduced. The revised rules used in attributing input uncertainties are stated here.

• For recent mass-spectrometric measurements, the quoted uncertainty was used provided it was not less than 1%. Otherwise, 1% was used, unless there was good justification for the published value in the reference.

• For other types of measurement, the quoted uncertainty was used provided it was not less than 5%. Otherwise, 5% was used, unless there was good justification for the published value in the reference.

• Mass-spectrometric results quoted without any estimate of uncertainty were given a standard deviation of 10%.

• Other results quoted without any estimate of uncertainty were given a standard deviation of 15%.

These standard deviations were used to obtain weighted means using inverse variance weighting. Both internal and external standard deviations of the mean were determined in the analysis and the larger of these were used for subsequent calculations. From χ2 and the number of degrees of freedom, the probability of the data not being consistent can be calculated. Those with a probability of less than 10% were listed in a set of discrepancy tables, values less than 1% and 0.01% being flagged for special consideration. In these cases, the data were checked for transcription errors between the quoted values in the references and the values in the database. Next, the relevant papers were studied to see if there were reasons for re-normalising or down-weighting the measurements.

Consequently, after references had been checked, an automatic down-weighting procedure was applied to the data to reduce major discrepancies. This technique was based upon the normalised residual, which should normally be distributed with a mean of zero and a standard deviation of unity. Each component of the normalised residual |Ri| was constrained to be less than 2.5, for all yields with more than two measurements, by down-weighting the measurement with the largest value. If the maximum |Ri| was greater than 2.5 the variance was adjusted to give Ri equal to 2.5, and then the averaging process was repeated. This procedure reduces the weight of points far from the mean, thus reducing the effect of discrepant data on the weighted mean. The theoretical justification for these

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definitions and statements is given in (James, 1991c). It should be emphasised that the automatic down-weighting described here (or any alternative method) should not be used in preference to a detailed analysis of the original measurements.

Separate analyses were made for chain, fractional independent and fractional cumulative yields. From these evaluations, sets of mean chain yields, fractional independent and cumulative yields with standard deviations were produced that could be used as input in the fitting of semi-empirical models as described below.

Chain yields

Measurements were included both of a chain yield itself and of cumulative yields of nuclides close enough to the end of the decay chain, and with sufficiently small independent yields, for their cumulative yields to be good approximations to the chain yield. As several chains have nuclides with isomers near the stable end, it is possible to apply the method of least-squares to the measurements and the branching ratios to improve the estimate of the chain yield and its uncertainty (James, 1991; Mills, 1995).

Fractional independent and cumulative yields

For nuclides away from the stable ends of mass chains, measurements may be of either fractional or of absolute yields: the former being obtained if the same experiment also determines the chain yield. For the present purpose, fractional yields were required, so absolute values in the database were converted by dividing by the evaluated (unadjusted) mass yield. The latter was either the experimental mass yield average (see above) or obtained from a fit to the mass yield distribution.

3.3.4 Interpolation and extrapolation to fill gaps

General

To produce independent and cumulative yield libraries for reactor and decay heat calculations, all significant chain yields and fractional independent yields need to be known. About 120 chain yields are required (mass 60 to 180) for these purposes. As even the system with the best coverage of measurements, 235U thermal, has only 111 measured chains and some systems (for example 243Am) have none, a model or method of prediction is required for chain yields. Similarly, if fractional independent yields greater than 10–8 are considered to be important, approximately 900 are required, whereas even for 235U less than 250 have been measured. There are several semi-empirical models and methods of interpolation or extrapolation for fractional independent and chain yields which can be used.

Chain yields

In UKFY3.6A the mass-yield curve is fitted by a set of Gaussians, as proposed by Musgrove, et al. (1973) and used more recently by Dickens (1987). This technique is based upon the apparent similarity of the chain yield distributions to Gaussian distributions. This method can be readily used to predict yields from systems on which few or even no measurements have been made.

We have followed Musgrove, et al. (1973) in using five Gaussians (viz. two for each peak of the mass distribution, and one for near-symmetric fission). More recently theoretical justification for such a multiple Gaussian fit has been attempted; see for example Brosa, et al. (1990). The 15 parameters (strength, mean and width of each Gaussian) were reduced to 8 by assuming symmetry and requiring a total yield of 2. This model gives the chain yield Y(A) as:

( ) ( ) ( )

( ) ( )

( ) 23

2

22

22

22

22

21

21

21

21

2

3

3

22

2

2

22

1

1

2

2

2

σ−−

σ+−−σ−−−

σ+−−σ−−−

πσ+

⎥⎦⎤

⎢⎣⎡ +

πσ+

⎥⎦⎤

⎢⎣⎡ +

πσ=

AA

DAADAA

DAADAA

eN

eeN

eeN

AY

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where Ni is the strength coefficient of the ith Gaussian and σi its width parameter, A is the mean mass of the distribution and Di is the separation of the ith Gaussian peak from A. Because the chain yields sum to 2: N3 = 2(1-N1-N2).

The analysed chain yields were fitted to this model, and the values of the parameters for systems for which there were sufficient data for satisfactory fits are given in Mills (1995). The fits for 235U thermal and fast, 233U thermal and 239Pu thermal are shown in James, et al. (1991), Figures 2-5. This five-Gaussian representation smoothes the distribution, removing both experimental noise and the expected small odd-even fluctuations.

To extend the five-Gaussian representation to systems with sparse data, the parameters already obtained were plotted against fissioning mass and charge, and fitted by linear or quadratic functions of Af. (No systematic trend with Zf could be detected.) New five-Gaussian fits were made to the chain yield data, allowing only one of the parameters to vary in turn. Linear or quadratic fits were then made to each of the varied parameters, with the functions of Af. After all parameters had been fitted in this manner, the whole process was repeated. After two iterations the refitting procedure failed to produce any improvement in χ2. The functions obtained are given below and can be found in James, et al. (1991) and Mills (1995).

( ) ( )

( ) ( )012

2300012502305950919

37524112502860

2300136640230678320127

9064220170

][4579000105630

][6215000038460

][2

3

22

2

2

21

1

1

1

.

A.A..D

.A.

.N

A.A..D

.A.

thermal.A.N

fast.A.N

onconservatinucleonbyfixedA

A

ff

f

ff

f

f

f

pf

=σ−+−−=

−=σ=

−+−−=

−=σ

+=

+=

ν−=

Although this is a simple model and the goodness of fit to the parameters only moderate, reasonable results were obtained when chain yields were calculated for systems using these predicted Gaussian parameters when compared with experimental data, see figures in report (James, 1991).

In UKFY3.6A chain yields were first taken from the experimental averages. Then gaps were filled using the five-Gaussian model with the fitted parameters if appropriate, or obtained from the above equations if not. The predictions from this model were modified before being used to produce complete data sets. First, the central Gaussian was not allowed to contribute outside the two main peaks (to avoid unrealistic flaring of the distribution at very low yields). Secondly the predictions were re-normalised with the experimental data. This re-normalisation considered the two cases of: (a) the wings of the distribution; (b) gaps in the experimental data. The predictions in the wings, up to the first experimental point, were re-normalised by a constant factor so that for this point the predicted yield equalled the measured value. In gaps, predicted yields at each end were fitted to measured values by making the logarithm of the normalisation factor vary linearly with mass across the gap. This procedure gave a complete set of chain yields for each fissioning system based as firmly as possible on experimental data. Graphs of these chain yields are given in reports (James, 1991; Mills, 1995) for some of the 39 fissioning systems considered.

In UKFY3.6A it was found that some systems (252Cf spontaneous and 238Pu thermal neutron induced) had unphysical shapes when the above procedure was performed. The 252Cf was corrected by re-fitting the data using a spreadsheet and the 238Pu by using the predicted parameters rather than the explicit fit. It was also discovered that some experimental data, because of the model re-normalisations, were skewing the distributions in some systems with only a few measurements, especially in Cm fissioning systems. This was solved by ignoring the few experimental measurements that lead to the skewed distributions.

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Figure 1 shows the mass distributions for several fissioning systems in JEFF-3.1. These slopes show three features. First, it should be noted that as the mass of the compound nucleus increases the lower mass peak moves to higher masses, but the higher mass peak remains almost stationary. Second, the depth of the valley between the peaks decreases with compound nucleus excitation energy. Finally, the upper edge of the higher mass peak falls off with a greater slope for lower compound nucleus masses.

Figure 1:JEFF-3.1 fission product mass distributions for seven fissioning systems

Fractional independent yields

The fractional independent yields were fitted by the Zp model, developed and described by Wahl (1985, 1988 and references therein). This model represents the fractional independent yields as Gaussian distributions in charge for a given mass, modified by an odd-even effect.

We used the same Zp model parameterisation as Wahl. This considered the independent yields of each mass to be a Gaussian distribution, centred on a mass ΔZ from the unchanged charge distribution approximation, which assumes the charge to mass ratio of the fragments are the same as the compound nucleus. The distribution has a width σ and an odd-even effect with charge and mass. Trends in these parameters for the different mass chains were fitted by relatively simple functions of mass number. Around symmetrical fission the ΔZ and σ undergo rapid changes described by Wahl (1985, 1988).

To fit Wahl’s parameterisation it was necessary to have the number of neutron emitted on average from each fragment mass νp (A). For 235U thermal the values for νp (A) were taken from Wahl (1988), and for other reactions the 235U thermal values re-normalised to give the appropriate total νp. Using similar techniques to Wahl a least-squares fit of the parameters to the analysed experimental data was used. The input yields to the least-squares fit were constrained to have uncertainties of 5% or greater to stop a few highly-weighted values dominating the fit. As small yields in a chain are difficult to measure, a lower limit was set on the fractional yields that were fitted at the point where the reduced χ2 rapidly diverged. For 235U thermal it was possible to fit all the parameters. However, for other reactions, it was not possible to fit some parameters as there are no significant data in the region near symmetric

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fission. Therefore the 235U thermal values for these parameters were used and only the five other parameters varied in the fits; even so only four fissioning systems were able to be fitted. The fitted parameters were then extrapolated for the other fissioning systems. The complete analysis is described in Mills (1995).

Ternary yields

The main requirements for ternary yields are yields of 4He and 3H for all the systems. This was achieved using the work of Serot, et al. (2004). Also where the UKFY3.6A database contained measurements of other yields these were included in the evaluated file, but it should be noted that these have not been analysed with the rigor that Serot, et al. extended to 4He and 3H. It should be noted that recent work has shown that the tritium produced in spent nuclear fuel from activation of other ternary products, principally 6Li, adds about 10% to the tritium produced (Mills, 2006). Thus it is necessary to improve the ternary yields in future files to better estimate tritium production.

3.3.5 Fitting to constraints Using the evaluation methods described above, a library in ENDF-6 format can be produced. However, as was pointed out, there are constraints that must apply to the yields due to the conservation of nucleons and charge.

In UKFY3.6A all constraints applying to the whole yield distribution were applied, and for the elements with the greatest yields constraints governing complementary pairs of elements were applied. The number of complementary pairs of elements considered being increased until the reduced χ2 did not excessively exceed unity or, where reduced χ2 was always greater than 1.0, the number of pairs was chosen to be that which gave a minimum value. The values of νp, used in the adjustment, are given in James, et al. (1991). It should be noted that only in a few cases are adjustments made greater than two standard deviations, and most adjustments are relatively small.

It is worth noting that the formulae for interpolation and extrapolation of chain and fractional independent yields described above are designed to satisfy the physical constraints. Consequently it was generally the case that greater percentage adjustments were needed for those fissioning systems that had more measured yields and thus more experimental noise in the data. Although, of course, values determined from experimental data have smaller uncertainties than values determined from systematic methods.

3.3.6 Isomeric yields So far, the evaluated independent yields considered have been those of nuclides including all isomeric states and we have ignored the division of the independent yield of a nuclide between its isomers. To allow for such a division for a nuclide with a single excited state m and ground state g, we define the isomeric yield ratio r(A,Z,m) given by:

( )( ) ( )m,Z,Ayg,Z,Ay

m,Z,Ay

+

Where possible, experimental data were used for the r(A,Z,m). There are two types of such measurements; first, direct determination of this ratio in a single experiment and second, determining the ratio from several independent experiments. Preference was given to direct measurements of the ratio, as these are free of normalisation problems and less likely to have confusion of the spin states. However, measurements of either kind were found to be sparse, so that recourse had to be made to theory.

In this work the method of Madland and England (1976) was used, as it requires minimal information (the spins of the excited and ground states) about the nuclide; even that was sometimes uncertain, but generally we relied on the spin data in the JEFF-3.1 decay data file. Nuclides with three or four isomeric states (including the ground state) were considered using a simple extension of the Madland and England model (Mills, 1995).

Using the above methodology it is possible to produce complete sets of adjusted independent yields, however, the ENDF-6 format requires that cumulative yields also be produced.

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FISSION YIELDS SUB-LIBRARY PRODUCTION

24 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

3.3.7 The calculation of cumulative yields The concept of the cumulative yield, c(A,Z,I), of the nuclide (A,Z,I) is described above. It should be noted that cumulative yields are derived parameters and in measuring these, account must be taken of the decay paths and half-lives of precursors. Only in a few special circumstances, where all a nuclide’s precursors are much shorter lived than it and no significant neutron reactions need to be taken into account, can the cumulative yield be used for practical calculations. First, it is reasonable, in practical applied files, to ignore the very long-lived α decays (144Nd [half-life 2.4 × 1015 years] and 147Sm [half-life 1011 years]), as these will lead to an apparent approximate doubling of the cumulative yields of the daughters (140Ce and 143Nd) which, because of the times involved, is absurd for applied nuclear industry applications. Other similarly long-lived β decays and other decays with half-lives greater than 1 000 years (3.16 × 1010 seconds) have also been removed in the calculation of cumulative yields in both JEF-2.2 and JEFF-3.1. Greater problems arise with half-lives of say 1-100 years, i.e. of the same order as irradiation or storage times. Because of these problems it is recommended that cumulative yields should be used only rarely; the safer method is always to use independent yields with an inventory code that correctly treats all relevant types of decay, and also permits the consideration of neutron, or other transmutation, reactions that produce and destroy the nuclide.

Cumulative yields are useful in some special applications, for example, in calculations of total delayed neutron emission and total energy release by decay following fission. This is because of the property of cumulative yields that at the end of long irradiations most radioactive nuclides are in equilibrium with their precursors and their production rate is thus equal to their decay rate. Of course, very long-lived nuclides never reach equilibrium, but due to their half-lives have very little effect on the results.

The easiest way to calculate cumulative yields is to use the Q-matrix approach described by James, et al. (1991), where the cumulative yield of nuclide j is calculated from the independent yields:

∑=i

ij,ij yQc

In UKFY3.6A, the Q matrix was determined from the JEFF-3.1 decay data, using the method of James, et al. (1991). The uncertainties of the cumulative yields were determined from the uncertainties on both the adjusted independent yields and the experimentally based chain yield. Using a least squares approach the uncertainty on the cumulative yield, δc, is approximated by:

2

j

2

iij,i

j

j ChCh

cyQ)

Ch

c1(c ⎟⎟

⎞⎜⎜⎝

⎛∂+⎟⎟

⎞⎜⎜⎝

⎛∂−=∂ ∑

where Ch is the chain yield of the mass chain containing the cumulative yield cj. As the adjustment procedure alters the cumulative yields, the difference between an adjusted and unadjusted cumulative yield was added to the cumulative yield’s uncertainty.

3.3.8 JEFF-3.1.1: A correction to the JEFF-3.1 fission yields Following the release of the JEFF-3.1 fission yields an inconsistency was noted between the cumulative and independent yields for 235U thermal fission (Vidal, 2007). The independent yield of 137I is in the file as 2.9508E-2 instead of 3.0976E-2. This was the result of an incorrect unit conversion in the modification of UKFY3.6 to produce UKFY3.6A. This has no effect on the cumulative yields in the JEFF-3.1 file which are correct. However, if using this file for inventory calculations based upon the independent yields, the 137Cs (half-life of 30 years) and 136Xe (stable) from 235U thermal neutron fission will be under predicted by 2.2% and 0.145% respectively. A revision of the JEFF-3.1 file is available on the JEFF-3.1 feedback page (www.nea.fr/html/dbdata/jeff3feedback/feedback-31.html) or as JEFF-3.1.1.

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THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 25

Chapter 4: Library testing and validation

The library has undergone some initial testing and validation, the results of which are discussed here. The library has been readily integrated into existing code systems owing to its strict adherence to the recognised ENDF-6 format. Since the library also contains data for all nuclei of interest in most envisaged domains, no extra data are required from other sources. This was often not the case for the JEF-2.2 library where additional libraries were required to provide supplementary data.

4.1 Delayed neutron yields and total energy release from fission

As described previously it is possible to use cumulative yields and decay data to calculate total delayed neutron yields and the total emitted energy following fission. The results of such calculations are shown in Tables 4.1 and 4.2 for the JEFF-3.1 fission yields, with decay data from JEFF-3.1 and JEFF-3.1.1. Where possible the results are compared with experimental values.

The delayed neutron results are given in Table 4.1. It should be noted that no significant differences arise from calculations with the JEFF-3.1 and JEFF-3.1.1 decay data library. These results are to be expected as the changes implemented in the decay data between JEFF-3.1 and JEFF-3.1.1 do not affect this particular calculation. As cumulative yields are used in the calculations the incorrect 137I independent yield has no effect on these results.

The calculations of the total emitted energy following fission are shown in Table 4.2 and show a reduction in the lepton energy of about 1-2% and an increase in the photon energy of about 1-3% for all systems. These results were to be expected as the incorporation of new average energy release data was the major part of the development of JEFF-3.1.1. Again cumulative yields are used in this calculation and thus the incorrect 137I independent yield has no effect on these results.

4.2 Fission pulse decay heat calculation1

Additionally, some comparisons were made using the JEFF-3.1/-3.1.1 data against fission pulse decay heat measurements. For rapid reactor transients, the prediction of decay heat is important in the range of seconds to minutes. Comparisons are thus most useful for irradiated samples of pure fissile nuclides cooled for these short periods. Tobias reviewed the status of decay heating in 1980, using 45 sets of experimental measurements. Tobias later updated this work (1989) using simultaneous least-squares fit to beta, gamma and total decay heat measurements for both 235U and 239Pu. This analysis considered 54 sets of 235U measurements and 28 sets for 239Pu. The results of the least-squares analysis were decay heat functions following a single fission event for both nuclides.

Figure 2 shows the results of FISPIN calculations for the total decay heat following a 235U single fission between 1 and 106 seconds. The FISPIN results using JEF-1, JEF-2.2, JEFF-3.1 and JEFF-3.1.1 are shown together with the results from Tobias’ evaluation of available experimental data. It should be noted that in the 235U figures the effect of the 137I independent yield and its daughter products are insignificant in the time range of 105 seconds (~1 day) and thus the JEFF-3.1 and JEFF-3.1.1 fission

1. Although results are only given for calculations made with the FISPIN code, similar results have been reported within the JEFF project using other codes and it is not expected that significant differences would exist between code systems following the conclusions reported in Duchemin, B., and C. Nordborg (1989), “Decay Heat Calculation – An International Nuclear Code Comparison”, NEACRP-319"L"/NEANDC-275"U", OECD Nuclear Energy Agency, Paris, which states that, “The overall results of the calculation of decay heat and contributing fission products are in very good agreement for the [different] codes.”

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26 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

yields give the same calculated results. Similar results were generated for 239Pu and are shown in Figure 3. The decay heat calculations and experimental data show reasonable agreement. To highlight differences, the ratios of the FISPIN results to the experimental data are shown in the lower parts of each figure where the experimentally derived uncertainties (one standard deviation) are shown as wide dotted grey lines about unity.

Figures 4-5 and 6-7 repeat similar calculations, but for the beta and gamma-ray heating components respectively. These results show that JEFF-3.1.1 gives better results compared to JEFF-3.1. The results are especially improved with this latest version for 235U gamma-ray heating, as was expected with the inclusion of the TAGS data. Similarly, the 239Pu gamma-ray heating is slightly improved. This is due to the different fission products produced in the different fissioning systems.

These results show the expected improvement in the prediction of the decay heat using the JEFF-3.1.1 decay data library.

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LIBRARY TESTING AND VALIDATION

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Table 4.1: Average delayed neutron yields following a single fission calculated using JEFF-3.1 and JEFF-3.1.1

Nuclide Energy Calculated JEFF-3.1

neutron per 100 fissions

Calculated JEFF-3.1.1

neutron per 100 fissions

Measured neutrons per 100 fissions with uncertainty

and reference code*

JEFF-3.1 and JEFF-3.1.1 ratio C/E

232Th Fast 5.38 ± 0.06 5.38 ± 0.06 5.47 ± 0.12 T 0.97 232Th 14 MeV 3.05 ± 0.03 3.05 ± 0.03 2.85 ± 0.13 V 1.06 233U Thermal 0.72 ± 0.01 0.72 ± 0.01 0.664 ± 0.018 T 1.08 233U Fast 1.04 ± 0.02 1.04 ± 0.02 0.729 ± 0.019 T 1.43 233U 14 MeV 0.55 ± 0.01 0.55 ± 0.01 0.422 ± 0.025 V 1.33 234U Fast 1.34 ± 0.03 1.34 ± 0.03 1.06 ± 0.12 T 1.26 235U Thermal 1.47 ± 0.02 1.47 ± 0.02 1.654 ± 0.042 T 0.88 235U Fast 1.69 ± 0.03 1.69 ± 0.03 1.714 ± 0.022 T 0.99 235U 14 MeV 0.93 ± 0.02 0.93 ± 0.02 0.927 ± 0.029 V 1.00 236U Fast 2.38 ± 0.04 2.38 ± 0.04 2.31 ± 0.26 T 1.03 238U Fast 4.03 ± 0.05 4.03 ± 0.05 4.51 ± 0.061 T 0.88 238U 14 MeV 2.36 ± 0.03 2.36 ± 0.03 2.73 ± 0.08 V 0.86

237Np Thermal 1.12 ± 0.03 1.12 ± 0.03 1.07 ± 0.10 W 1.05 237Np Fast 1.16 ± 0.03 1.16 ± 0.03 1.22 ± 0.03 B 0.96 238Np Thermal 1.41 ± 0.03 1.41 ± 0.03 238Np Fast 1.63 ± 0.03 1.63 ± 0.03 238Pu Thermal 0.31 ± 0.01 0.31 ± 0.01 0.456 ± 0.051 T 0.70 238Pu Fast 0.48 ± 0.01 0.48 ± 0.01 0.456 ± 0.051 T 1.05 239Pu Thermal 0.60 ± 0.02 0.60 ± 0.02 0.624 ± 0.024 T 0.96 239Pu Fast 0.67 ± 0.02 0.67 ± 0.02 0.664 ± 0.013 T 1.01 240Pu Fast 0.91 ± 0.02 0.91 ± 0.02 0.96 ± 0.11 T 0.96 241Pu Thermal 1.23 ± 0.03 1.23 ± 0.03 1.56 ± 0.16 T 0.78 241Pu Fast 1.29 ± 0.03 1.29 ± 0.03 1.63 ± 0.16 T 0.79 242Pu Fast 1.68 ± 0.03 1.68 ± 0.03 2.28 ± 0.25 T 0.73 241Am Thermal 0.37 ± 0.01 0.37 ± 0.01 0.44 ± 0.05 W 0.86 241Am Fast 0.41 ± 0.01 0.41 ± 0.01 0.394 ± 0.024 B 1.04

242mAm Thermal 0.58 ± 0.02 0.58 ± 0.02 0.69 ± 0.05 W 0.84 242mAm Fast 0.56 ± 0.02 0.56 ± 0.02 243Am Thermal 0.84 ± 0.02 0.84 ± 0.02 243Am Fast 0.81 ± 0.02 0.81 ± 0.02 242Cm Spont 0.12 ± 0.01 0.12 ± 0.01 243Cm Thermal 0.22 ± 0.01 0.22 ± 0.01 243Cm Fast 0.21 ± 0.01 0.21 ± 0.01 244Cm Spont 0.31 ± 0.01 0.31 ± 0.01 244Cm Thermal 0.32 ± 0.01 0.32 ± 0.01 244Cm Fast 0.33 ± 0.01 0.33 ± 0.01 245Cm Thermal 0.52 ± 0.01 0.52 ± 0.01 0.59 ± 0.04 W 0.88 245Cm Fast 0.46 ± 0.01 0.46 ± 0.01 252Cf Spont 0.58 ± 0.01 0.58 ± 0.01 0.86 ± 0.1 M 0.67

* The reference codes signify: B – Benedetti (1982), M – Manero (1972), T – Tuttle (1975), W – Waldo (1981), V –Tuttle (1979).

Page 28: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Tabl

e 4.

2: A

vera

ge d

elay

ed e

nerg

y em

issi

on fo

llow

ing

a si

ngle

fiss

ion

calc

ulat

ed u

sing

JEF

F-3.

1 an

d JE

FF-3

.1.1

Nuc

lide

Neu

tron

en

ergy

JEFF

3.1

calc

ulat

ion

JEFF

3.1.

1 ca

lcul

atio

n C

ompa

rison

with

exp

erim

enta

l dat

a (J

ames

, 196

9, 1

971)

Le

pton

Ph

oton

B

aryo

nN

eutr

ino

Lept

onPh

oton

Bar

yon

Neu

trin

oB

eta

JEFF

-3.1

C

/E

JEFF

-3.1

.1

C/E

G

amm

aJE

FF-3

.1

C/E

JE

FF-3

.1.1

C/E

M

eV/fi

ssio

n 23

2 Th

Fast

9.

569

7.79

7 0.

259

17.6

26

9.36

9 8.

022

0.25

9 17

.651

8.

3 ±

0.6

1.15

1.

13

8.6

± 2.

00.

91

0.93

23

2 Th

14 M

eV

8.22

6 6.

708

0.14

4 15

.078

8.

093

6.86

3 0.

144

15.0

99

233 U

Th

erm

al

6.13

6 4.

989

0.14

7 11

.272

6.

014

5.13

6 0.

147

11.2

97

5.7

± 0.

41.

08

1.06

5.

9 ±

1.3

0.85

0.

87

233 U

Fa

st

6.20

4 5.

106

0.14

2 11

.452

6.

090

5.25

1 0.

142

11.4

83

233 U

14

MeV

5.

160

4.24

8 0.

092

9.50

0 5.

100

4.31

7 0.

092

9.50

9

23

4 U

Fast

6.

852

5.47

8 0.

149

12.4

79

6.72

2 5.

633

0.14

9 12

.503

6.

2 ±

0.5

1.11

1.

08

6.4

± 1.

30.

86

0.88

23

5 U

Ther

mal

7.

749

6.01

5 0.

180

13.9

44

7.59

0 6.

193

0.18

0 13

.963

7.

0 ±

0.3

1.11

1.

08

7.2

± 1.

10.

84

0.86

23

5 U

Fast

7.

835

6.05

5 0.

171

14.0

61

7.68

3 6.

230

0.17

1 14

.084

23

5 U

14 M

eV

6.49

9 5.

052

0.11

1 11

.663

6.

401

5.15

3 0.

111

11.6

65

236 U

Fa

st

8.51

3 6.

464

0.17

3 15

.150

8.

355

6.63

8 0.

173

15.1

66

7.5

± 0.

51.

14

1.11

7.

7 ±

1.7

0.84

0.

86

238 U

Fa

st

10.1

27

7.52

2 0.

199

17.8

48

9.97

2 7.

684

0.19

9 17

.856

8.

9 ±

0.6

1.14

1.

12

8.4

± 1.

60.

90

0.91

23

8 U

14 M

eV

8.65

4 6.

580

0.15

0 15

.385

8.

532

6.69

7 0.

150

15.3

80

237 N

p Th

erm

al

7.28

3 5.

449

0.16

6 12

.899

7.

150

5.60

1 0.

166

12.9

18

6.4

± 0.

51.

14

1.12

6.

6 ±

1.4

0.83

0.

85

237 N

p Fa

st

7.17

3 5.

452

0.15

7 12

.782

7.

049

5.59

1 0.

157

12.7

97

238 N

p Th

erm

al

7.80

7 5.

896

0.16

0 13

.863

7.

671

6.04

0 0.

160

13.8

71

238 N

p Fa

st

7.97

3 5.

897

0.16

5 14

.035

7.

835

6.04

7 0.

165

14.0

47

238 Pu

Th

erm

al

5.68

5 4.

433

0.10

1 10

.219

5.

610

4.51

7 0.

101

10.2

28

5.5

± 0.

41.

03

1.02

5.

7 ±

1.2

0.78

0.

79

238 Pu

Fa

st

5.88

0 4.

461

0.15

1 10

.492

5.

789

4.56

6 0.

151

10.5

07

239 Pu

Th

erm

al

6.55

1 4.

883

0.14

4 11

.578

6.

448

4.99

2 0.

144

11.5

84

6.1

± 0.

61.

07

1.06

6.

1 ±

1.3

0.80

0.

82

239 Pu

Fa

st

6.56

0 4.

921

0.13

7 11

.618

6.

462

5.02

6 0.

137

11.6

26

240 Pu

Fa

st

7.08

9 5.

280

0.15

3 12

.522

6.

978

5.39

0 0.

153

12.5

22

6.5

± 0.

51.

09

1.07

6.

8 ±

1.4

0.78

0.

79

241 Pu

Th

erm

al

7.93

7 5.

911

0.16

2 14

.010

7.

816

6.02

5 0.

162

14.0

04

7.4

± 0.

61.

07

1.06

7.

8 ±

1.6

0.76

0.

77

241 Pu

Fa

st

7.96

3 5.

899

0.16

3 14

.024

7.

844

6.01

3 0.

163

14.0

20

242 Pu

Fa

st

8.59

3 6.

357

0.17

3 15

.122

8.

466

6.47

4 0.

172

15.1

13

8.0

± 0.

61.

07

1.06

8.

2 ±

1.6

0.78

0.

79

241 Am

Th

erm

al

5.96

3 4.

372

0.13

6 10

.471

5.

879

4.45

6 0.

136

10.4

72

241 Am

Fa

st

5.85

3 4.

338

0.14

6 10

.337

5.

767

4.42

9 0.

146

10.3

42

242m

Am

Ther

mal

6.

586

4.89

1 0.

179

11.6

56

6.47

1 5.

007

0.17

9 11

.657

24

2mAm

Fa

st

6.48

0 4.

826

0.16

5 11

.471

6.

380

4.92

9 0.

165

11.4

74

243 Am

Th

erm

al

7.23

5 5.

366

0.16

8 12

.769

7.

119

5.46

8 0.

168

12.7

55

243 Am

Fa

st

7.16

4 5.

314

0.16

9 12

.647

7.

053

5.41

6 0.

169

12.6

38

242 C

m

Spon

t 4.

783

3.48

9 0.

105

8.37

8 4.

742

3.53

0 0.

105

8.37

7

24

3 Cm

Th

erm

al

5.39

5 3.

946

0.13

2 9.

473

5.32

8 4.

012

0.13

2 9.

472

243 C

m

Fast

5.

267

3.86

6 0.

158

9.29

1 5.

202

3.93

0 0.

158

9.29

1

24

4 Cm

Sp

ont

5.85

1 4.

295

0.14

5 10

.291

5.

781

4.36

3 0.

145

10.2

89

244 C

m

Ther

mal

5.

823

4.30

5 0.

169

10.2

97

5.73

2 4.

392

0.16

9 10

.294

24

4 Cm

Fa

st

5.90

3 4.

280

0.17

6 10

.360

5.

815

4.36

9 0.

176

10.3

61

245 C

m

Ther

mal

6.

350

4.71

2 0.

183

11.2

44

6.24

8 4.

804

0.18

3 11

.234

24

5 Cm

Fa

st

6.38

9 4.

691

0.17

5 11

.255

6.

293

4.77

4 0.

175

11.2

41

252 C

f Sp

ont

7.33

8 5.

082

0.26

4 12

.684

7.

179

5.20

1 0.

264

12.6

43

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Figure 2: The calculated total decay heat (β + γ) from fission products following a 235U fission pulse compared to the Tobias Standard (1989) (top) and as a ratio (bottom)

0.2

0.4

0.6

0.8

1.0

1.2

1.4

1.6

1E+0 1E+1 1E+2 1E+3 1E+4 1E+5Cooling time (s)

Heat

rate

per

fiss

ion

x tim

e (M

eV/s

/ fis

sion

. s)

Tobias (1989)JEFF311JEF-2.2JEF1JEFF31

0.80

0.85

0.90

0.95

1.00

1.05

1.10

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1E+0 1E+1 1E+2 1E+3 1E+4 1E+5Cooling time (s)

Cal

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ted

/ Sta

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d

JEF1JEF22JEFF31JEFF311

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LIBRARY TESTING AND VALIDATION

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Figure 3: The calculated total decay heat (β + γ) from fission products following a 239Pu fission pulse compared to the Tobias Standard (1989) (top) and as a ratio (bottom)

0.2

0.4

0.6

0.8

1.0

1.2

1E+0 1E+1 1E+2 1E+3 1E+4 1E+5Cooling time (s)

Hea

t rat

e pe

r fis

sion

x ti

me

(MeV

/s /

fissi

on .

s)

Tobias (1989)JEFF31JEF-2.2JEF1JEFF311

0.85

0.90

0.95

1.00

1.05

1.10

1.15

1.20

1E+0 1E+1 1E+2 1E+3 1E+4 1E+5Cooling time (s)

Cal

cula

ted

/ Sta

ndar

d

JEF1JEF22JEFF31JEFF311

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Figure 4: The calculated beta decay heat from fission products following a 235U fission pulse compared to the Tobias Standard (1989) (top) and as a ratio (bottom)

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1E+0 1E+1 1E+2 1E+3 1E+4 1E+5Cooling time (s)

Heat

rat

e pe

r fis

sion

x ti

me

(MeV

/s /

fissi

on .

s)

Tobias (1989)JEFF311JEF-2.2JEF1JEFF31

0.80

0.85

0.90

0.95

1.00

1.05

1.10

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1E+0 1E+1 1E+2 1E+3 1E+4 1E+5Cooling time (s)

Cal

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ted

/ Sta

ndar

d

JEF1JEF22JEFF31JEFF311

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LIBRARY TESTING AND VALIDATION

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Figure 5: The calculated beta decay heat from fission products following a 239Pu fission pulse compared to the Tobias Standard (1989) (top) and (bottom) as a ratio

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

1E+0 1E+1 1E+2 1E+3 1E+4 1E+5Cooling time (s)

Heat

rate

per

fiss

ion

x tim

e (M

eV/s

/ fis

sion

. s)

Tobias (1989)JEFF311JEF-2.2JEF1JEFF31

0.80

0.85

0.90

0.95

1.00

1.05

1.10

1.15

1.20

1E+0 1E+1 1E+2 1E+3 1E+4 1E+5Cooling time (s)

Cal

cula

ted

/ Sta

ndar

d

JEF1

JEF22

JEFF31

JEFF311

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LIBRARY TESTING AND VALIDATION

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Figure 6: The calculated gamma-ray decay heat from fission products following a 235U fission pulse compared to the Tobias Standard (1989) (top) and as a ratio (bottom)

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1E+0 1E+1 1E+2 1E+3 1E+4 1E+5Cooling time (s)

Heat

rat

e pe

r fis

sion

x ti

me

(MeV

/s /

fissi

on .

s)

Tobias (1989)JEFF311JEFF31JEF1JEF-2.2

0.700.750.800.850.900.951.001.051.101.151.20

1E+0 1E+1 1E+2 1E+3 1E+4 1E+5Cooling time (s)

Calc

ulat

ed /

Stan

dard

JEF1JEF22JEFF31JEFF311

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Figure 7: The calculated gamma-ray decay heat from fission products following a 239Pu fission pulse compared to the Tobias Standard (1989) (top) and as a ratio (bottom)

0.1

0.2

0.3

0.4

0.5

0.6

1E+0 1E+1 1E+2 1E+3 1E+4 1E+5Cooling time (s)

Hea

t rat

e pe

r fis

sion

x ti

me

(MeV

/s /

fissi

on .

s)

Tobias (1989)JEFF311JEF-2.2JEF1JEFF31

0.80

0.85

0.90

0.95

1.00

1.05

1.10

1.15

1.20

1.25

1E+0 1E+1 1E+2 1E+3 1E+4 1E+5Cooling time (s)

Calc

ulat

ed /

Stan

dard

JEF1JEF22JEFF31JEFF311

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CONCLUSIONS

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 35

Chapter 5: Conclusions

The JEFF-3.1 Radioactive Decay Data and Fissions Yields Sub-libraries were constructed and tested within the JEFF Project during the approximate period 2000-2005, and were released in May 2005, in conjunction with the other JEFF-3.1 sub-libraries. Following initial testing within the JEFF Project, including decay heat validation calculations, an update was made to the decay data and fission yield data that was released as JEFF-3.1.1 in 2007.

The JEFF Project therefore recommends the JEFF-3.1.1 Fission Yields Sub-library and the JEFF-3.1.1 Radioactive Decay Data Sub-library for general use.1

1. The JEFF-3.1 Radioactive Decay Data Sub-library of May 2005 is no longer being distributed and should be updated with the JEFF-3.1.1 November 2007 release.

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REFERENCES

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 37

References

Audi, G., O. Bersillon, J. Blachot and A.H. Wapstra (2003), “The NUBASE Evaluation of Nuclear and Decay Properties”, Nuclear Physics A, 729, pp. 3-128.

Banai, J. and M.F. James (1987), unpublished.

Bé, M.M., E. Browne, V. Chechev, V. Chisté, R. Dersch, C. Dulieu, R.G. Helmer, N. Kuzmenco, A.L. Nichols and E. Schönfeld (2004), Nucléide, Table des Radionucléides sur CD-Rom, Version 2-2004, and the following site last accessed 20 March 2009, www.nucleide.org/NucData.htm.

Benedetti, G. (1982), et al., Nucl. Sci. Eng., 80, 379-387.

Bersillon, O. and J. Blachot (2009), SDf2NDF Code for Converting ENSDF to ENDF, forthcoming.

Brosa, U., S. Grossmann and A. Muller (1990), Physics Reports, 197, No. 4.

Burstall, R.F. (1979), “FISPIN – A Computer Code for Nuclide Inventory Calculations”, UKAEA Report ND-R-328(R).

Crouch, E.A.C. (1977), Atomic Data and Nuclear Data Tables 19, 417 and earlier references therein.

Crouch, E.A.C., M.F. James, P.S. Whitworth and C. Dunn (1985), unpublished.

Dickens, J.K. (1987), Nucl. Sci. Eng., 96, 8.

Dunford, C.L. (n.d.), ENDF Utility Checking Codes, 7.01, Brookhaven National Laboratory, Upton NY, USA.

Greenwood, R.C., R.G. Helmer, M.H. Putnam and K.D. Watts (1997), “Measurement of β–-decay Intensity Distributions of Several Fission-product Isotopes Using a Total Absorption γ-ray Spectrometer”, Nuclear Instruments and Methods in Physics Research A 390, pp. 95-154.

Herman, M. (Ed.) (2005), ENDF-102: ENDF-6 Formats Manual, Data Formats and Procedures for the Evaluated Nuclear Data File, ENDF/B-VI and ENDF/B-VII, Report BNL-NCS-44945-05-Rev., June.

James, M.F. (1969), Journal of Nuclear Energy, Vol. 23, pp. 517-536.

James, M.F. (1971), Journal of Nuclear Energy, Vol. 25, pp. 513-523.

James, M.F. (1987), “A Review of Libraries of Fission Product Yields”, Proc. of a Specialists Mtg. on Data for Decay Heat Predictions, Studsvik, Sweden, NEACRP-302'L'/NEANDC-245'U', OECD, Paris, p. 69.

James, M.F., R.W. Mills and D.R. Weaver (1991), “A New Evaluation of Fission Product Yields and the Production of a New Library (UKFY2) of Independent and Cumulative Yields. Part I. Methods and Outline of the Evaluation”, AEA-TRS-1015.

James, M.F., R.W. Mills and D.R. Weaver (1991a), “A New Evaluation of Fission Product Yields and the Production of a New Library (UKFY2) of Independent and Cumulative Yields. Part II. Tables of Measured and Recommended Fission Yields”, AEA-TRS-1018.

James, M.F., R.W. Mills and D.R. Weaver (1991b), “A New Evaluation of Fission Product Yields and the Production of a New Library (UKFY2) of Independent and Cumulative Yields. Part III. Tables of fission Yields with Discrepant or Sparse Data”, AEA-TRS-1019.

James, M.F., R.W. Mills and D.R. Weaver (1991c), The Use of the Normalised Residual in Using Experimental Data and in Treating Outliers, UKAEA report AEA-RS-1082 and later published in Nucl. Inst. and Meths., A313, 277 (1992).

Kellett, M.A. (2007), et al., Assessment of Fission Product Decay Data for Decay Heat Calculations, report by the Working Party on International Evaluation Co-operation of the NEA Nuclear Science Committee, Vol. 25, NEA/WPEC-25, OECD Nuclear Energy Agency, Paris, ISBN 978-92-64-99034-0.

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REFERENCES

38 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

Kinsey, R. and B.A. Magurno (Eds.) (1983), Data Formats and Procedures for the Evaluated Nuclear Data File, ENDF/B-V, BNL-NCS-50496/ENDF-102.

Klapdor, H.V. (1989), private communication.

Lemmel, H.D. (1996), Short Guide to EXFOR, Report IAEA-NDS-1, Rev.7.

Lund, E., G. Rudstam, K. Aleklett, B. Ekstrom, B. Fogelberg and L. Jacobsson (1986), “A Status Report on Delayed Neutron Branching Ratios of Fission Products”, Proc. of the Specialists Meeting on Delayed Neutron Properties, D.R. Weaver (Ed.), p. 59, University of Birmingham, UK.

Madland, D.G. and T.R. England (1976), Nucl. Sci. Eng., 64, 859.

Madland, D.G. and L. Stewart (1977), LA-6783.

Manero, F. and V.A. Konshin (1972), in Atomic Energy Review, 10, p. 637, IAEA, Vienna, Austria.

Mills, R.W., M.F. James and D.R. Weaver (1989), “The Production of a New Evaluation of Fission Product Yields”, Proc. of the Conf. on 50 Years with Nuclear Fission, Gaithersburg, Vol. I, p. 471.

Mills, R.W. (1995), “Fission Product Yield Evaluation”, Thesis, The University of Birmingham, UK.

Mills, R.W. (2006), Technical Note on a Study of Indirect Tritium Production Using FISPIN and JEFF-3.1, JEFDOC-1152. Also referenced as NDA00712.5/06/10/02 and UKNSF(2006)P208.

Musgrove, A.R., J.L. Cook and G.D. Trimble (1973), “Prediction of Unmeasured Fission Yields”, Proc. Panel Fission Product Nuclear Data, Bologna, Italy, IAEA-169 2, 163.

Nichols, A.L. and R.J. Perry (2005), Assessment and Evaluation of Decay Data for EAF – 2004/05, UKNSF(2005)P188 (JEF/DOC-1072) relates to UKPADD-6.4 and both libraries are available from the OECD/NEA Databank upon request.

Nichols, A.L. and R.J. Perry (2007), Activation Product Decay Data: UKPADD-6.7, UKNSF(2007)P212 (JEF/DOC-1165), and A.L. Nichols and R.J. Perry, Heavy Element and Actinide Decay Data: UKHEDD-2.5, UKNSF(2007)P213 (JEF/DOC-1166).

Ouasti, R. (1988), “Étude de l’émission des particules légères chargées alphas et tritons dans la fission de uranium 235, uranium 238 et plutonium 239 induites par des neutrons rapides”, Thesis, The University of Bordeaux, CENBG 8801.

Perry, R.J., M.J. Grimstone and C.J. Dean (2003), Specification and Maintenance Document for Decay Data Checking in FIZCON, UKNSF(2003)P160 (JEFDOC-959) and references therein.

Rider, B.F. (1981), NEDO-12154-3(C) and references therein.

Rider, B.F. and T.R. England (1987), “Evaluation of Fission Product Yields for the USA National Nuclear Data Files”, Proc. of a Specialists Mtg. on Data for Decay Heat Predictions, Studsvik, Sweden, NEACRP-302'L'/NEANDC-245'U', OECD, Paris, p. 21.

Rudstam, G. (1992), Proceedings of a Specialists Mtg. on Fission Product Nuclear Data, NEA/NSC/DOC(92)9, Tokai, Japan, 25-27 May 1992, p. 27.

Serot, O., C. Wagemans and Jan Heyse (2004), “New Results on Helium and Tritium Gas Production from Ternary Fission”, International Conference on Nuclear Data for Science and Technology, Santa Fe, USA.

Tobias, A. (1980), “Decay Heat”, Progress in Nuclear Energy, Vol. 5, No. 1, pp. 1-193.

Tobias, A. (1989), Derivation of Decay Heat Benchmarks for 235U and 239Pu by a Least Squares Fit to Measured Data, CEGB report RD/B/6210/R89.

Tuli, J.K. (1987), The Evaluated Nuclear Structure Data file (ENSDF), Report BNL-NCS-51655 Rev. 87, April.

Tuttle, R.J. (1975), Nucl. Sci. Eng., 56, 37.

Tuttle, R.J. (1979), in Proc. Consultants’ Meeting on Delayed Neutron Properties, Vienna, Austria, 26-30 March.

Vidal, Jean-Marc, private communication, CEA Cadarache (2007).

Wahl, A.C. (1985), Phys. Rev., C 32, 184.

Wahl, A.C. (1988), Atomic Data and Nuclear Data Tables 39, 1.

Waldo, R.W. (1981), et al., Phys. Rev., C. 23, 1113.

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MAIN DATA TABLES

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 39

Main data tables

Table A: Atomic weights and natural abundances included in JEFF-3.1.1

Mat no. Element Atomic weight

Natural abundance (%)

1 0-nn- 1 1.000000 See footnote * 2 1-H - 1 0.999167 99.9885 70 † 3 1-H - 2 1.996800 0.0115 70 9 2-He- 3 2.990120 0.000137 3 10 2-He- 4 3.968220 99.999863 3 19 3-Li- 6 5.963450 7.59 4 20 3-Li- 7 6.955730 92.41 4 30 4-Be- 9 8.934760 100.00 42 5-B - 10 9.926920 19.9 7 43 5-B - 11 10.914700 80.1 7 56 6-C - 12 11.896900 98.93 8 57 6-C - 13 12.891600 1.07 8 71 7-N - 14 13.882800 99.632 7 72 7-N - 15 14.871300 0.368 7 87 8-O - 16 15.857500 99.757 16 88 8-O - 17 16.853100 0.038 1 89 8-O - 18 17.844500 0.205 14

105 9-F - 19 18.835200 100.00 122 10-Ne- 20 19.820700 90.48 3 123 10-Ne- 21 20.813500 0.27 1 124 10-Ne- 22 21.802500 9.25 3 142 11-Na- 23 22.792300 100.00 162 12-Mg- 24 23.779000 78.99 4 163 12-Mg- 25 24.771200 10.00 1 164 12-Mg- 26 25.759400 11.01 3 187 13-Al- 27 26.749800 100.00 209 14-Si- 28 27.736600 92.2297 7 210 14-Si- 29 28.727600 4.6832 5 211 14-Si- 30 29.716300 3.0872 5 233 15-P - 31 30.707700 100.00 255 16-S - 32 31.697400 94.93 31 256 16-S - 33 32.688200 0.76 2 257 16-S - 34 33.676100 4.29 28 259 16-S - 36 35.658100 0.02 1 281 17-Cl- 35 34.668500 75.78 4 283 17-Cl- 37 36.648300 24.22 4 305 18-Ar- 36 35.658600 0.3365 30 307 18-Ar- 38 37.636600 0.0632 5

* All atomic weights are given relative to the neutron mass of 1.0086649157 (6) unified atomic mass units (u). † The uncertainty is given following the value, i.e. 99.9885 70 is 99.9885 ± 70.

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MAIN DATA TABLES

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Table A: Atomic weights and natural abundances included in JEFF-3.1.1 (cont.)

Mat no. Element Atomic weight

Natural abundance (%)

309 18-Ar- 40 39.619100 99.6003 30 331 19-K - 39 38.629000 93.2581 44 332 19-K - 40 39.620700 0.0117 1 333 19-K - 41 40.609900 6.7302 44 354 20-Ca- 40 39.619300 96.941 156 356 20-Ca- 42 41.598200 0.647 23 357 20-Ca- 43 42.589700 0.135 10 358 20-Ca- 44 43.577900 2.086 110 360 20-Ca- 46 45.558900 0.004 3 362 20-Ca- 48 47.540600 0.187 21 383 21-Sc- 45 44.569700 100.00 410 22-Ti- 46 45.557900 8.25 3 411 22-Ti- 47 46.548400 7.44 2 412 22-Ti- 48 47.536100 73.72 3 413 22-Ti- 49 48.527400 5.41 2 414 22-Ti- 50 49.515700 5.18 2 440 23-V - 50 49.518100 0.250 4 441 23-V - 51 50.506300 99.750 4 465 24-Cr- 50 49.517000 4.345 13 467 24-Cr- 52 51.494300 83.789 18 468 24-Cr- 53 52.485900 9.501 17 469 24-Cr- 54 53.475500 2.365 7 497 25-Mn- 55 54.466100 100.00 526 26-Fe- 54 53.476200 5.845 35 528 26-Fe- 56 55.454400 91.754 36 529 26-Fe- 57 56.446300 2.119 10 530 26-Fe- 58 57.435600 0.282 4 561 27-Co- 59 58.426900 100.00 592 28-Ni- 58 57.437700 68.0769 89 594 28-Ni- 60 59.416000 26.2231 77 595 28-Ni- 61 60.407600 1.1399 6 596 28-Ni- 62 61.396400 3.6345 17 598 28-Ni- 64 63.378800 0.9256 9 625 29-Cu- 63 62.389000 69.17 3 627 29-Cu- 65 64.370000 30.83 3 660 30-Zn- 64 63.380000 48.63 60 662 30-Zn- 66 65.359700 27.90 27 663 30-Zn- 67 66.352200 4.10 13 664 30-Zn- 68 67.341300 18.75 51 667 30-Zn- 70 69.324600 0.62 3 698 31-Ga- 69 68.333500 60.108 9 700 31-Ga- 71 70.315400 39.892 9 730 32-Ge- 70 69.323600 20.84 87 733 32-Ge- 72 71.304200 27.54 34 734 32-Ge- 73 72.297000 7.73 5 736 32-Ge- 74 73.286200 36.28 73 739 32-Ge- 76 75.269200 7.61 38 772 33-As- 75 74.278000 100.00 803 34-Se- 74 73.287400 0.89 4 805 34-Se- 76 75.267000 9.37 29 806 34-Se- 77 76.259100 7.63 16

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MAIN DATA TABLES

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Table A: Atomic weights and natural abundances included in JEFF-3.1.1 (cont.)

Mat no. Element Atomic weight

Natural abundance (%)

808 34-Se- 78 77.248000 23.77 28 811 34-Se- 80 79.230000 49.61 41 814 34-Se- 82 81.213000 8.73 22 845 35-Br- 79 78.240400 50.69 7 849 35-Br- 81 80.221200 49.31 7 877 36-Kr- 78 77.251000 0.35 1 880 36-Kr- 80 79.229900 2.28 6 883 36-Kr- 82 81.209800 11.58 14 884 36-Kr- 83 82.201900 11.49 6 886 36-Kr- 84 83.190700 57.00 4 889 36-Kr- 86 85.172600 17.30 22 923 37-Rb- 85 84.182400 72.17 2 926 37-Rb- 87 86.162600 27.83 2 957 38-Sr- 84 83.192600 0.56 1 960 38-Sr- 86 85.171300 9.86 1 961 38-Sr- 87 86.162300 7.00 1 963 38-Sr- 88 87.150500 82.58 1 1002 39-Y - 89 88.142100 100.00 1047 40-Zr- 90 89.132400 51.45 40 1049 40-Zr- 91 90.124700 11.22 5 1050 40-Zr- 92 91.115500 17.15 8 1052 40-Zr- 94 93.099600 17.38 28 1054 40-Zr- 96 95.084400 2.80 9 1090 41-Nb- 93 92.108300 100.00 1131 42-Mo- 92 91.117300 14.84 35 1134 42-Mo- 94 93.098400 9.25 12 1135 42-Mo- 95 94.090600 15.92 13 1136 42-Mo- 96 95.080800 16.68 2 1137 42-Mo- 97 96.073600 9.55 8 1138 42-Mo- 98 97.064300 24.13 31 1140 42-Mo-100 99.049200 9.63 23 1213 44-Ru- 96 95.083700 5.54 14 1215 44-Ru- 98 97.064200 1.87 3 1216 44-Ru- 99 98.056300 12.76 14 1217 44-Ru-100 99.046000 12.60 7 1218 44-Ru-101 100.039000 17.06 2 1219 44-Ru-102 101.029000 31.55 14 1222 44-Ru-104 103.013000 18.62 27 1264 45-Rh-103 102.021000 100.00 1305 46-Pd-102 101.030000 1.02 1 1307 46-Pd-104 103.011000 11.14 8 1308 46-Pd-105 104.004000 22.33 8 1309 46-Pd-106 104.994000 27.33 3 1312 46-Pd-108 106.977000 26.46 9 1315 46-Pd-110 108.961000 11.72 9 1362 47-Ag-107 105.987000 51.839 8 1366 47-Ag-109 107.969000 48.161 8 1412 48-Cd-106 104.997000 1.25 6 1414 48-Cd-108 106.977000 0.89 3 1416 48-Cd-110 108.959000 12.49 18 1417 48-Cd-111 109.951000 12.80 12

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MAIN DATA TABLES

42 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

Table A: Atomic weights and natural abundances included in JEFF-3.1.1 (cont.)

Mat no. Element Atomic weight

Natural abundance (%)

1419 48-Cd-112 110.941000 24.13 21 1420 48-Cd-113 111.934000 12.22 12 1422 48-Cd-114 112.925000 28.73 42 1425 48-Cd-116 114.909000 7.49 18 1478 49-In-113 111.934000 4.29 5 1483 49-In-115 113.917000 95.71 5 1542 50-Sn-112 110.944000 0.97 1 1545 50-Sn-114 112.924000 0.66 1 1546 50-Sn-115 113.916000 0.34 1 1547 50-Sn-116 114.906000 14.54 9 1548 50-Sn-117 115.899000 7.68 7 1550 50-Sn-118 116.889000 24.22 9 1551 50-Sn-119 117.882000 8.59 4 1553 50-Sn-120 118.872000 32.58 9 1556 50-Sn-122 120.856000 4.63 3 1559 50-Sn-124 122.841000 5.79 5 1601 51-Sb-121 119.865000 57.21 5 1604 51-Sb-123 121.848000 42.79 5 1648 52-Te-120 118.874000 0.09 1 1651 52-Te-122 120.856000 2.55 12 1652 52-Te-123 121.848000 0.89 3 1654 52-Te-124 122.838000 4.74 14 1655 52-Te-125 123.831000 7.07 15 1657 52-Te-126 124.822000 18.84 25 1660 52-Te-128 126.806000 31.74 8 1663 52-Te-130 128.790000 34.08 62 1700 53-I -127 125.814000 100.00 1737 54-Xe-124 122.841000 0.09 1 1740 54-Xe-126 124.823000 0.09 1 1743 54-Xe-128 126.805000 1.92 3 1744 54-Xe-129 127.797000 26.44 24 1746 54-Xe-130 128.788000 4.08 2 1747 54-Xe-131 129.781000 21.18 3 1749 54-Xe-132 130.771000 26.89 6 1753 54-Xe-134 132.755000 10.44 10 1757 54-Xe-136 134.740000 8.87 16 1802 55-Cs-133 131.764000 100.00 1844 56-Ba-130 128.790000 0.106 1 1848 56-Ba-132 130.772000 0.101 1 1851 56-Ba-134 132.754000 2.417 18 1852 56-Ba-135 133.747000 6.592 12 1854 56-Ba-136 134.737000 7.854 24 1856 56-Ba-137 135.730000 11.232 24 1858 56-Ba-138 136.721000 71.698 42 1904 57-La-138 136.722000 0.090 1 1905 57-La-139 137.713000 99.910 1 1945 58-Ce-136 134.740000 0.185 2 1948 58-Ce-138 136.721000 0.251 2 1952 58-Ce-140 138.704000 88.450 51 1954 58-Ce-142 140.690000 11.114 51 1997 59-Pr-141 139.697000 100.00

Page 43: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

MAIN DATA TABLES

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 43

Table A: Atomic weights and natural abundances included in JEFF-3.1.1 (cont.)

Mat no. Element Atomic weight

Natural abundance (%)

2042 60-Nd-142 140.689000 27.2 5 2043 60-Nd-143 141.682000 12.2 2 2044 60-Nd-144 142.674000 23.8 3 2045 60-Nd-145 143.668000 8.3 1 2046 60-Nd-146 144.660000 17.2 3 2048 60-Nd-148 146.646000 5.7 1 2050 60-Nd-150 148.633000 5.6 2 2135 62-Sm-144 142.676000 3.07 7 2138 62-Sm-147 145.653000 14.99 18 2139 62-Sm-148 146.644000 11.24 10 2140 62-Sm-149 147.638000 13.82 7 2141 62-Sm-150 148.629000 7.38 1 2143 62-Sm-152 150.615000 26.75 16 2146 62-Sm-154 152.600000 22.75 29 2184 63-Eu-151 149.623000 47.81 3 2188 63-Eu-153 151.608000 52.19 3 2226 64-Gd-152 150.615000 0.20 1 2228 64-Gd-154 152.599000 2.18 3 2229 64-Gd-155 153.592000 14.80 12 2231 64-Gd-156 154.583000 20.47 9 2232 64-Gd-157 155.576000 15.65 2 2233 64-Gd-158 156.567000 24.84 7 2235 64-Gd-160 158.553000 21.86 19 2286 65-Tb-159 157.560000 100.00 2322 66-Dy-156 154.585000 0.06 1 2325 66-Dy-158 156.568000 0.10 1 2327 66-Dy-160 158.551000 2.34 8 2328 66-Dy-161 159.544000 18.91 24 2329 66-Dy-162 160.536000 25.51 26 2330 66-Dy-163 161.529000 24.90 16 2331 66-Dy-164 162.521000 28.18 37 2387 67-Ho-165 163.513000 100.00 2424 68-Er-162 160.538000 0.14 1 2426 68-Er-164 162.521000 1.61 3 2428 68-Er-166 164.505000 33.61 35 2429 68-Er-167 165.498000 22.93 17 2431 68-Er-168 166.490000 26.78 26 2433 68-Er-170 168.476000 14.93 27 2478 69-Tm-169 167.483000 100.00 2510 70-Yb-168 166.491000 0.13 1 2513 70-Yb-170 168.475000 3.04 15 2514 70-Yb-171 169.468000 14.28 57 2516 70-Yb-172 170.459000 21.83 67 2517 70-Yb-173 171.453000 16.13 27 2518 70-Yb-174 172.445000 31.83 92 2521 70-Yb-176 174.431000 12.76 41 2574 71-Lu-175 173.438000 97.41 2 2575 71-Lu-176 174.431000 2.59 2 2614 72-Hf-174 172.446000 0.16 1 2616 72-Hf-176 174.430000 5.26 7 2617 72-Hf-177 175.423000 18.60 9

Page 44: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

MAIN DATA TABLES

44 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

Table A: Atomic weights and natural abundances included in JEFF-3.1.1 (cont.)

Mat no. Element Atomic weight

Natural abundance (%)

2620 72-Hf-178 176.415000 27.28 7 2623 72-Hf-179 177.409000 13.62 2 2626 72-Hf-180 178.401000 35.08 16 2677 73-Ta-180M 178.402000 0.012 2 2678 73-Ta-181 179.394000 99.988 2 2714 74-W -180 178.401000 0.12 1 2717 74-W -182 180.385000 26.50 16 2718 74-W -183 181.379000 14.31 4 2720 74-W -184 182.371000 30.64 2 2723 74-W -186 184.357000 28.43 19 2769 75-Re-185 183.364000 37.40 2 2772 75-Re-187 185.350000 62.60 2 2806 76-Os-184 182.372000 0.02 1 2808 76-Os-186 184.356000 1.59 3 2809 76-Os-187 185.350000 1.96 2 2810 76-Os-188 186.341000 13.24 8 2811 76-Os-189 187.335000 16.15 5 2813 76-Os-190 188.327000 26.26 2 2817 76-Os-192 190.312000 40.78 19 2867 77-Ir-191 189.320000 37.3 2 2873 77-Ir-193 191.305000 62.7 2 2913 78-Pt-190 188.328000 0.014 1 2915 78-Pt-192 190.312000 0.782 7 2918 78-Pt-194 192.296000 32.967 99 2919 78-Pt-195 193.290000 33.832 10 2921 78-Pt-196 194.282000 25.242 41 2924 78-Pt-198 196.267000 7.163 55 2978 79-Au-197 195.275000 100.00 3022 80-Hg-196 194.282000 0.15 1 3025 80-Hg-198 196.266000 9.97 20 3026 80-Hg-199 197.259000 16.87 22 3028 80-Hg-200 198.251000 23.10 19 3029 80-Hg-201 199.244000 13.18 9 3030 80-Hg-202 200.236000 29.86 26 3032 80-Hg-204 202.221000 6.87 15 3092 81-Tl-203 201.229000 29.524 14 3094 81-Tl-205 203.214000 70.476 14 3143 82-Pb-204 202.221000 1.4 1 3147 82-Pb-206 204.205000 24.1 1 3148 82-Pb-207 205.198000 22.1 1 3150 82-Pb-208 206.190000 52.4 1 3208 83-Bi-209 207.185000 100.00 3486 90-Th-232 230.045000 100.00 3541 92-U -234 232.030000 0.0055 2 3542 92-U -235 233.025000 0.7200 51 3546 92-U -238 236.006000 99.2745 106

Page 45: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

MAIN DATA TABLES

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 45

Table B: Updated average energy values from TAGS measurements in JEFF-3.1.1

Matn Nuclide Original From TAGS JEFF-3.1

source <β> (eV) <γ> (eV) <β> (eV) <γ> (eV) 0929 37-Rb- 90 2.049E+06 1.982E+06 1.916E+06 2.271E+06 ENSDF 0930 37-Rb- 90M 1.403E+06 3.241E+06 1.118E+06 3.869E+06 ENSDF 0931 37-Rb- 91 1.612E+06 2.269E+06 1.368E+06 2.706E+06 ENSDF 0970 38-Sr- 95 2.208E+06 1.118E+06 1.901E+06 1.790E+06 ENSDF 1812 55-Cs-139 1.640E+06 3.446E+05 1.671E+06 3.050E+05 ENSDF 1814 55-Cs-141 1.935E+06 7.696E+05 1.506E+06 1.701E+06 ENSDF 1863 56-Ba-143 1.417E+06 1.417E+06 1.195E+06 1.341E+06 NUBASE 1864 56-Ba-144 1.040E+06 1.040E+06 9.298E+05 7.847E+05 NUBASE 1865 56-Ba-145 1.860E+06 1.860E+06 1.285E+06 1.833E+06 NUBASE 1908 57-La-142 8.682E+05 2.325E+06 9.619E+05 2.121E+06 ENSDF 1909 57-La-143 1.237E+06 2.523E+05 1.235E+06 4.394E+05 ENSDF 1910 57-La-144 1.382E+06 2.330E+06 9.862E+05 3.085E+06 ENSDF 1911 57-La-145 1.499E+06 6.239E+05 7.618E+05 2.144E+06 ENSDF 1960 58-Ce-148 7.133E+05 7.133E+05 5.857E+05 4.858E+05 NUBASE 2005 59-Pr-147 8.990E+05 8.990E+05 6.685E+05 9.285E+05 NUBASE 2006 59-Pr-148 1.679E+06 9.377E+05 1.348E+06 1.776E+06 ENSDF 2007 59-Pr-148M 1.701E+06 9.368E+05 1.239E+06 2.050E+06 ENSDF 2008 59-Pr-149 1.286E+06 3.049E+05 8.107E+05 1.332E+06 ENSDF 2010 59-Pr-151 1.394E+06 1.394E+06 1.114E+06 1.362E+06 NUBASE 2053 60-Nd-153 1.112E+06 1.112E+06 1.153E+06 5.086E+05 NUBASE 2054 60-Nd-154 9.367E+05 9.367E+05 8.562E+05 5.506E+05 NUBASE 2055 60-Nd-155 1.500E+06 1.500E+06 1.085E+06 1.543E+06 NUBASE 2098 61-Pm-152 1.326E+06 2.852E+05 1.304E+06 3.454E+05 ENSDF 2101 61-Pm-153 6.858E+05 7.339E+04 6.626E+05 1.225E+05 ENSDF 2102 61-Pm-154 1.321E+06 1.321E+06 8.491E+05 1.876E+06 NUBASE 2105 61-Pm-156 1.717E+06 1.717E+06 1.206E+06 2.206E+06 NUBASE 2106 61-Pm-157 1.453E+06 1.453E+06 1.540E+06 8.490E+05 NUBASE 2149 62-Sm-157 9.123E+05 9.123E+05 8.389E+05 5.850E+05 NUBASE 2150 62-Sm-158 6.667E+05 6.667E+05 5.121E+05 5.903E+05 NUBASE

Page 46: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

MAIN DATA TABLES

46 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

Table C: Total number of neutrons per fission ( totalυ )

Matn. Nuclide totalυ

3484 90-Th-230M 1.3900 3486 90-Th-232M 1.5000 3513 91-Pa-231M 1.7100 3539 92-U -232M 1.7100 3541 92-U -234M 1.8000 3542 92-U -235M 1.8700 3544 92-U -236M 1.9000 3546 92-U -238M 2.0000 3582 94-Pu-236M 2.1200 3585 94-Pu-238M 2.2100 3586 94-Pu-239M 2.3200 3587 94-Pu-240M 2.1510 3589 94-Pu-242M 2.1410 3591 94-Pu-244M 2.2900 3605 95-Am-241M 2.5000 3607 95-Am-242M 2.5600 3609 95-Am-243M 2.6100 3627 96-Cm-242M 2.5280 3629 96-Cm-244M 2.6875 3632 96-Cm-246M 2.9480 3634 96-Cm-248M 3.1610 3636 96-Cm-250M 3.3000 3654 97-Bk-249M 3.4000 3672 98-Cf-249M 3.4000 3673 98-Cf-250M 3.5200 3675 98-Cf-252M 3.7560 3694 99-Es-253M 4.7000

Page 47: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Tabl

e D

: Orig

inal

JEF

F-3.

1 da

ta, u

pdat

ed in

JEF

F-3.

1.1

a) T

he fo

llow

ing

nucl

ei h

ad u

nkno

wn

spin

s/pa

ritie

s in

JEF

F-3.

1, w

hich

wer

e up

date

d in

JEF

F-3.

1.1

Matn

Nuclide

Source

Matn

Nuclide

Source

0092

8-O - 21

ENSDF

3434

89-Ac-211

ENSDF

0159

12-Mg- 21

NUBASE

3436

89-Ac-213

ENSDF

0216

14-Si- 35

ENSDF

3444

89-Ac-220

ENSDF

0472

24-Cr- 57

ENSDF

3445

89-Ac-221

ENSDF

0603

28-Ni- 69

ENSDF

3466

90-Th-213

ENSDF

0870

36-Kr- 71

ENSDF

3470

90-Th-217

ENSDF

0936

37-Rb- 96

ENSDF

3472

90-Th-219

ENSDF

0986

39-Y - 80

ENSDF

3498

91-Pa-217

ENSDF

1190

43-Tc-107

ENSDF

3499

91-Pa-217M

ENSDF

1194

43-Tc-111

ENSDF

3505

91-Pa-223

ENSDF

1231

44-Ru-113

ENSDF

3507

91-Pa-225

ENSDF

1586

51-Sb-110

ENSDF

3526

92-U -219

ENSDF

1819

55-Cs-145

ENSDF

3530

92-U -223

ENSDF

2733

75-Re-161

ENSDF

3625

96-Cm-240

ENSDF

2832

77-Ir-169

ENSDF

3745

102-No-251

ENSDF

2936

79-Au-173

ENSDF

3752

102-No-256

ENSDF

2994

80-Hg-175

ENSDF

3766

103-Lr-257

ENSDF

b) O

rigin

al d

ata

from

JE

FF-3

.1 fo

r tho

se n

ucle

i upd

ated

in J

EFF

-3.1

.1 (n

ew e

valu

atio

ns o

r bet

ter t

reat

men

t of o

rigin

al s

ourc

e da

ta)

Matn

Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0078 7-N - 21 0.5- 0.087 s 6.90

β-:20.00; β-,n:80.00 0

3.822E+06

3.822E+06

2.676E+06

NUBASE

0107 9-F - 21 2.5+ 4.158 s 0.48

β-:100.00

2

2.354E+06

5.373E+05

1.492E+03

ENSDF

0286 17-Cl- 39 1.5+ 55.6 m 0.36

β-:100.00

2

8.230E+05

1.451E+06

ENSDF

0384 21-Sc- 45M 1.5+ 1.240E+04 0.318 s 2.20

IT:100.00

0

1.240E+04

NUBASE

0532 26-Fe- 60 0.0+ 1.5E+06 y 20

β-m:100.00

1

8.767E+04

UKPADD64

0575 27-Co- 70 ? 0.125 s 5.60

β-:100.00

0

4.503E+06

4.503E+06

NUBASE

0633 29-Cu- 70 1.0+ 4.5 s 22.22

β-:100.00

2

2.782E+06

4.778E+05

ENSDF

0634 29-Cu- 70M 3.0- 1.010E+05 33 s 6.06

β-:50.00; IT:50.00

0

1.115E+06

1.165E+06

NUBASE

0635 29-Cu- 70N 1.0+ 2.420E+05 6.6 s 3.03

β-:95.00; ITm:5.00

0

2.163E+06

2.170E+06

NUBASE

0665 30-Zn- 69 0.5- 56.4 m 1.60

β-:100.00

2

3.216E+05

6.000E+00

ENSDF

0666 30-Zn- 69M 4.5+ 4.387E+05 13.76 h 0.15

IT:99.97; β-:0.03

4

2.204E+04

4.161E+05

ENSDF

0735 32-Ge- 73M 0.5- 6.673E+04 0.499 s 2.20

IT:100.00

0

6.673E+04

NUBASE

0770 33-As- 73 1.5- 80.3 d 0.07

β+m:100.00

0

1.369E+04

2.738E+04

NUBASE

0774 33-As- 76 2.0- 1.093 d 0.34

β-:100.00

2

1.065E+06

4.163E+05

ENSDF

0780 33-As- 82 1.0+ 19.1 s 2.62

β-:100.00

2

3.297E+06

3.273E+05

ENSDF

0807 34-Se- 77M 3.5+ 1.619E+05 17.36 s 0.29

IT:100.00

0

1.619E+05

NUBASE

0809 34-Se- 79 3.5+ 1.1E+06 y 18.18

β-:100.00

1

5.580E+04

ENSDF

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 47

MAIN DATA TABLES

Page 48: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

b) O

rigin

al d

ata

from

JE

FF-3

.1 fo

r tho

se n

ucle

i upd

ated

in J

EFF

-3.1

.1 (n

ew e

valu

atio

ns o

r bet

ter t

reat

men

t of o

rigin

al s

ourc

e da

ta) (

cont

.)

Matn

Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0812 34-Se- 81 0.5- 18.45 m 0.65

β-:100.00

4

6.107E+05

7.991E+03

ENSDF

0813 34-Se- 81M 3.5+ 1.030E+05 57.28 m 0.03

β-:0.05; IT:99.95

4

8.445E+04

1.825E+04

ENSDF

0820 34-Se- 87 2.5+ 5.29 s 2.08

β-:100.00

2

2.833E+06

1.067E+06

ENSDF

0856 35-Br- 86 2.0- 55 s 1.45

β-:100.00

2

1.968E+06

3.232E+06

ENSDF

0869 36-Kr- 70 0.0+ 0.057 s 36.84

β+m:100.00

0

2.486E+06

2.486E+06

NUBASE

0926 37-Rb- 87 1.5- 4.75E+10 y 0.84

β-:100.00

1

8.170E+04

ENSDF

0962 38-Sr- 87M 0.5- 3.885E+05 2.803 h 0.11

β+:0.30; IT:99.70

4

6.654E+04

3.195E+05

ENSDF

0998 39-Y - 87 0.5- 3.325 d 0.38

β+m:100.00

0

4.911E+05

4.911E+05

NUBASE

0999 39-Y - 87M 4.5+ 3.808E+05 13.37 h 0.22

IT:98.43; β+:1.57

0

1.174E+04

3.866E+05

NUBASE

1005 39-Y - 90M 7.0+ 6.820E+05 3.19 h 0.31

IT:100.00;

β-:~;

β-m:~

4

4.528E+04

6.353E+05

ENSDF

1015 39-Y - 97 0.5- 3.75 s 0.80

β-:100.00

4

2.148E+06

1.818E+06

ENSDF

1016 39-Y - 97M 4.5+ 6.675E+05 1.17 s 2.56

β-:99.22;

IT:0.70;

β-,n:0.08

0

2.433E+06

2.438E+06

3.562E+02

NUBASE

1017 39-Y - 97N 13.5- 3.523E+06 0.142 s 5.63

ITm:80.00; β-:20.00

0

6.808E+05

2.965E+06

NUBASE

1048 40-Zr- 90M 5.0- 2.319E+06 0.809 s 0.25

IT:100.00

3

1.554E+04

2.303E+06

ENSDF

1096 41-Nb- 96 6.0+ 23.35 h 0.21

β-:100.00

4

2.497E+05

2.460E+06

ENSDF

1107 41-Nb-102M ? 4.3 s 9.30

β-:100.00

2

2.276E+06

2.094E+06

ENSDF

1185 43-Tc-102M ? 4.35 m 1.61

β-:100.00

2

7.798E+05

2.511E+06

ENSDF

1260 45-Rh-101 0.5- 3.3 y 9.09

β+:100.00

4

2.554E+04

2.878E+05

ENSDF

1261 45-Rh-101M 4.5+ 1.573E+05 4.34 d 0.23

β+:93.60; IT:6.40

0

3.271E+04

7.550E+04

NUBASE

1278 45-Rh-111 3.5+ 11 s 9.09

β-:99.60; β-

m:0.40

0

1.215E+06

1.215E+06

NUBASE

1319 46-Pd-113 2.5+ 1.55 m 5.38

β-:4.24; β-

m:95.76

4

1.365E+06

1.209E+05

ENSDF

1320 46-Pd-113M 4.5- 8.130E+04 0.3 s 33.33

IT:100.00

3

5.842E+04

2.136E+04

ENSDF

1367 47-Ag-109M 3.5+ 8.803E+04 39.6 s 0.51

IT:100.00

3

7.575E+04

1.124E+04

ENSDF

1389 47-Ag-121 3.5+ 0.78 s 1.28

β-:89.55; β-

m:10.45

4

2.301E+06

1.167E+06

ENSDF

1429 48-Cd-119 1.5+ 2.69 m 0.74

β-:9.72; β-

m:90.28

4

8.107E+05

1.485E+06

ENSDF

1430 48-Cd-119M 5.5- 1.465E+05 2.2 m 0.91

β-:99.78; β-

m:0.22

4

7.000E+05

2.162E+06

ENSDF

1431 48-Cd-120 0.0+ 50.8 s 0.41

β-:100.00

1

7.080E+05

ENSDF

1432 48-Cd-121 1.5+ 13.5 s 2.22

β-:33.68; β-

m:66.32

4

1.240E+06

1.725E+06

ENSDF

1495 49-In-120 1.0+ 3.08 s 2.60

β-:100.00

2

2.210E+06

2.566E+05

ENSDF

1496 49-In-120M ? 46.2 s 1.73

β-:100.00

2

1.310E+06

2.838E+06

ENSDF

1498 49-In-121 4.5+ 23.1 s 2.60

β-:88.67; β-

m:11.33

4

9.847E+05

9.229E+05

ENSDF

1499 49-In-121M 0.5- 3.136E+05 3.88 m 100

IT:1.20; β-:98.80

4

1.516E+06

6.402E+04

ENSDF

1509 49-In-126 3.0+ 1.6 s 6.25

β-:100.00

2

2.399E+06

2.764E+06

ENSDF

1554 50-Sn-121 1.5+ 1.127 d 0.15

β-:100.00

1

1.152E+05

ENSDF

1565 50-Sn-128 0.0+ 59.1 m 0.85

β-:100.00; β-

m:~

4

2.503E+05

6.034E+05

ENSDF

1567 50-Sn-129 1.5+ 2.23 m 1.79

β-:100.00

0

1.345E+06

1.345E+06

NUBASE

1568 50-Sn-129M 5.5- 3.520E+04 6.9 m 1.45

β-:50.00;

β-m:50.00;

IT:~

0

1.048E+06

1.048E+06

NUBASE

1569 50-Sn-130 0.0+ 3.72 m 1.08

β-:100.00

4

4.667E+05

9.273E+05

ENSDF

1570 50-Sn-130M 7.0- 1.947E+06 1.7 m 5.88

β-:50.00; β-

m:50.00

0

1.366E+06

1.366E+06

NUBASE

48 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 49: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

b) O

rigin

al d

ata

from

JE

FF-3

.1 fo

r tho

se n

ucle

i upd

ated

in J

EFF

-3.1

.1 (n

ew e

valu

atio

ns o

r bet

ter t

reat

men

t of o

rigin

al s

ourc

e da

ta) (

cont

.)

Matn

Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1613 51-Sb-128 8.0- 9.01 h 0.33

β-:100.00

4

4.864E+05

3.048E+06

ENSDF

1754 54-Xe-134M 7.0- 1.966E+06 0.29 s 5.86

IT:100.00

0

1.966E+06

NUBASE

1788 55-Cs-123 0.5+ 5.94 m 0.67

β+:100.00

4

9.986E+05

9.988E+05

ENSDF

1789 55-Cs-123M 5.5- 1.563E+05 1.64 s 7.32

IT:100.00

3

1.119E+05

4.684E+04

ENSDF

1805 55-Cs-135 3.5+ 2.3E+06 y 13.04

β-:100.00

1

8.940E+04

ENSDF

1811 55-Cs-138M 6.0- 7.990E+04 2.91 m 2.75

IT:81.00; β-:19.00

0

3.455E+05

4.102E+05

NUBASE

1815 55-Cs-142 0.0- 1.7 s 1.18

β-:100.00

4

2.899E+06

6.753E+05

ENSDF

1859 56-Ba-139 3.5- 1.384 h 0.34

β-:100.00

4

8.977E+05

4.562E+04

ENSDF

1915 57-La-148 2.0- 1.428 s 0.84

β-:100.00

4

2.145E+06

1.194E+06

ENSDF

1955 58-Ce-143 1.5- 1.379 d 0.15

β-:100.00

4

4.289E+05

2.790E+05

ENSDF

1958 58-Ce-146 0.0+ 13.52 m 0.96

β-:100.00

0

3.433E+05

3.433E+05

NUBASE

1961 58-Ce-149 1.5- 5.3 s 3.77

β-:100.00

0

1.453E+06

1.453E+06

NUBASE

2003 59-Pr-145 3.5+ 5.984 h 0.17

β-:100.00

0

6.017E+05

6.017E+05

NUBASE

2104 61-Pm-155 2.5- 41.5 s 0.48

β-:100.00

4

1.265E+06

1.233E+05

ENSDF

2139 62-Sm-148 0.0+ 8E+15 y 25

α:100.00

1

1.986E+06

ENSDF

2148 62-Sm-156 0.0+ 9.4 h 2.13

β-:100.00

4

2.185E+05

1.149E+05

ENSDF

2192 63-Eu-156 0.0+ 15.19 d 0.53

β-:100.00

4

4.541E+05

1.230E+06

ENSDF

2238 64-Gd-163 3.5+ 1.133 m 4.41

β-:100.00

0

1.037E+06

1.037E+06

NUBASE

2260 65-Tb-146 1.0+ 8 s 50

β+:100.00

0

2.774E+06

2.774E+06

NUBASE

2261 65-Tb-146M 5.0- 1.500E+05 24.1 s 2.07

β+:100.00

0

2.824E+06

2.824E+06

NUBASE

2284 65-Tb-158 3.0- 180.004 y 6.11

β+:83.40; β-:16.60

0

3.908E+05

3.908E+05

NUBASE

2285 65-Tb-158M 0.0- 1.103E+05 10.7 s 1.59

IT:99.39; β-:0.60;

β+:0.01

0

2.135E+03

1.118E+05

NUBASE

2287 65-Tb-160 3.0- 72.3 d 0.28

β-:100.00

4

2.572E+05

1.126E+06

ENSDF

2334 66-Dy-166 0.0+ 3.4 d 0.12

β-:100.00

0

1.623E+05

1.623E+05

NUBASE

2430 68-Er-167M 0.5- 2.078E+05 2.269 s 0.26

IT:100.00

0

2.078E+05

NUBASE

2458 69-Tm-155 5.5- 21.6 s 0.93

β+:98.10; α:1.90

0

1.825E+06

1.825E+06

8.687E+04

NUBASE

2459 69-Tm-155M 0.5+ 4.100E+04 45 s 6.67

β+:92.00; α m:8.00

0

1.724E+06

1.724E+06

3.658E+05

NUBASE

2476 69-Tm-167 0.5+ 9.25 d 0.22

β+:1.70; β+

m:98.30

0

2.721E+04

5.441E+04

NUBASE

2477 69-Tm-168 3.0+ 93.1 d 0.21

β+:99.99; β-:0.01

0

5.596E+05

5.596E+05

NUBASE

2480 69-Tm-171 0.5+ 1.92 y 0.52

β-:100.00

4

2.541E+04

6.220E+02

ENSDF

2481 69-Tm-172 2.0- 2.65 d 0.47

β-:100.00

4

5.279E+05

4.743E+05

ENSDF

2536 71-Lu-155 5.5- 0.069 s 2.33

α:88.00; β+:12.00

0

3.180E+05

3.180E+05

5.107E+06

NUBASE

2624 72-Hf-179M 0.5- 3.750E+05 18.67 s 0.21

IT:100.00

0

3.750E+05

NUBASE

2625 72-Hf-179N 12.5- 1.106E+06 25.05 d 1

IT:100.00

0

1.106E+06

NUBASE

2726 74-W -188 0.0+ 69.78 d 0.07

β-:100.00

4

9.961E+04

1.890E+03

ENSDF

2765 75-Re-183 2.5+ 70 d 2

β+:50.00; β+

m:50.00

0

2.006E+04

4.013E+04

NUBASE

2766 75-Re-183M 12.5+ 1.908E+06 1.04E-03 s 4.81

IT:100.00

0

1.908E+06

NUBASE

2767 75-Re-184 3.0- 38 d 1.32

β+:100.00

0

4.934E+05

4.934E+05

NUBASE

2768 75-Re-184M 8.0+ 1.880E+05 169 d 4.73

IT:75.40; β+:24.60

0

2.052E+04

1.828E+05

NUBASE

2770 75-Re-186 1.0- 3.775 d 0.19

β+:6.90; β-:93.10

5

3.373E+05

2.030E+04

LNHB

2771 75-Re-186M 8.0+ 1.490E+05 2E+05 y 25

IT:90.00; β-:10.00

0

4.061E+04

1.747E+05

NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 49

MAIN DATA TABLES

Page 50: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

b) O

rigin

al d

ata

from

JE

FF-3

.1 fo

r tho

se n

ucle

i upd

ated

in J

EFF

-3.1

.1 (n

ew e

valu

atio

ns o

r bet

ter t

reat

men

t of o

rigin

al s

ourc

e da

ta) (

cont

.)

Matn

Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2815 76-Os-191 4.5- 15.4 d 0.65

β-:52.80; β-

m:47.20

0

7.729E+04

7.729E+04

NUBASE

2816 76-Os-191M 1.5- 7.438E+04 13.1 h 0.76

IT:100.00

3

6.649E+04

7.855E+03

UKPADD64

2820 76-Os-194 0.0+ 6 y 3.33

β-:100.00

0

3.220E+04

3.220E+04

NUBASE

2868 77-Ir-191M 5.5- 1.712E+05 4.9 s 0.41

IT:100.00

3

9.709E+04

7.547E+04

UKPADD64

2874 77-Ir-193M 5.5- 8.024E+04 10.53 d 0.38

IT:100.00

0

8.024E+04

NUBASE

2876 77-Ir-194M 4.0+ 1.471E+05 0.032 s 0.75

IT:100.00

0

1.471E+05

NUBASE

2920 78-Pt-195M 6.5+ 2.593E+05 4.02 d 0.25

IT:100.00

0

2.593E+05

NUBASE

2940 79-Au-175 0.5+ 70 d 2.86

α:100.00

1

6.562E+06

ENSDF

2973 79-Au-195 1.5+ 186.1 d 0.03

β+:100.00

0

1.134E+04

2.268E+04

NUBASE

2974 79-Au-195M 5.5- 3.186E+05 30.5 s 0.66

IT:100.00

0

3.186E+05

NUBASE

3019 80-Hg-194 0.0+ 440.008 y 18.18

β+:100.00

0

3.450E+03

6.900E+03

NUBASE

3168 83-Bi-189M 0.5+ 1.850E+05 6.6E-03 s 9.09

α:50.00; β+:50.00

0

1.334E+06

1.334E+06

3.730E+06

NUBASE

3546 92-U -238 0.0+ 4.468E+09 y 0.07

α:99.99; SF:0.01

6

1.021E+04

1.492E+03

4.268E+06

UKHEDD24

3663 98-Cf-240 0.0+ 1.06 m 14.15

α:98.00; SF:2.00

0

7.561E+06

NUBASE

50 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 51: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Tabl

e E:

Mai

n pa

ram

eter

s of

the

JEFF

-3.1

.1 R

adio

activ

e D

ecay

Dat

a Su

b-lib

rary

Mat

n:

Mat

eria

l nu

mbe

r –

allo

cate

d b

y in

crem

enti

ng

from

1 f

or

each

nu

clid

e to

385

2.

Nu

clid

e:

Co

nsi

sts

of

the

nu

clid

e id

enti

fier

in

th

e fo

llo

win

g fo

rmat

; Z

ZZ

-Sy-

AA

AX

, w

her

e Z

ZZ

is

the

atom

ic n

um

ber,

Sy

is t

he

chem

ical

sy

mbo

l (l

ow

erca

se s

eco

nd

let

ter)

, A

AA

is

the

mas

s n

um

ber

and

X d

eno

tes

if g

rou

nd

(bl

ank)

, fi

rst

met

asta

ble

(M),

sec

on

d

met

asta

ble

(N) o

r th

ird

met

asta

ble

(O).

SpPa

: D

eno

tes

the

spin

an

d p

arit

y. A

“?”

sh

ow

s th

is is

un

know

n, d

eno

ted

as

-77.

777

in t

he

actu

al E

ND

F fo

rmat

.

Exc

ener

: G

ives

th

e ex

cita

tion

en

ergy

(in

eV

) for

a m

etas

tabl

e st

ate

(lef

t bl

ank

for

grou

nd

sta

tes)

.

Hal

f-li

fe:

Th

e h

alf-

life

of

the

iso

top

e is

pre

sen

ted

in

eit

her

sec

ond

s (s

), m

inu

tes

(m),

hou

rs (

h)

or

year

s (y

) al

on

g w

ith

its

per

cen

tage

err

or

(all

hal

f-li

ves

are

sto

red

in

sec

on

ds

in t

he

ori

gin

al l

ibra

ry).

Th

ose

mar

ked

100

% m

ean

s th

at n

o er

ror

was

giv

en i

n t

he

ori

gin

al f

ile,

i.e

. was

giv

en a

s ze

ro, a

nd

th

ose

mar

ked

“~

” m

ean

s th

at t

he

per

cen

tage

err

or

is l

ess

than

0.0

1%. T

he

nu

mbe

r o

f se

con

ds

in a

yea

r is

th

at u

sed

in

NU

BA

SE-2

003,

i.e.

1 y

ear

= 36

5.24

22 d

ays

= 3

1 55

6 92

6 se

con

ds.

A m

axim

um

of

thre

e d

ecim

al p

lace

s ar

e u

sed

(w

ith

tr

aili

ng

zero

es r

emo

ved

).

Dec

ay m

od

es:

Th

e d

ecay

mo

des

are

giv

en f

ollo

wed

by

thei

r br

anch

ing

rati

o (

give

n i

n %

), a

“~”

den

ote

s th

e br

anch

ing

rati

o i

s le

ss t

han

0.0

1%.

Each

in

div

idu

al m

ode

is s

epar

ated

by

a “;

” an

d a

n “

m”

or a

n “

n”

subs

crip

t d

enot

es t

he

dau

ghte

r is

in

its

fir

st o

r se

con

d m

etas

tabl

e st

ate

resp

ecti

vely

. Co

mp

ou

nd

mo

des

are

sep

arat

ed b

y a

com

ma

e.g.

β-,

n in

dic

ates

a β

- d

ecay

fo

llo

wed

by

a n

eutr

on

dec

ay.

Nsp

: Sh

ows

the

nu

mbe

r of

sp

ectr

a gi

ven

in t

he

file

.

<β>

(eV

): Sh

ow

s th

e av

erag

e li

ght

par

ticl

e en

ergy

(in

eV

) re

leas

ed i

n t

he

dec

ay, i

.e. <

β> =

<β-

> +

<β+

> +

<e-

> +

<γ>

(eV

): Sh

ows

the

aver

age

elec

trom

agn

etic

rad

iati

on

en

ergy

(in

eV

) rel

ease

d in

th

e d

ecay

, i.e

. <γ>

= <

γ> +

<X

-ray

s> +

<an

n. r

ad.>

+ …

<α>

(eV

):

Sho

ws

the

aver

age

hea

vy p

arti

cle

ener

gy (i

n e

V)

rele

ased

in

th

e d

ecay

, i.e

. <α>

= <

α> +

<SF

> +

<p

> +

<n

> +

Fo

r th

e th

ree

aver

age

ener

gies

abo

ve, a

val

ue

of z

ero

is r

epla

ced

by

blan

ks f

or b

ette

r re

adab

ilit

y.

Sou

rce:

G

ives

th

e n

ame

of

the

ori

gin

al l

ibra

ry w

her

e th

e d

ata

wer

e ta

ken

fro

m.

Sta

ble

nu

clei

are

in

clu

ded

in

th

e li

brar

y fo

r th

e fi

rst

tim

e an

d a

re i

ncl

ud

ed i

n t

he

tabl

e w

ith

in

form

atio

n g

iven

fo

r th

e m

ater

ial

nu

mbe

r,

nu

clid

e id

enti

fier

, sp

in/p

arit

y an

d s

ou

rce

libr

ary.

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 51

MAIN DATA TABLES

Page 52: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0001 0-nn- 1 0.5+ 10.243 m 0.21

β-:100.00

1

3.014E+05 ENSDF

0002 1-H - 1 0.5+

NUBASE

0003 1-H - 2 1.0+

NUBASE

0004 1-H - 3 0.5+ 12.33 y 0.16

β-:100.00

1

5.707E+03 UKPADD67

0005 1-H - 4 2.0- 1.39E-22 s 7.19

n:100.00

0

2.879E+06 NUBASE

0006 1-H - 5 0.5+ 9.1E-22 s 100

2n:100.00

0

1.798E+06 NUBASE

0007 1-H - 6 2.0- 2.9E-22 s 24.14

n:50.00; 3n:50.00

0

1.798E+06 NUBASE

0008 1-H - 7 0.5+ 2.3E-23 s 2.61

2n:100.00

0

1.074E+05 NUBASE

0009 2-He- 3 0.5+

NUBASE

0010 2-He- 4 0.0+

NUBASE

0011 2-He- 5 1.5- 7E-22 s 4.29

n:100.00

0

8.938E+05 NUBASE

0012 2-He- 6 0.0+ 0.808 s 0.25

β-:100.00

1

1.561E+06 5.644E+03 UKPADD67

0013 2-He- 7 1.5- 2.9E-21 s 17.24

n:100.00

0

4.346E+05 NUBASE

0014 2-He- 8 0.0+ 0.122 s 1.64

β-:88.00; β-,n:12.00

3

4.449E+06 8.850E+05 1.414E+05 UKPADD67

0015 2-He- 9 0.5- 7E-21 s 57.14

n:100.00

0

1.270E+06 NUBASE

0016 2-He- 10 0.0+ 2.7E-21 s 66.67

2n:100.00

0

1.069E+06 NUBASE

0017 3-Li- 4 2.0- 9.1E-23 s 9.89

p:100.00

0

3.100E+06 NUBASE

0018 3-Li- 5 1.5- 3.7E-22 s 8.11

p:100.00

0

1.966E+06 NUBASE

0019 3-Li- 6 1.0+

NUBASE

0020 3-Li- 7 1.5-

NUBASE

0021 3-Li- 8 2.0+ 0.838 s 0.72

β-,α:100.00

2

6.205E+06 3.298E+04 3.125E+06 UKPADD67

0022 3-Li- 9 1.5- 0.178 s 0.22

β-:50.50; β-,n:49.50

1

5.696E+06 2.990E+04 UKPADD67

0023 3-Li- 10 ? 2E-21 s 25

n:100.00

0

2.540E+04 NUBASE

0024 3-Li- 11 1.5- 8.75E-03 s 1.60

β-:9.10; β-,n:84.90;

β-,2n:4.10; β-,3n:1.90

0

5.088E+06 5.088E+06 4.462E+06 NUBASE

0025 3-Li- 12 ? 1E-08 s 100

n:100.00

0

1.232E+06 NUBASE

0026 4-Be- 5 0.5+ 1E-09 s 100

p:100.00

0

5.391E+06 NUBASE

0027 4-Be- 6 0.0+ 5E-21 s 6

2p:100.00

0

1.372E+06 NUBASE

0028 4-Be- 7 1.5- 53.22 d 0.11

β+:100.00

3

2.724E+01 4.986E+04 LNHB

0029 4-Be- 8 0.0+ 7E-17 s 28.57

α:100.00

1

9.190E+04 UKPADD67

0030 4-Be- 9 1.5-

NUBASE

0031 4-Be- 10 0.0+ 1.6E+06 y 12.50

β-:100.00

1

2.522E+05 UKPADD67

0032 4-Be- 11 0.5+ 13.81 s 0.58

β-:97.00; β-,α:3.00

3

4.647E+06 1.419E+06 3.627E+04 UKPADD67

0033 4-Be- 12 0.0+ 0.021 s 0.47

β-:100.00

1

5.615E+06 1.224E+04 ENSDF

0034 4-Be- 13 0.5+ 5E-10 s 20

n:100.00

0

1.017E+05 NUBASE

0035 4-Be- 14 0.0+ 4.35E-03 s 3.91

β-:~; β-,n:98.00;

β-,2n:1.80; β-,3n:0.20

0

3.803E+06 3.803E+06 3.803E+06 NUBASE

0036 4-Be- 15 ? 2E-07 s 100

n:100.00

0

1.779E+06 NUBASE

0037 4-Be- 16 0.0+ 2E-07 s 100

2n:100.00

0

1.587E+06 NUBASE

0038 5-B - 6 2.0- 1E-09 s 100

2p:100.00

0

3.702E+06 NUBASE

0039 5-B - 7 1.5- 3.5E-22 s 14.29

p:100.00

0

2.206E+06 NUBASE

0040 5-B - 8 2.0+ 0.77 s 0.39

β+,n:100.00

0

4.518E+06 4.518E+06 4.518E+06 NUBASE

0041 5-B - 9 1.5- 8E-19 s 37.50

p:100.00

0

1.850E+05 NUBASE

52 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 53: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0042 5-B - 10 3.0+

NUBASE

0043 5-B - 11 1.5-

NUBASE

0044 5-B - 12 1.0+ 0.02 s 0.10

β-:98.42; β-,α:1.58

3

6.308E+06 9.056E+04 6.642E+03 UKPADD67

0045 5-B - 13 1.5- 0.017 s 0.98

β-:99.72; β-,n:0.28

3

6.278E+06 3.135E+05 9.757E+03 UKPADD67

0046 5-B - 14 2.0- 0.013 s 4

β-:100.00

2

7.085E+06 5.936E+06 2.318E+04 ENSDF

0047 5-B - 15 1.5- 9.87E-03 s 0.71

β-:6.00; β-,n:93.60;

β-,2n:0.40

0

4.576E+06 4.576E+06 4.194E+06 NUBASE

0048 5-B - 16 0.0- 1.9E-10 s 100

n:100.00

0

3.670E+04 NUBASE

0049 5-B - 17 1.5- 5.08E-03 s 0.98

β-:22.50; β-,n:63.00;

β-,2n:11.00; β-,3n:3.50 0

5.804E+06 5.804E+06 4.099E+06 NUBASE

0050 5-B - 18 4.0- 2.6E-08 s 100

n:100.00

0

4.787E+05 NUBASE

0051 5-B - 19 1.5- 2.92E-03 s 4.45

β-,n:75.00; β-,2n:25.00 0

6.328E+06 6.328E+06 6.328E+06 NUBASE

0052 6-C - 8 0.0+ 2E-21 s 20

2p:100.00

0

2.141E+06 NUBASE

0053 6-C - 9 1.5- 0.127 s 0.71

β+:60.00; β+,p:23.00;

β+,n:17.00

0

4.887E+06 4.887E+06 1.588E+06 NUBASE

0054 6-C - 10 0.0+ 19.255 s 0.28

β+:100.00

4

8.086E+05 1.744E+06 ENSDF

0055 6-C - 11 1.5- 20.37 m 0.14

β+:100.00

3

3.846E+05 1.019E+06 LNHB

0056 6-C - 12 0.0+

NUBASE

0057 6-C - 13 0.5-

NUBASE

0058 6-C - 14 0.0+ 5699.985 y 0.53

β-:100.00

1

4.948E+04 LNHB

0059 6-C - 15 0.5+ 2.449 s 0.20

β-:100.00

2

2.856E+06 3.622E+06 UKPADD67

0060 6-C - 16 0.0+ 0.747 s 1.07

β-:2.10; β-,n:97.90

0

1.407E+06 1.407E+06 1.351E+06 NUBASE

0061 6-C - 17 1.5+ 0.193 s 2.59

β-:71.60; β-,n:28.40

0

3.660E+06 3.660E+06 5.172E+05 NUBASE

0062 6-C - 18 0.0+ 0.092 s 2.17

β-:68.50; β-,n:31.50

0

3.406E+06 3.406E+06 7.078E+05 NUBASE

0063 6-C - 19 0.5+ 0.046 s 4.98

β-:46.00; β-,n:47.00;

β-,2n:7.00

0

4.006E+06 4.006E+06 1.467E+06 NUBASE

0064 6-C - 20 0.0+ 0.016 s 18.75

β-:28.00; β-,n:72.00

0

3.927E+06 3.927E+06 2.453E+06 NUBASE

0065 6-C - 21 0.5+ 3E-08 s 100

n:100.00

0

3.287E+05 NUBASE

0066 6-C - 22 0.0+ 6.2E-03 s 20.97

β-:1.00; β-,n:99.00

0

5.011E+06 5.011E+06 4.940E+06 NUBASE

0067 7-N - 10 2.0- 2E-22 s 70

p:100.00

0

2.600E+06 NUBASE

0068 7-N - 11 0.5+ 5.9E-22 s 35.59

p:100.00

0

1.312E+06 NUBASE

0069 7-N - 12 1.0+ 0.011 s 0.15

β+:100.00

4

7.729E+06 1.191E+06 2.466E+04 ENSDF

0070 7-N - 13 0.5- 9.967 m 0.04

β+:100.00

3

4.908E+05 1.020E+06 LNHB

0071 7-N - 14 1.0+

NUBASE

0072 7-N - 15 0.5-

NUBASE

0073 7-N - 16 2.0- 7.13 s 0.28

β-:100.00; β-,α:~

3

2.679E+06 4.622E+06 2.970E+01 UKPADD67

0074 7-N - 17 0.5- 4.17 s 0.10

β-:5.00; β-,n:95.00;

β-,α:~

4

1.698E+06 4.451E+04 9.011E+05 UKPADD67

0075 7-N - 18 1.0- 0.622 s 1.45

β-:76.90; β-,n:10.90;

β-,α:12.20

0

3.955E+06 3.955E+06 3.934E+05 NUBASE

0076 7-N - 19 0.5- 0.271 s 2.95

β-:45.40; β-,n:54.60

0

3.066E+06 3.066E+06 1.170E+06 NUBASE

0077 7-N - 20 ? 0.13 s 5.38

β-:43.00; β-,n:57.00

0

4.053E+06 4.053E+06 1.477E+06 NUBASE

0078 7-N - 21 0.5- 0.087 s 6.90

β-:19.00; β-,n:81.00

0

3.798E+06 3.798E+06 2.710E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 53

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Page 54: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0079 7-N - 22 ? 0.014 s 10.07

β-:65.00; β-,n:35.00

0

6.323E+06 6.323E+06 1.392E+06 NUBASE

0080 7-N - 23 0.5- 0.015 s 9.66

β-:20.00; β-,n:80.00

0

5.796E+06 5.796E+06 4.210E+06 NUBASE

0081 7-N - 24 ? 5.2E-08 s 100

n:100.00

0

1.069E+06 NUBASE

0082 7-N - 25 0.5- 2.6E-07 s 100

n:50.00; 2n:50.00

0

1.423E+06 NUBASE

0083 8-O - 12 0.0+ 5.8E-22 s 5.17

2p:60.00; β+:40.00

0

1.961E+06 1.961E+06 1.063E+06 NUBASE

0084 8-O - 13 1.5- 8.58E-03 s 0.58

β+:89.10; β+,p:10.90

0

5.708E+06 5.708E+06 4.312E+05 NUBASE

0085 8-O - 14 0.0+ 1.177 m 0.03

β+:100.00

4

7.762E+05 3.320E+06 ENSDF

0086 8-O - 15 0.5- 2.041 m 0.29

β+:100.00

3

7.357E+05 1.021E+06 LNHB

0087 8-O - 16 0.0+

NUBASE

0088 8-O - 17 2.5+

NUBASE

0089 8-O - 18 0.0+

NUBASE

0090 8-O - 19 2.5+ 26.91 s 0.30

β-:100.00

2

1.710E+06 1.005E+06 UKPADD67

0091 8-O - 20 0.0+ 13.51 s 0.37

β-:100.00

2

1.197E+06 1.057E+06 ENSDF

0092 8-O - 21 2.5+ 3.42 s 2.92

β-:100.00

2

2.447E+06 2.946E+06 2.178E+03 ENSDF

0093 8-O - 22 0.0+ 2.25 s 6.67

β-:78.00; β-,n:22.00

0

1.756E+06 1.756E+06 6.910E+04 NUBASE

0094 8-O - 23 0.5+ 0.09 s 44.44

β-:69.00; β-,n:31.00

0

2.885E+06 2.885E+06 2.903E+05 NUBASE

0095 8-O - 24 0.0+ 0.065 s 7.69

β-:82.00; β-,n:18.00

0

3.491E+06 3.491E+06 3.451E+05 NUBASE

0096 8-O - 25 1.5+ 5E-08 s 100

n:100.00

0

2.987E+05 NUBASE

0097 8-O - 26 0.0+ 4E-08 s 100

2n:70.00; n:30.00

0

4.078E+05 NUBASE

0098 8-O - 27 1.5+ 2.6E-07 s 100

n:50.00; 2n:50.00

0

1.268E+06 NUBASE

0099 8-O - 28 0.0+ 1E-07 s 100

n:50.00; 2n:50.00

0

1.413E+06 NUBASE

0100 9-F - 14 2.0- 1E-09 s 100

p:100.00

0

2.259E+06 NUBASE

0101 9-F - 15 0.5+ 4.1E-22 s 14.63

p:100.00

0

1.484E+06 NUBASE

0102 9-F - 16 0.0- 1.1E-20 s 54.55

p:100.00

0

5.354E+05 NUBASE

0103 9-F - 17 2.5+ 1.075 m 0.25

β+:100.00

3

7.386E+05 1.021E+06 ENSDF

0104 9-F - 18 1.0+ 1.829 h 0.02

β+:100.00

3

2.420E+05 9.899E+05 LNHB

0105 9-F - 19 0.5+

NUBASE

0106 9-F - 20 2.0+ 11.03 s 0.27

β-:100.00

2

2.467E+06 1.645E+06 UKPADD67

0107 9-F - 21 2.5+ 4.158 s 0.48

β-:100.00

4

2.342E+06 5.569E+05 UKPADD67

0108 9-F - 22 ? 4.23 s 0.95

β-:100.00

2

2.326E+06 5.749E+06 2.661E+03 ENSDF

0109 9-F - 23 ? 2.23 s 6.28

β-:86.00; β-,n:14.00

0

2.547E+06 2.547E+06 1.149E+05 NUBASE

0110 9-F - 24 ? 0.4 s 12.50

β-:100.00

2

6.101E+06 1.982E+06 7.684E+03 ENSDF

0111 9-F - 25 2.5+ 0.05 s 12

β-:86.00; β-,n:14.00

0

4.155E+06 4.155E+06 3.203E+05 NUBASE

0112 9-F - 26 1.0+ 0.01 s 13.73

β-:89.00; β-,n:11.00

0

5.631E+06 5.631E+06 3.384E+05 NUBASE

0113 9-F - 27 2.5+ 4.9E-03 s 4.08

β-:23.00; β-,n:77.00

0

4.532E+06 4.532E+06 3.163E+06 NUBASE

0114 9-F - 28 ? 4E-08 s 100

n:100.00

0

2.287E+05 NUBASE

0115 9-F - 29 2.5+ 2.6E-03 s 11.54

β-:40.00; β-,n:60.00

0

6.114E+06 6.114E+06 3.148E+06 NUBASE

0116 9-F - 30 ? 2.6E-07 s 100

n:100.00

0

5.287E+05 NUBASE

0117 9-F - 31 2.5+ 1E-03 s 100

β-:100.00

0

8.483E+06 8.483E+06 NUBASE

0118 10-Ne- 16 0.0+ 9E-21 s 100

2p:100.00

0

1.411E+06 NUBASE

0119 10-Ne- 17 0.5- 0.109 s 0.55

β+:1.30; β+,p:96.00;

β+,n:2.70

0

3.460E+06 3.460E+06 3.397E+06 NUBASE

0120 10-Ne- 18 0.0+ 1.672 s 0.48

β+:100.00

4

1.499E+06 1.105E+06 ENSDF

54 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

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Page 55: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0121 10-Ne- 19 0.5+ 17.22 s 0.12

β+:100.00

3

9.621E+05 1.021E+06 ENSDF

0122 10-Ne- 20 0.0+

NUBASE

0123 10-Ne- 21 1.5+

NUBASE

0124 10-Ne- 22 0.0+

NUBASE

0125 10-Ne- 23 2.5+ 37.2 s 0.54

β-:100.00

2

1.890E+06 1.728E+05 UKPADD67

0126 10-Ne- 24 0.0+ 3.38 m 0.59

β-m:100.00

0

6.648E+05 6.648E+05 NUBASE

0127 10-Ne- 25 1.5+ 0.602 s 1.33

β-:100.00

0

2.417E+06 2.417E+06 NUBASE

0128 10-Ne- 26 0.0+ 0.197 s 0.51

β-:100.00

2

2.179E+03 ENSDF

0129 10-Ne- 27 1.5+ 0.032 s 6.25

β-:98.00; β-,n:2.00

0

4.141E+06 4.141E+06 2.930E+04 NUBASE

0130 10-Ne- 28 0.0+ 0.018 s 12.02

β-:84.00; β-,n:16.00

0

3.772E+06 3.772E+06 3.474E+05 NUBASE

0131 10-Ne- 29 1.5+ 0.016 s 3.21

β-:78.80; β-,n:19.00;

β-,2n:2.20

0

4.606E+06 4.606E+06 5.623E+05 NUBASE

0132 10-Ne- 30 0.0+ 5.8E-03 s 3.45

β-:87.00; β-,n:13.00

0

4.676E+06 4.676E+06 4.018E+05 NUBASE

0133 10-Ne- 31 3.5- 3.4E-03 s 23.53

β-:100.00

0

6.063E+06 6.063E+06 NUBASE

0134 10-Ne- 32 0.0+ 3.5E-03 s 25.71

β-:100.00

0

6.073E+06 6.073E+06 NUBASE

0135 10-Ne- 33 3.5- 2.6E-07 s 100

n:100.00

0

6.487E+05 NUBASE

0136 10-Ne- 34 0.0+ 1E-03 s 100

β-:100.00

0

6.787E+06 6.787E+06 NUBASE

0137 11-Na- 18 1.0- 1.3E-21 s 30.77

p:50.00; β+:50.00

0

3.145E+06 3.145E+06 2.200E+05 NUBASE

0138 11-Na- 19 2.5+ 4E-08 s 100

p:100.00

0

3.208E+05 NUBASE

0139 11-Na- 20 2.0+ 0.448 s 0.51

β+:75.00; β+,n:25.00

0

4.045E+06 4.045E+06 5.725E+05 NUBASE

0140 11-Na- 21 1.5+ 22.49 s 0.18

β+:100.00

4

1.101E+06 1.037E+06 ENSDF

0141 11-Na- 22 3.0+ 2.603 y 0.04

β+:100.00

4

1.942E+05 2.192E+06 LNHB

0142 11-Na- 23 1.5+

NUBASE

0143 11-Na- 24 4.0+ 14.957 h 0.01

β-:100.00

4

5.548E+05 4.121E+06 LNHB

0144 11-Na- 24M 1.0+ 4.723E+05 0.02 s 0.99

IT:99.50; β-:0.50

2

1.384E+04 4.699E+05 LNHB

0145 11-Na- 25 2.5+ 59.6 s 1.17

β-:100.00

2

1.496E+06 4.369E+05 UKPADD67

0146 11-Na- 26 3.0+ 1.08 s 0.93

β-:100.00

2

3.329E+06 2.180E+06 UKPADD67

0147 11-Na- 27 2.5+ 0.301 s 1.99

β-:100.00

2

3.615E+06 1.166E+06 2.802E+03 ENSDF

0148 11-Na- 28 1.0+ 0.03 s 1.31

β-:100.00

2

6.129E+06 1.139E+06 6.881E+03 ENSDF

0149 11-Na- 29 1.5+ 0.045 s 2.67

β-:74.10; β-,n:25.90

0

3.904E+06 3.904E+06 6.224E+05 NUBASE

0150 11-Na- 30 2.0+ 0.048 s 3.51

β-:68.83; β-,n:30.00;

β-,2n:1.17; β-,α:~

0

4.802E+06 4.802E+06 8.393E+05 NUBASE

0151 11-Na- 31 1.5+ 0.017 s 2.35

β-:62.05; β-,n:37.00;

β-,2n:0.90; β-,3n:0.05

0

4.546E+06 4.546E+06 1.264E+06 NUBASE

0152 11-Na- 32 ? 0.013 s 5.43

β-:68.00; β-,n:24.00;

β-,2n:8.00

0

5.626E+06 5.626E+06 1.089E+06 NUBASE

0153 11-Na- 33 1.5+ 8.2E-03 s 2.44

β-:40.00; β-,n:47.00;

β-,2n:13.00

0

5.143E+06 5.143E+06 2.477E+06 NUBASE

0154 11-Na- 34 1.0+ 5.5E-03 s 18.18

β-:35.00; β-,2n:50.00;

β-,n:15.00

0

5.733E+06 5.733E+06 2.939E+06 NUBASE

0155 11-Na- 35 1.5+ 1.5E-03 s 33.33

β-:100.00

0

7.810E+06 7.810E+06 NUBASE

0156 11-Na- 36 ? 2.6E-07 s 100

n:100.00

0

2.987E+05 NUBASE

0157 11-Na- 37 1.5+ 1E-03 s 100

β-:100.00

0

8.677E+06 8.677E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 55

MAIN DATA TABLES

Page 56: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0158 12-Mg- 20 0.0+ 0.09 s 6.67

β+:69.60; β+,p:30.40

0

3.136E+06 3.136E+06 6.482E+05 NUBASE

0159 12-Mg- 21 2.5+ 0.122 s 2.46

β+:66.90; β+,p:32.60;

β+,n:0.50

0

3.798E+06 3.798E+06 8.773E+05 NUBASE

0160 12-Mg- 22 0.0+ 3.857 s 0.23

β+:100.00

4

1.369E+06 1.723E+06 ENSDF

0161 12-Mg- 23 1.5+ 11.317 s 0.10

β+:100.00

4

1.336E+06 1.057E+06 ENSDF

0162 12-Mg- 24 0.0+

NUBASE

0163 12-Mg- 25 2.5+

NUBASE

0164 12-Mg- 26 0.0+

NUBASE

0165 12-Mg- 27 0.5+ 9.458 m 0.13

β-:100.00

2

6.996E+05 8.950E+05 UKPADD67

0166 12-Mg- 28 0.0+ 20.9 h 0.14

β-:100.00

4

1.979E+05 1.380E+06 UKPADD67

0167 12-Mg- 29 1.5+ 1.3 s 9.23

β-:100.00

2

2.634E+06 1.858E+06 1.611E+03 ENSDF

0168 12-Mg- 30 0.0+ 0.335 s 5.07

β-:99.94; β-,n:0.06

0

2.319E+06 2.319E+06 1.849E+02 NUBASE

0169 12-Mg- 31 1.5+ 0.23 s 8.70

β-:93.80; β-,n:6.20

0

3.741E+06 3.741E+06 7.105E+04 NUBASE

0170 12-Mg- 32 0.0+ 0.095 s 16.84

β-:97.60; β-,n:2.40

0

3.323E+06 3.323E+06 3.557E+04 NUBASE

0171 12-Mg- 33 3.5- 0.09 s 1.77

β-:83.00; β-,n:17.00

0

4.049E+06 4.049E+06 3.350E+05 NUBASE

0172 12-Mg- 34 0.0+ 0.02 s 50

β-:100.00

0

3.913E+06 3.913E+06 NUBASE

0173 12-Mg- 35 3.5- 0.07 s 57.14

β-:48.00; β-,n:52.00

0

4.036E+06 4.036E+06 1.431E+06 NUBASE

0174 12-Mg- 36 0.0+ 5E-03 s 100

β-:100.00

0

5.213E+06 5.213E+06 NUBASE

0175 12-Mg- 37 3.5- 0.04 s 100

β-:100.00

0

6.433E+06 6.433E+06 NUBASE

0176 12-Mg- 38 0.0+ 1E-03 s 100

β-:100.00

0

6.317E+06 6.317E+06 NUBASE

0177 12-Mg- 39 3.5- 2.6E-07 s 100

n:100.00

0

4.987E+05 NUBASE

0178 12-Mg- 40 0.0+ 1E-03 s 100

β-:100.00

0

6.980E+06 6.980E+06 NUBASE

0179 13-Al- 21 0.5+ 3.5E-08 s 100

p:100.00

0

1.261E+06 NUBASE

0180 13-Al- 22 3.0+ 0.059 s 5.08

β+:54.79; β+,p:44.00;

β+,2p:0.90; β+,n:0.31

0

4.863E+06 4.863E+06 1.470E+06 NUBASE

0181 13-Al- 23 2.5+ 0.47 s 6.38

β+:92.00; β+,p:8.00

0

3.848E+06 3.848E+06 9.327E+04 NUBASE

0182 13-Al- 24 4.0+ 2.053 s 0.19

β+:100.00

4

2.026E+06 9.499E+06 2.741E+03 ENSDF

0183 13-Al- 24M 1.0+ 4.258E+05 0.131 s 1.90

IT:82.00; β+:17.97;

β+,n:0.03

0

8.572E+05 1.206E+06 3.490E+02 NUBASE

0184 13-Al- 25 2.5+ 7.183 s 0.17

β+:100.00

4

1.454E+06 1.034E+06 ENSDF

0185 13-Al- 26 5.0+ 7.17E+05 y 3.35

β+:100.00

4

3.989E+05 2.675E+06 LNHB

0186 13-Al- 26M 0.0+ 2.284E+05 6.345 s 0.09

β+:100.00

3

1.434E+06 1.026E+06 UKPADD67

0187 13-Al- 27 2.5+

NUBASE

0188 13-Al- 28 3.0+ 2.241 m 0.13

β-:100.00

2

1.238E+06 1.783E+06 UKPADD67

0189 13-Al- 29 2.5+ 6.56 m 0.91

β-:100.00

2

9.728E+05 1.381E+06 UKPADD67

0190 13-Al- 30 3.0+ 3.65 s 1.64

β-:100.00

2

2.290E+06 3.512E+06 UKPADD67

0191 13-Al- 31 ? 0.644 s 3.88

β-:100.00

2

3.381E+06 7.131E+05 2.005E+03 ENSDF

0192 13-Al- 32 1.0+ 0.033 s 12.12

β-:100.00

2

5.894E+06 5.461E+05 5.445E+03 ENSDF

0193 13-Al- 33 2.5+ 0.042 s 0.48

β-:91.50; β-,n:8.50

0

3.808E+06 3.808E+06 1.589E+05 NUBASE

0194 13-Al- 34 4.0- 0.056 s 0.89

β-:87.50; β-,n:12.50

0

5.263E+06 5.263E+06 2.966E+05 NUBASE

0195 13-Al- 35 2.5+ 0.039 s 1.04

β-:59.00; β-,n:41.00

0

4.004E+06 4.004E+06 1.205E+06 NUBASE

0196 13-Al- 36 ? 0.09 s 44.44

β-:70.00; β-,n:30.00

0

5.166E+06 5.166E+06 9.052E+05 NUBASE

0197 13-Al- 37 1.5+ 0.02 s 100

β-:100.00

0

5.510E+06 5.510E+06 NUBASE

56 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 57: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0198 13-Al- 38 ? 0.04 s 100

β-:100.00

0

6.707E+06 6.707E+06 NUBASE

0199 13-Al- 39 1.5+ 0.01 s 100

β-:100.00

0

6.490E+06 6.490E+06 NUBASE

0200 13-Al- 40 ? 0.01 s 100

β-:100.00

0

7.943E+06 7.943E+06 NUBASE

0201 13-Al- 41 1.5+ 2E-03 s 100

β-:100.00

0

7.380E+06 7.380E+06 NUBASE

0202 13-Al- 42 ? 1E-03 s 100

β-:100.00

0

8.417E+06 8.417E+06 NUBASE

0203 14-Si- 22 0.0+ 0.029 s 6.90

β+:68.00; β+,p:32.00

0

4.286E+06 4.286E+06 1.117E+06 NUBASE

0204 14-Si- 23 1.5+ 4.23E-08 s 0.95

β+:8.40; β+,p:88.00;

β+,2p:3.60

0

4.292E+06 4.292E+06 3.816E+06 NUBASE

0205 14-Si- 24 0.0+ 0.14 s 5.71

β+m:62.40; β+,p:37.60

0

3.001E+06 3.001E+06 8.403E+05 NUBASE

0206 14-Si- 25 2.5+ 0.22 s 1.36

β+:63.19; β+,p:36.81

0

3.647E+06 3.647E+06 9.634E+05 NUBASE

0207 14-Si- 26 0.0+ 2.234 s 0.58

β+:0.04; β+

m:99.96

4

1.620E+06 1.255E+06 ENSDF

0208 14-Si- 27 2.5+ 4.16 s 0.48

β+:100.00

0

1.604E+06 1.604E+06 NUBASE

0209 14-Si- 28 0.0+

NUBASE

0210 14-Si- 29 0.5+

NUBASE

0211 14-Si- 30 0.0+

NUBASE

0212 14-Si- 31 1.5+ 2.62 h 0.38

β-:100.00

2

5.937E+05 2.172E+03 UKPADD67

0213 14-Si- 32 0.0+ 132.003 y 9.85

β-:100.00

1

6.468E+04 UKPADD67

0214 14-Si- 33 1.5+ 6.18 s 2.91

β-:100.00

0

1.948E+06 1.948E+06 NUBASE

0215 14-Si- 34 0.0+ 2.77 s 7.22

β-:100.00

0

1.534E+06 1.534E+06 NUBASE

0216 14-Si- 35 3.5- 0.78 s 15.38

β-:100.00

2

2.670E+06 4.472E+06 1.912E+03 ENSDF

0217 14-Si- 36 0.0+ 0.45 s 13.33

β-:100.00

2

3.068E+06 1.671E+06 1.462E+03 ENSDF

0218 14-Si- 37 3.5- 0.09 s 66.67

β-:83.00; β-,n:17.00

0

3.671E+06 3.671E+06 2.380E+05 NUBASE

0219 14-Si- 38 0.0+ 0.09 s 100

β-:100.00

0

3.563E+06 3.563E+06 NUBASE

0220 14-Si- 39 3.5- 0.09 s 100

β-:100.00

0

4.933E+06 4.933E+06 NUBASE

0221 14-Si- 40 0.0+ 0.033 s 3.03

β-:100.00

0

4.527E+06 4.527E+06 NUBASE

0222 14-Si- 41 3.5- 0.03 s 100

β-:100.00

0

6.280E+06 6.280E+06 NUBASE

0223 14-Si- 42 0.0+ 5E-03 s 100

β-:100.00

0

5.830E+06 5.830E+06 NUBASE

0224 14-Si- 43 1.5- 0.015 s 100

β-:100.00

0

6.977E+06 6.977E+06 NUBASE

0225 14-Si- 44 0.0+ 0.01 s 100

β-:100.00

0

6.913E+06 6.913E+06 NUBASE

0226 15-P - 24 1.0+ 1E-09 s 100

p:50.00; β+:50.00

0

3.541E+06 3.541E+06 4.705E+05 NUBASE

0227 15-P - 25 0.5+ 3E-08 s 100

p:100.00

0

8.260E+05 NUBASE

0228 15-P - 26 3.0+ 0.03 s 83.33

β+:98.10; β+,2p:1.00;

β+,p:0.90

0

5.978E+06 5.978E+06 5.416E+04 NUBASE

0229 15-P - 27 0.5+ 0.26 s 30.77

β+:99.93; β+,pm:0.07

0

3.887E+06 3.887E+06 6.958E+02 NUBASE

0230 15-P - 28 3.0+ 0.27 s 0.18

β+:100.00

3

4.587E+06 4.729E+06 5.277E+03 ENSDF

0231 15-P - 29 0.5+ 4.142 s 0.36

β+:100.00

0

1.647E+06 1.647E+06 NUBASE

0232 15-P - 30 1.0+ 2.498 m 0.16

β+:100.00

4

1.435E+06 1.022E+06 ENSDF

0233 15-P - 31 0.5+

NUBASE

0234 15-P - 32 1.0+ 14.27 d 0.28

β-:100.00

1

6.929E+05 1.710E+03 UKPADD67

0235 15-P - 33 0.5+ 25.383 d 0.16

β-:100.00

1

7.640E+04 LNHB

0236 15-P - 34 1.0+ 12.4 s 0.81

β-:100.00

2

2.285E+06 3.475E+05 UKPADD67

0237 15-P - 35 0.5+ 47.3 s 1.48

β-:100.00

0

1.330E+06 1.330E+06 NUBASE

0238 15-P - 36 4.0- 5.6 s 5.36

β-:100.00

0

3.471E+06 3.471E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 57

MAIN DATA TABLES

Page 58: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0239 15-P - 37 0.5+ 2.31 s 5.63

β-:100.00

0

2.635E+06 2.635E+06 NUBASE

0240 15-P - 38 ? 0.64 s 21.88

β-:100.00

2

4.290E+06 2.778E+06 3.221E+03 ENSDF

0241 15-P - 39 0.5+ 0.19 s 26.32

β-:74.00; β-,n:26.00

0

2.923E+06 2.923E+06 3.848E+05 NUBASE

0242 15-P - 40 ? 0.15 s 5.33

β-:84.20; β-,n:15.80

0

4.418E+06 4.418E+06 2.757E+05 NUBASE

0243 15-P - 41 0.5+ 0.15 s 10

β-:70.00; β-,n:30.00

0

3.920E+06 3.920E+06 7.139E+05 NUBASE

0244 15-P - 42 ? 0.12 s 25

β-:50.00; β-,n:50.00

0

4.589E+06 4.589E+06 1.486E+06 NUBASE

0245 15-P - 43 0.5+ 0.033 s 9.09

β-,n:100.00

0

3.845E+06 3.845E+06 3.845E+06 NUBASE

0246 15-P - 44 ? 0.03 s 100

β-:100.00

0

7.073E+06 7.073E+06 NUBASE

0247 15-P - 45 0.5+ 8E-03 s 100

β-:100.00

0

7.050E+06 7.050E+06 NUBASE

0248 15-P - 46 ? 4E-03 s 100

β-:100.00

0

8.267E+06 8.267E+06 NUBASE

0249 16-S - 26 0.0+ 0.01 s 100

2p:100.00

0

6.370E+05 NUBASE

0250 16-S - 27 2.5+ 0.021 s 19.05

β+:98.00; β+,2p:2.00

0

6.023E+06 6.023E+06 5.939E+04 NUBASE

0251 16-S - 28 0.0+ 0.125 s 8

β+:79.30; β+,p:20.70

0

3.442E+06 3.442E+06 4.743E+05 NUBASE

0252 16-S - 29 2.5+ 0.187 s 2.14

β+:53.60; β+,p:46.40

0

3.745E+06 3.745E+06 1.281E+06 NUBASE

0253 16-S - 30 0.0+ 1.178 s 0.42

β+:100.00

4

2.084E+06 1.608E+06 ENSDF

0254 16-S - 31 0.5+ 2.572 s 0.51

β+:100.00

4

1.996E+06 1.038E+06 ENSDF

0255 16-S - 32 0.0+

NUBASE

0256 16-S - 33 1.5+

NUBASE

0257 16-S - 34 0.0+

NUBASE

0258 16-S - 35 1.5+ 87.32 d 0.18

β-:100.00

1

4.872E+04 LNHB

0259 16-S - 36 0.0+

NUBASE

0260 16-S - 37 3.5- 4.99 m 0.40

β-:100.00

2

7.932E+05 2.937E+06 UKPADD67

0261 16-S - 38 0.0+ 2.838 h 0.41

β-:100.00

2

4.890E+05 1.695E+06 ENSDF

0262 16-S - 39 ? 11.5 s 4.35

β-:100.00

2

2.256E+06 1.783E+06 ENSDF

0263 16-S - 40 0.0+ 8.8 s 25

β-:100.00

2

1.445E+06 1.471E+06 ENSDF

0264 16-S - 41 3.5- 1.99 s 2.51

β-:100.00

0

2.763E+06 2.763E+06 NUBASE

0265 16-S - 42 0.0+ 1.013E-03 s 1.48

β-:96.00; β-,n:4.00

0

2.329E+06 2.329E+06 1.559E+04 NUBASE

0266 16-S - 43 1.5- 0.26 s 5.77

β-:60.00; β-,n:40.00

0

2.927E+06 2.927E+06 4.869E+05 NUBASE

0267 16-S - 44 0.0+ 0.123 s 8.13

β-:82.00; β-,n:18.00

0

3.351E+06 3.351E+06 3.140E+05 NUBASE

0268 16-S - 45 1.5- 0.082 s 15.85

β-:46.00; β-,n:54.00

0

3.520E+06 3.520E+06 1.203E+06 NUBASE

0269 16-S - 46 0.0+ 0.03 s 100

β-:100.00

0

5.137E+06 5.137E+06 NUBASE

0270 16-S - 47 1.5- 0.02 s 100

β-:100.00

0

6.173E+06 6.173E+06 NUBASE

0271 16-S - 48 0.0+ 0.01 s 100

β-:100.00

0

5.967E+06 5.967E+06 NUBASE

0272 16-S - 49 1.5- 2E-07 s 100

n:100.00

0

7.287E+05 NUBASE

0273 17-Cl- 28 1.0+ 1E-09 s 100

p:100.00

0

1.731E+06 NUBASE

0274 17-Cl- 29 1.5+ 2E-08 s 100

p:100.00

0

1.781E+06 NUBASE

0275 17-Cl- 30 3.0+ 3E-08 s 100

p:100.00

0

3.110E+05 NUBASE

0276 17-Cl- 31 1.5+ 0.15 s 16.67

β+:99.30; β+,p:0.70

0

3.974E+06 3.974E+06 1.022E+04 NUBASE

0277 17-Cl- 32 1.0+ 0.298 s 0.34

β+:99.92; β+,n:0.05;

β+,p:0.03

0

4.226E+06 4.226E+06 1.023E+03 NUBASE

0278 17-Cl- 33 1.5+ 2.511 s 0.12

β+:100.00

4

2.082E+06 1.048E+06 ENSDF

0279 17-Cl- 34 0.0+ 1.526 s 0.20

β+:100.00

3

2.044E+06 1.029E+06 UKPADD67

0280 17-Cl- 34M 3.0+ 1.464E+05 32.1 m 0.31

β+:52.00; IT:48.00

4

4.414E+05 1.979E+06 UKPADD67

58 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 59: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0281 17-Cl- 35 1.5+

NUBASE

0282 17-Cl- 36 2.0+ 3.01E+05 y 1

β+:1.90; β-:98.10

4

2.731E+05 1.833E+01 LNHB

0283 17-Cl- 37 1.5+

NUBASE

0284 17-Cl- 38 2.0- 37.2 m 0.27

β-:100.00

2

1.523E+06 1.494E+06 UKPADD67

0285 17-Cl- 38M 5.0- 6.713E+05 0.715 s 0.42

IT:100.00

3

4.295E+02 6.713E+05 UKPADD67

0286 17-Cl- 39 1.5+ 55.6 m 0.36

β-:100.00

4

8.226E+05 1.454E+06 UKPADD67

0287 17-Cl- 40 2.0- 1.35 m 1.48

β-:100.00

2

1.519E+06 4.081E+06 ENSDF

0288 17-Cl- 41 ? 38.4 s 2.08

β-:100.00

0

1.919E+06 1.919E+06 NUBASE

0289 17-Cl- 42 ? 6.8 s 4.41

β-:100.00

0

3.171E+06 3.171E+06 NUBASE

0290 17-Cl- 43 1.5+ 3.07 s 2.28

β-:100.00

0

2.613E+06 2.613E+06 NUBASE

0291 17-Cl- 44 ? 0.56 s 19.64

β-:92.00; β-,n:8.00

0

3.890E+06 3.890E+06 7.417E+04 NUBASE

0292 17-Cl- 45 1.5+ 0.4 s 10

β-:76.00; β-,n:24.00

0

3.265E+06 3.265E+06 3.745E+05 NUBASE

0293 17-Cl- 46 ? 0.22 s 18.18

β-:40.00; β-,n:60.00

0

3.050E+06 3.050E+06 1.048E+06 NUBASE

0294 17-Cl- 47 1.5+ 0.2 s 100

β-:97.00; β-,n:3.00

0

5.060E+06 5.060E+06 8.347E+04 NUBASE

0295 17-Cl- 48 ? 0.1 s 100

β-:100.00

0

6.340E+06 6.340E+06 NUBASE

0296 17-Cl- 49 1.5+ 0.05 s 100

β-:100.00

0

6.150E+06 6.150E+06 NUBASE

0297 17-Cl- 50 ? 0.02 s 100

β-:100.00

0

7.267E+06 7.267E+06 NUBASE

0298 17-Cl- 51 1.5+ 2E-03 s 100

β-:100.00

0

7.100E+06 7.100E+06 NUBASE

0299 18-Ar- 30 0.0+ 2E-08 s 100

2p:100.00

0

1.432E+06 NUBASE

0300 18-Ar- 31 2.5+ 0.014 s 4.17

β+:28.40; β+,p:63.00;

β+,2p:7.20; β+,3p:1.40

0

4.867E+06 4.867E+06 3.129E+06 NUBASE

0301 18-Ar- 32 0.0+ 0.098 s 2.04

β+:57.00; β+,p:43.00

0

3.142E+06 3.142E+06 1.027E+06 NUBASE

0302 18-Ar- 33 0.5+ 0.173 s 1.16

β+:61.30; β+,p:38.70

0

3.278E+06 3.278E+06 9.039E+05 NUBASE

0303 18-Ar- 34 0.0+ 0.845 s 0.40

β+:100.00

4

2.289E+06 1.105E+06 ENSDF

0304 18-Ar- 35 1.5+ 1.775 s 0.23

β+:100.00

4

2.265E+06 1.050E+06 ENSDF

0305 18-Ar- 36 0.0+

NUBASE

0306 18-Ar- 37 1.5+ 35.04 d 0.09

β+:100.00

3

1.950E+03 2.229E+02 LNHB

0307 18-Ar- 38 0.0+

NUBASE

0308 18-Ar- 39 3.5- 269.006 y 3.35

β-:100.00

1

2.187E+05 UKPADD67

0309 18-Ar- 40 0.0+

NUBASE

0310 18-Ar- 41 3.5- 1.827 h 0.36

β-:100.00

4

4.636E+05 1.284E+06 UKPADD67

0311 18-Ar- 42 0.0+ 33.001 y 6.06

β-:100.00

1

2.328E+05 UKPADD67

0312 18-Ar- 43 2.5- 5.37 m 1.12

β-:100.00

2

1.378E+06 1.490E+06 ENSDF

0313 18-Ar- 44 0.0+ 11.87 m 0.42

β-:100.00

0

1.046E+06 1.046E+06 NUBASE

0314 18-Ar- 45 ? 21.48 s 0.70

β-:100.00

0

2.279E+06 2.279E+06 NUBASE

0315 18-Ar- 46 0.0+ 8.4 s 7.14

β-:100.00

0

1.899E+06 1.899E+06 NUBASE

0316 18-Ar- 47 1.5- 0.58 s 20.69

β-:99.00; β-,n:1.00

0

3.233E+06 3.233E+06 3.592E+03 NUBASE

0317 18-Ar- 48 0.0+ 0.5 s 100

β-:100.00

0

2.801E+06 2.801E+06 NUBASE

0318 18-Ar- 49 1.5- 0.17 s 29.41

β-:35.00; β-,n:65.00

0

2.379E+06 2.379E+06 9.592E+05 NUBASE

0319 18-Ar- 50 0.0+ 0.085 s 35.29

β-:65.00; β-,n:35.00

0

3.029E+06 3.029E+06 6.780E+05 NUBASE

0320 18-Ar- 51 1.5- 0.06 s 100

β-:100.00

0

4.733E+06 4.733E+06 NUBASE

0321 18-Ar- 52 0.0+ 0.01 s 100

β-:100.00

0

4.400E+06 4.400E+06 NUBASE

0322 18-Ar- 53 2.5- 3E-03 s 100

β-:100.00

0

5.533E+06 5.533E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 59

MAIN DATA TABLES

Page 60: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0323 19-K - 32 1.0+ 1E-09 s 100

p:100.00

0

1.841E+06 NUBASE

0324 19-K - 33 1.5+ 2.5E-08 s 100

p:100.00

0

1.671E+06 NUBASE

0325 19-K - 34 1.0+ 4E-08 s 100

p:100.00

0

6.151E+05 NUBASE

0326 19-K - 35 1.5+ 0.178 s 4.49

β+:100.00

4

3.589E+06 4.268E+06 2.766E+03 ENSDF

0327 19-K - 36 2.0+ 0.342 s 0.58

β+:100.00

4

3.470E+06 5.449E+06 2.807E+03 ENSDF

0328 19-K - 37 1.5+ 1.226 s 0.57

β+:100.00

4

2.347E+06 1.072E+06 ENSDF

0329 19-K - 38 3.0+ 7.61 m 0.53

β+:100.00

4

1.201E+06 3.190E+06 UKPADD67

0330 19-K - 38M 0.0+ 1.304E+05 0.924 s 0.22

β+:100.00

3

2.312E+06 1.031E+06 UKPADD67

0331 19-K - 39 1.5+

NUBASE

0332 19-K - 40 4.0- 1.265E+09 y 1.58

β+:10.86; β-:89.14

5

4.534E+05 1.558E+05 LNHB

0333 19-K - 41 1.5+

NUBASE

0334 19-K - 42 2.0- 12.359 h 0.02

β-:100.00

4

1.421E+06 2.760E+05 LNHB

0335 19-K - 43 1.5+ 22.2 h 0.90

β-:100.00

4

3.096E+05 9.662E+05 UKPADD67

0336 19-K - 44 2.0- 22.13 m 0.86

β-:100.00

4

1.436E+06 2.391E+06 UKPADD67

0337 19-K - 45 1.5+ 17.3 m 3.47

β-:100.00

4

9.865E+05 1.834E+06 ENSDF

0338 19-K - 46 2.0- 1.75 m 9.52

β-:100.00

2

2.321E+06 2.651E+06 ENSDF

0339 19-K - 47 0.5+ 17.5 s 1.37

β-:100.00

2

1.809E+06 2.624E+06 ENSDF

0340 19-K - 48 2.0- 6.8 s 2.94

β-:100.00

2

2.658E+06 6.450E+06 1.571E+03 ENSDF

0341 19-K - 49 1.5+ 1.26 s 3.97

β-:14.00; β-,n:86.00

0

1.764E+06 1.764E+06 1.252E+06 NUBASE

0342 19-K - 50 ? 0.472 s 0.85

β-:71.00; β-,n:29.00

0

3.936E+06 3.936E+06 5.704E+05 NUBASE

0343 19-K - 51 1.5+ 0.365 s 1.37

β-:53.00; β-,n:47.00

0

3.565E+06 3.565E+06 1.116E+06 NUBASE

0344 19-K - 52 2.0- 0.105 s 4.76

β-:15.00; β-,n:64.00;

β-,2n:21.00

0

3.049E+06 3.049E+06 2.234E+06 NUBASE

0345 19-K - 53 1.5+ 0.03 s 16.67

β-:16.00; β-,n:67.00;

β-,2n:17.00

0

3.259E+06 3.259E+06 2.411E+06 NUBASE

0346 19-K - 54 2.0- 0.01 s 50

β-:100.00

0

6.163E+06 6.163E+06 NUBASE

0347 19-K - 55 1.5+ 3E-03 s 100

β-:100.00

0

5.950E+06 5.950E+06 NUBASE

0348 20-Ca- 34 0.0+ 3.5E-08 s 100

2p:100.00

0

7.722E+05 NUBASE

0349 20-Ca- 35 0.5+ 0.026 s 0.78

β+:0.10; β+,p:95.70;

β+,2p:4.20

0

3.874E+06 3.874E+06 3.869E+06 NUBASE

0350 20-Ca- 36 0.0+ 0.102 s 1.96

β+:43.20; β+,p:56.80

0

2.905E+06 2.905E+06 1.323E+06 NUBASE

0351 20-Ca- 37 1.5+ 0.181 s 0.55

β+:17.90; β+,p:82.10

0

2.702E+06 2.702E+06 2.007E+06 NUBASE

0352 20-Ca- 38 0.0+ 0.44 s 1.82

β+:0.02; β+

m:99.98

4

2.433E+06 1.374E+06 1.000E+03 ENSDF

0353 20-Ca- 39 1.5+ 0.86 s 0.16

β+:100.00

4

2.561E+06 1.022E+06 ENSDF

0354 20-Ca- 40 0.0+

NUBASE

0355 20-Ca- 41 3.5- 1.03E+05 y 3.88

β+:100.00

3

2.843E+03 4.371E+02 UKPADD67

0356 20-Ca- 42 0.0+

NUBASE

0357 20-Ca- 43 3.5-

NUBASE

0358 20-Ca- 44 0.0+

NUBASE

0359 20-Ca- 45 3.5- 163 d 0.61

β-:100.00; β-

m:~

4

7.720E+04 9.543E-03 LNHB

0360 20-Ca- 46 0.0+

NUBASE

0361 20-Ca- 47 3.5- 4.538 d 0.04

β-:100.00

4

3.446E+05 1.060E+06 UKPADD67

0362 20-Ca- 48 0.0+ 5.3E+19 y 32.08

2β-:50.00; β-:50.00

0

2.184E+06 4.700E+04 NUBASE

60 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 61: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0363 20-Ca- 49 1.5- 8.72 m 0.23

β-:100.00

2

8.695E+05 3.167E+06 UKPADD67

0364 20-Ca- 50 0.0+ 13.9 s 4.32

β-m:100.00

0

1.570E+06 1.570E+06 NUBASE

0365 20-Ca- 51 1.5- 10 s 8

β-:100.00

0

2.453E+06 2.453E+06 NUBASE

0366 20-Ca- 52 0.0+ 4.6 s 6.52

β-:98.00; β-,n:2.00

0

2.578E+06 2.578E+06 1.318E+04 NUBASE

0367 20-Ca- 53 1.5- 0.09 s 16.67

β-:70.00; β-,n:30.00

0

2.597E+06 2.597E+06 3.292E+05 NUBASE

0368 20-Ca- 54 0.0+ 0.05 s 100

β-:100.00

0

3.443E+06 3.443E+06 NUBASE

0369 20-Ca- 55 2.5- 0.03 s 100

β-:100.00

0

3.820E+06 3.820E+06 NUBASE

0370 20-Ca- 56 0.0+ 0.01 s 100

β-:100.00

0

3.943E+06 3.943E+06 NUBASE

0371 20-Ca- 57 2.5- 5E-03 s 100

β-:100.00

0

4.523E+06 4.523E+06 NUBASE

0372 21-Sc- 36 ? 1E-09 s 100

p:100.00

0

2.011E+06 NUBASE

0373 21-Sc- 37 3.5- 1E-09 s 100

p:100.00

0

1.991E+06 NUBASE

0374 21-Sc- 38 2.0- 3E-07 s 100

p:100.00

0

9.330E+05 NUBASE

0375 21-Sc- 39 3.5- 3E-07 s 100

p:100.00

0

6.020E+05 NUBASE

0376 21-Sc- 40 4.0- 0.182 s 0.38

β+:100.00

4

3.399E+06 7.119E+06 2.772E+03 ENSDF

0377 21-Sc- 41 3.5- 0.596 s 0.29

β+:100.00

4

2.541E+06 1.022E+06 ENSDF

0378 21-Sc- 42 0.0+ 0.681 s 0.04

β+:100.00

4

2.508E+06 1.021E+06 ENSDF

0379 21-Sc- 42M 7.0+ 6.163E+05 1.033 m 0.48

β+:100.00

4

1.256E+06 4.204E+06 ENSDF

0380 21-Sc- 43 3.5- 3.891 h 0.31

β+:100.00

4

4.198E+05 9.848E+05 ENSDF

0381 21-Sc- 44 2.0+ 3.97 h 1.01

β+:100.00

4

5.960E+05 2.136E+06 LNHB

0382 21-Sc- 44M 6.0+ 2.711E+05 2.442 d 0.17

β+:1.23; IT:98.77

4

3.282E+04 2.753E+05 UKPADD67

0383 21-Sc- 45 3.5-

NUBASE

0384 21-Sc- 45M 1.5+ 1.240E+04 0.318 s 2.20

IT:100.00

3

1.163E+04 6.118E+02 ENSDF

0385 21-Sc- 46 4.0+ 83.788 d 0.02

β-:100.00

4

1.121E+05 2.010E+06 LNHB

0386 21-Sc- 46M 1.0- 1.425E+05 18.7 s 0.37

IT:100.00

3

5.890E+04 8.296E+04 UKPADD67

0387 21-Sc- 47 3.5- 3.351 d 0.06

β-:100.00

4

1.626E+05 1.084E+05 LNHB

0388 21-Sc- 48 6.0+ 1.82 d 0.21

β-:100.00

2

2.196E+05 3.350E+06 UKPADD67

0389 21-Sc- 49 3.5- 57.2 m 0.35

β-:100.00

2

8.199E+05 3.340E+03 UKPADD67

0390 21-Sc- 50 5.0+ 1.708 m 0.49

β-:100.00

2

1.624E+06 3.198E+06 UKPADD67

0391 21-Sc- 50M 2.0+ 2.569E+05 0.35 s 8.57

β-:1.25; IT:98.75

4

4.069E+04 2.644E+05 UKPADD67

0392 21-Sc- 51 3.5- 12.4 s 0.81

β-:100.00

2

1.841E+06 2.350E+06 ENSDF

0393 21-Sc- 52 3.0+ 8.2 s 2.44

β-:100.00

2

2.849E+06 2.893E+06 1.165E+03 ENSDF

0394 21-Sc- 53 3.5- 3 s 100

β-:100.00

0

3.070E+06 3.070E+06 NUBASE

0395 21-Sc- 54 3.0+ 0.26 s 11.54

β-:100.00

0

3.790E+06 3.790E+06 NUBASE

0396 21-Sc- 55 3.5- 0.12 s 33.33

β-:100.00

0

4.030E+06 4.030E+06 NUBASE

0397 21-Sc- 56 3.0+ 0.08 s 100

β-:100.00

0

4.557E+06 4.557E+06 NUBASE

0398 21-Sc- 57 3.5- 0.013 s 30.77

β-:67.00; β-,n:33.00

0

3.710E+06 3.710E+06 8.397E+05 NUBASE

0399 21-Sc- 58 3.0+ 0.012 s 41.67

β-:100.00

0

5.200E+06 5.200E+06 NUBASE

0400 21-Sc- 59 3.5- 0.01 s 100

β-:100.00

0

5.060E+06 5.060E+06 NUBASE

0401 21-Sc- 60 3.0+ 3E-03 s 100

β-:100.00

0

5.883E+06 5.883E+06 NUBASE

0402 22-Ti- 38 0.0+ 1.2E-07 s 100

2p:100.00

0

9.620E+05 NUBASE

0403 22-Ti- 39 1.5+ 0.031 s 12.90

β+:~; β+,p:85.00;

β+,2p:15.00

0

3.897E+06 3.897E+06 3.897E+06 NUBASE

0404 22-Ti- 40 0.0+ 0.053 s 2.81

β+,p:100.00

0

2.784E+06 2.784E+06 2.784E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 61

MAIN DATA TABLES

Page 62: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0405 22-Ti- 41 1.5+ 0.081 s 1.48

β+,p:100.00

0

2.964E+06 2.964E+06 2.964E+06 NUBASE

0406 22-Ti- 42 0.0+ 0.199 s 3.02

β+:100.00

4

2.637E+06 1.385E+06 1.014E+03 ENSDF

0407 22-Ti- 43 3.5- 0.509 s 0.98

β+:100.00

4

2.637E+06 1.202E+06 ENSDF

0408 22-Ti- 44 0.0+ 60 y 1.83

β+:100.00

4

1.063E+04 1.383E+05 LNHB

0409 22-Ti- 45 3.5- 3.08 h 0.32

β+:100.00

4

3.733E+05 8.718E+05 UKPADD67

0410 22-Ti- 46 0.0+

NUBASE

0411 22-Ti- 47 2.5-

NUBASE

0412 22-Ti- 48 0.0+

NUBASE

0413 22-Ti- 49 3.5-

NUBASE

0414 22-Ti- 50 0.0+

NUBASE

0415 22-Ti- 51 1.5- 5.8 m 0.52

β-:100.00

4

8.689E+05 3.646E+05 UKPADD67

0416 22-Ti- 52 0.0+ 1.7 m 5.88

β-:100.00

4

7.546E+05 1.284E+05 ENSDF

0417 22-Ti- 53 1.5- 32.7 s 2.75

β-:100.00

0

1.673E+06 1.673E+06 NUBASE

0418 22-Ti- 54 0.0+ 1.5 s 26.67

β-:100.00

0

1.434E+06 1.434E+06 NUBASE

0419 22-Ti- 55 1.5- 0.49 s 18.37

β-:100.00

0

2.493E+06 2.493E+06 NUBASE

0420 22-Ti- 56 0.0+ 0.164 s 14.63

β-:100.00

0

2.380E+06 2.380E+06 NUBASE

0421 22-Ti- 57 2.5- 0.06 s 26.67

β-:99.70; β-,n:0.30

0

3.543E+06 3.543E+06 3.352E+03 NUBASE

0422 22-Ti- 58 0.0+ 0.054 s 12.96

β-:100.00

0

3.147E+06 3.147E+06 NUBASE

0423 22-Ti- 59 2.5- 0.03 s 8.33

β-:100.00

0

3.950E+06 3.950E+06 NUBASE

0424 22-Ti- 60 0.0+ 0.022 s 9.09

β-:100.00

0

3.643E+06 3.643E+06 NUBASE

0425 22-Ti- 61 0.5- 0.01 s 100

β-:100.00

0

4.570E+06 4.570E+06 NUBASE

0426 22-Ti- 62 0.0+ 0.01 s 100

β-:100.00

0

4.257E+06 4.257E+06 NUBASE

0427 22-Ti- 63 0.5- 3E-03 s 100

β-:100.00

0

5.237E+06 5.237E+06 NUBASE

0428 23-V - 40 2.0- 1E-09 s 100

p:100.00

0

1.541E+06 NUBASE

0429 23-V - 41 3.5- 1E-09 s 100

p:100.00

0

1.351E+06 NUBASE

0430 23-V - 42 2.0- 5.5E-08 s 100

p:100.00

0

2.410E+05 NUBASE

0431 23-V - 43 3.5- 0.08 s 100

β+:100.00

0

3.767E+06 3.767E+06 NUBASE

0432 23-V - 44 2.0+ 0.111 s 6.31

β+:100.00

4

4.349E+06 4.526E+06 2.991E+03 ENSDF

0433 23-V - 44M 6.0+ 2.700E+05 0.15 s 2

β+:100.00

0

4.566E+06 4.566E+06 NUBASE

0434 23-V - 45 3.5- 0.539 s 3.34

β+:100.00

4

2.854E+06 1.022E+06 1.038E+03 ENSDF

0435 23-V - 46 0.0+ 0.423 s 0.03

β+:100.00

4

2.814E+06 1.022E+06 ENSDF

0436 23-V - 46M 3.0+ 8.011E+05 1.02E-03 s 6.86

IT:100.00

1

8.011E+05 ENSDF

0437 23-V - 47 1.5- 32.6 m 0.92

β+:100.00

4

8.031E+05 9.950E+05 ENSDF

0438 23-V - 48 4.0+ 15.974 d 0.02

β+:100.00

4

1.493E+05 2.916E+06 UKPADD67

0439 23-V - 49 3.5- 330 d 6.06

β+:100.00

3

3.583E+03 9.469E+02 UKPADD67

0440 23-V - 50 6.0+ 1.4E+17 y 28.57

β+:83.00; β-:17.00

5

1.568E+04 1.423E+06 ENSDF

0441 23-V - 51 3.5-

NUBASE

0442 23-V - 52 3.0+ 3.745 m 0.13

β-:100.00

4

1.064E+06 1.448E+06 UKPADD67

0443 23-V - 53 3.5- 1.62 m 2.47

β-:100.00

2

1.005E+06 1.042E+06 UKPADD67

0444 23-V - 54 3.0+ 49.8 s 1

β-:100.00

2

1.358E+06 4.098E+06 UKPADD67

0445 23-V - 55 3.5- 6.54 s 2.29

β-:100.00

2

2.382E+06 6.892E+05 ENSDF

0446 23-V - 56 1.0+ 0.216 s 1.85

β-:100.00

0

3.067E+06 3.067E+06 NUBASE

0447 23-V - 57 1.5- 0.35 s 2.86

β-:99.60; β-,n:0.40

0

2.770E+06 2.770E+06 3.020E+03 NUBASE

62 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 63: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0448 23-V - 58 3.0+ 0.191 s 4.19

β-:20.00; β-,n:80.00

0

1.623E+06 1.623E+06 8.486E+05 NUBASE

0449 23-V - 59 3.5- 0.075 s 9.33

β-:100.00

0

3.607E+06 3.607E+06 NUBASE

0450 23-V - 60 3.0+ 0.122 s 14.75

β-:100.00

0

4.640E+06 4.640E+06 NUBASE

0451 23-V - 61 3.5- 0.047 s 2.55

β-:94.00; β-,n:6.00

0

4.153E+06 4.153E+06 1.360E+05 NUBASE

0452 23-V - 62 3.0+ 0.034 s 5.97

β-:100.00

0

5.330E+06 5.330E+06 NUBASE

0453 23-V - 63 3.5- 0.017 s 17.65

β-:65.00; β-,n:35.00

0

4.168E+06 4.168E+06 1.000E+06 NUBASE

0454 23-V - 64 ? 0.01 s 100

β-:100.00

0

5.917E+06 5.917E+06 NUBASE

0455 23-V - 65 2.5- 0.01 s 100

β-:100.00

0

5.517E+06 5.517E+06 NUBASE

0456 24-Cr- 42 0.0+ 0.014 s 21.43

β+:100.00

0

4.720E+06 4.720E+06 NUBASE

0457 24-Cr- 43 1.5+ 0.022 s 3.24

β+:71.00; β+,p:23.00;

β+,2p:6.00

0

4.843E+06 4.843E+06 1.082E+06 NUBASE

0458 24-Cr- 44 0.0+ 0.054 s 7.41

β+:93.00; β+,p:7.00

0

3.455E+06 3.455E+06 1.500E+05 NUBASE

0459 24-Cr- 45 3.5- 0.05 s 12

β+:73.00; β+,p:27.00

0

3.903E+06 3.903E+06 7.620E+05 NUBASE

0460 24-Cr- 45M 1.5+ 5.000E+04 1E-03 s 100

IT:50.00; β+:50.00

0

2.160E+06 2.185E+06 NUBASE

0461 24-Cr- 46 0.0+ 0.26 s 23.08

β+:100.00

3

3.089E+06 1.022E+06 1.168E+03 ENSDF

0462 24-Cr- 47 1.5- 0.5 s 3

β+:100.00

4

3.012E+06 1.025E+06 1.093E+03 ENSDF

0463 24-Cr- 48 0.0+ 21.56 h 0.14

β+:100.00

4

8.222E+03 4.331E+05 ENSDF

0464 24-Cr- 49 2.5- 41.9 m 0.72

β+:100.00

4

5.965E+05 1.047E+06 UKPADD67

0465 24-Cr- 50 0.0+ 1.8E+17 y 100

2β+:100.00

0

1.167E+06 NUBASE

0466 24-Cr- 51 3.5- 27.703 d 0.01

β+:100.00

4

3.665E+03 3.271E+04 LNHB

0467 24-Cr- 52 0.0+

NUBASE

0468 24-Cr- 53 1.5-

NUBASE

0469 24-Cr- 54 0.0+

NUBASE

0470 24-Cr- 55 1.5- 3.54 m 0.85

β-:100.00

4

1.097E+06 4.243E+03 UKPADD67

0471 24-Cr- 56 0.0+ 5.94 m 1.68

β-:100.00

4

6.067E+05 9.169E+04 ENSDF

0472 24-Cr- 57 1.5- 21.1 s 4.74

β-:100.00

4

1.949E+06 4.622E+05 ENSDF

0473 24-Cr- 58 0.0+ 7 s 4.29

β-:100.00

0

1.360E+06 1.360E+06 NUBASE

0474 24-Cr- 59 2.5- 0.46 s 10.87

β-:100.00

0

2.530E+06 2.530E+06 NUBASE

0475 24-Cr- 60 0.0+ 0.56 s 10.71

β-:100.00

0

2.227E+06 2.227E+06 NUBASE

0476 24-Cr- 61 2.5- 0.261 s 5.75

β-:100.00

0

3.127E+06 3.127E+06 NUBASE

0477 24-Cr- 62 0.0+ 0.199 s 4.52

β-:50.00; β-

m:50.00

0

2.543E+06 2.543E+06 NUBASE

0478 24-Cr- 63 0.5- 0.129 s 1.55

β-:100.00

0

3.607E+06 3.607E+06 NUBASE

0479 24-Cr- 64 0.0+ 0.043 s 2.33

β-:100.00

0

3.157E+06 3.157E+06 NUBASE

0480 24-Cr- 65 0.5- 0.027 s 11.11

β-:100.00

0

4.290E+06 4.290E+06 NUBASE

0481 24-Cr- 66 0.0+ 0.01 s 60

β-:100.00

0

3.817E+06 3.817E+06 NUBASE

0482 24-Cr- 67 0.5- 0.01 s 100

β-:100.00

0

4.783E+06 4.783E+06 NUBASE

0483 25-Mn- 44 2.0- 1.05E-07 s 100

p:100.00

0

1.241E+06 NUBASE

0484 25-Mn- 45 3.5- 7E-08 s 100

p:100.00

0

1.061E+06 NUBASE

0485 25-Mn- 46 4.0+ 0.037 s 8.11

β+:60.00; β+,p:22.00;

β+,2p:18.00

0

4.570E+06 4.570E+06 1.149E+06 NUBASE

0486 25-Mn- 46M 1.0- 1.500E+05 1E-03 s 100

β+:100.00

0

5.751E+06 5.751E+06 NUBASE

0487 25-Mn- 47 2.5- 0.1 s 50

β+:96.60; β+,p:1.70;

β+,pm:1.70

0

4.020E+06 4.020E+06 6.055E+04 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 63

MAIN DATA TABLES

Page 64: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0488 25-Mn- 48 4.0+ 0.158 s 1.39

β+:99.72; β+,p:0.28;

β+,n:~

0

4.491E+06 4.491E+06 3.784E+03 NUBASE

0489 25-Mn- 49 2.5- 0.382 s 1.83

β+:100.00

4

3.105E+06 1.094E+06 1.119E+03 ENSDF

0490 25-Mn- 50 0.0+ 0.284 s 0.16

β+:100.00

4

3.100E+06 1.021E+06 1.083E+03 ENSDF

0491 25-Mn- 50M 5.0+ 2.290E+05 1.75 m 1.71

β+:100.00

0

2.621E+06 2.621E+06 NUBASE

0492 25-Mn- 51 2.5- 46.2 m 0.22

β+:100.00

4

9.350E+05 9.977E+05 ENSDF

0493 25-Mn- 52 6.0+ 5.595 d 0.05

β+:100.00

4

7.156E+04 3.461E+06 LNHB

0494 25-Mn- 52M 2.0+ 3.777E+05 21.2 m 1.89

β+:98.25; IT:1.75

4

1.133E+06 2.409E+06 LNHB

0495 25-Mn- 53 3.5- 3.68E+06 y 5.71

β+:100.00

3

4.002E+03 1.422E+03 UKPADD67

0496 25-Mn- 54 3.0+ 312.13 d 0.01

β+:100.00

4

4.027E+03 8.360E+05 LNHB

0497 25-Mn- 55 2.5-

NUBASE

0498 25-Mn- 56 3.0+ 2.582 h 0.19

β-:100.00

4

8.212E+05 1.710E+06 LNHB

0499 25-Mn- 57 2.5- 1.423 m 2.11

β-:100.00

4

1.104E+06 9.963E+04 ENSDF

0500 25-Mn- 58 3.0+ 1.087 m 0.77

β-:100.00

4

1.711E+06 2.382E+06 UKPADD67

0501 25-Mn- 58M 0.0+ 7.300E+04 2.7 s 22.22

β-:100.00

4

2.828E+06 1.201E+05 UKPADD67

0502 25-Mn- 59 2.5- 4.59 s 1.09

β-:100.00

4

2.060E+06 5.379E+05 ENSDF

0503 25-Mn- 60 0.0+ 51 s 11.76

β-:100.00

1

3.840E+06 1.215E+03 ENSDF

0504 25-Mn- 60M 3.0+ 2.719E+05 1.77 s 1.13

β-:88.50; IT:11.50

0

2.509E+06 2.540E+06 NUBASE

0505 25-Mn- 61 2.5- 0.67 s 5.97

β-:100.00

2

3.256E+06 1.303E+05 ENSDF

0506 25-Mn- 62 3.0+ 0.88 s 17.05

β-:100.00

2

3.803E+06 2.148E+06 1.552E+03 ENSDF

0507 25-Mn- 62M 1.0+ 1.000E+03 0.092 s 14.13

β-:100.00

0

3.621E+06 3.621E+06 NUBASE

0508 25-Mn- 63 2.5- 0.275 s 1.45

β-:100.00

0

3.067E+06 3.067E+06 NUBASE

0509 25-Mn- 64 1.0+ 0.089 s 2.82

β-:100.00

0

4.050E+06 4.050E+06 NUBASE

0510 25-Mn- 65 2.5- 0.092 s 1.09

β-:100.00

0

3.403E+06 3.403E+06 NUBASE

0511 25-Mn- 66 ? 0.064 s 2.80

β-:100.00

0

4.440E+06 4.440E+06 NUBASE

0512 25-Mn- 67 2.5- 0.045 s 8.89

β-:100.00

0

4.097E+06 4.097E+06 NUBASE

0513 25-Mn- 68 ? 0.028 s 14.29

β-:100.00

0

4.843E+06 4.843E+06 NUBASE

0514 25-Mn- 69 2.5- 0.014 s 28.57

β-:76.00; β-,n:24.00

0

3.904E+06 3.904E+06 5.855E+05 NUBASE

0515 26-Fe- 45 1.5+ 4.9E-03 s 30.61

2p:75.00; β+,p:25.00

0

1.234E+06 1.234E+06 2.083E+06 NUBASE

0516 26-Fe- 46 0.0+ 9E-03 s 44.44

β+m:64.00; β+,p:18.00;

β+,pm:18.00

0

3.887E+06 3.887E+06 1.117E+06 NUBASE

0517 26-Fe- 47 3.5- 0.022 s 3.21

β+:13.00; β+,p:87.00

0

4.063E+06 4.063E+06 3.385E+06 NUBASE

0518 26-Fe- 48 0.0+ 0.044 s 15.91

β+:96.40; β+,p:3.60

0

3.668E+06 3.668E+06 8.198E+04 NUBASE

0519 26-Fe- 49 3.5- 0.07 s 4.29

β+:48.00; β+,p:52.00

0

3.509E+06 3.509E+06 1.424E+06 NUBASE

0520 26-Fe- 50 0.0+ 0.155 s 7.10

β+:100.00

0

2.716E+06 2.716E+06 NUBASE

0521 26-Fe- 51 2.5- 5.083 h 1.64

β+:100.00

4

3.270E+06 1.062E+06 1.174E+03 ENSDF

0522 26-Fe- 52 0.0+ 8.275 h 0.10

β+m:100.00

4

1.920E+05 7.424E+05 ENSDF

0523 26-Fe- 52M 12.0+ 6.820E+06 45.9 s 1.31

β+:100.00

4

1.982E+06 4.886E+06 ENSDF

0524 26-Fe- 53 3.5- 8.51 m 0.82

β+:100.00

4

1.107E+06 1.184E+06 UKPADD67

0525 26-Fe- 53M 9.5- 3.040E+06 2.58 m 1.16

IT:100.00

1

3.035E+06 UKPADD67

0526 26-Fe- 54 0.0+

NUBASE

0527 26-Fe- 55 1.5- 2.735 y 0.80

β+:100.00

4

4.004E+03 1.661E+03 LNHB

0528 26-Fe- 56 0.0+

NUBASE

64 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 65: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0529 26-Fe- 57 0.5-

NUBASE

0530 26-Fe- 58 0.0+

NUBASE

0531 26-Fe- 59 1.5- 44.495 d 0.02

β-:100.00

4

1.184E+05 1.189E+06 LNHB

0532 26-Fe- 60 0.0+ 1.5E+06 y 20

β-m:100.00

1

5.110E+04 ENSDF

0533 26-Fe- 61 ? 5.98 m 1

β-:100.00

0

1.326E+06 1.326E+06 NUBASE

0534 26-Fe- 62 0.0+ 1.133 m 2.94

β-:100.00

2

8.240E+05 5.061E+05 ENSDF

0535 26-Fe- 63 2.5- 6.1 s 9.84

β-:100.00

4

2.604E+06 3.177E+05 UKPADD67

0536 26-Fe- 64 0.0+ 2 s 10

β-:100.00

2

2.105E+06 1.554E+04 ENSDF

0537 26-Fe- 65 0.5- 1.3 s 23.08

β-:100.00

0

2.763E+06 2.763E+06 NUBASE

0538 26-Fe- 66 0.0+ 0.44 s 9.09

β-:100.00

0

2.180E+06 2.180E+06 NUBASE

0539 26-Fe- 67 0.5- 0.394 s 2.28

β-:100.00

0

3.123E+06 3.123E+06 NUBASE

0540 26-Fe- 68 0.0+ 0.187 s 3.21

β-m:100.00

0

2.690E+06 2.690E+06 NUBASE

0541 26-Fe- 69 0.5- 0.109 s 8.26

β-:93.00; β-,nm:7.00

0

3.679E+06 3.679E+06 8.275E+04 NUBASE

0542 26-Fe- 70 0.0+ 0.094 s 18.09

β-m:100.00

0

3.180E+06 3.180E+06 NUBASE

0543 26-Fe- 71 3.5+ 0.03 s 100

β-:100.00

0

4.290E+06 4.290E+06 NUBASE

0544 26-Fe- 72 0.0+ 0.01 s 100

β-:100.00

0

3.667E+06 3.667E+06 NUBASE

0545 27-Co- 47 3.5- 1E-09 s 100

p:100.00

0

2.651E+06 NUBASE

0546 27-Co- 48 6.0+ 1E-09 s 100

p:100.00

0

9.710E+05 NUBASE

0547 27-Co- 49 3.5- 3.5E-08 s 100

p:100.00

0

1.291E+06 NUBASE

0548 27-Co- 50 6.0+ 0.044 s 9.09

β+:46.00; β+,p:54.00

0

4.422E+06 4.422E+06 1.772E+06 NUBASE

0549 27-Co- 51 3.5- 0.06 s 100

β+:100.00

0

4.317E+06 4.317E+06 NUBASE

0550 27-Co- 52 6.0+ 0.115 s 20

β+:50.00; β+

m:50.00

0

3.669E+06 3.669E+06 NUBASE

0551 27-Co- 52M 2.0+ 3.800E+05 0.104 s 10.58

β+:50.00; IT:50.00

0

2.465E+06 2.655E+06 NUBASE

0552 27-Co- 53 3.5- 0.24 s 8.33

β+:100.00

4

3.397E+06 1.096E+06 1.213E+03 ENSDF

0553 27-Co- 53M 9.5- 3.195E+06 0.247 s 4.86

β+m:98.50; p:1.50

0

2.776E+06 2.776E+06 2.390E+04 NUBASE

0554 27-Co- 54 0.0+ 0.193 s 0.07

β+:100.00

3

3.399E+06 1.021E+06 1.183E+03 ENSDF

0555 27-Co- 54M 7.0+ 1.974E+05 1.48 m 1.35

β+:100.00

4

2.047E+06 3.931E+06 ENSDF

0556 27-Co- 55 3.5- 17.53 h 0.17

β+:100.00

4

4.366E+05 2.007E+06 UKPADD67

0557 27-Co- 56 4.0+ 77.31 d 0.25

β+:100.00

4

1.222E+05 3.592E+06 LNHB

0558 27-Co- 57 3.5- 271.8 d 0.02

β+:100.00

4

1.829E+04 1.252E+05 LNHB

0559 27-Co- 58 2.0+ 70.86 d 0.10

β+:100.00

4

3.431E+04 9.762E+05 UKPADD67

0560 27-Co- 58M 5.0+ 2.488E+04 8.9 h 1.12

IT:100.00

3

2.227E+04 1.817E+03 LNHB

0561 27-Co- 59 3.5-

NUBASE

0562 27-Co- 60 5.0+ 5.271 y 0.02

β-:100.00

4

9.677E+04 2.504E+06 LNHB

0563 27-Co- 60M 2.0+ 5.860E+04 10.47 m 0.38

IT:99.75; β-:0.25

4

5.569E+04 6.786E+03 LNHB

0564 27-Co- 61 3.5- 1.65 h 0.30

β-:100.00

4

4.664E+05 9.697E+04 ENSDF

0565 27-Co- 62 2.0+ 1.5 m 2.67

β-:100.00

2

1.640E+06 1.600E+06 ENSDF

0566 27-Co- 62M 5.0+ 2.200E+04 13.91 m 0.36

β-:99.00; IT:1.00

0

1.761E+06 1.761E+06 NUBASE

0567 27-Co- 63 3.5- 27.4 s 1.82

β-:100.00

4

1.568E+06 1.441E+05 ENSDF

0568 27-Co- 64 1.0+ 0.3 s 10

β-:100.00

2

3.289E+06 1.812E+05 ENSDF

0569 27-Co- 65 3.5- 1.2 s 5

β-:100.00

4

2.665E+06 1.147E+05 ENSDF

0570 27-Co- 66 3.0+ 0.233 s 7.30

β-:100.00

2

3.356E+06 2.754E+06 1.170E+03 ENSDF

0571 27-Co- 67 3.5- 0.425 s 4.71

β-:100.00

2

2.754E+06 6.941E+05 ENSDF

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 65

MAIN DATA TABLES

Page 66: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0572 27-Co- 68 7.0- 0.199 s 10.55

β-:100.00

4

3.839E+06 3.444E+06 1.580E+03 ENSDF

0573 27-Co- 68M 3.0+ 1.500E+05 1.6 s 18.75

β-:50.00; IT:50.00

0

2.044E+06 2.119E+06 NUBASE

0574 27-Co- 69 3.5- 0.227 s 5.73

β-:99.00; β-,n:1.00

0

3.307E+06 3.307E+06 1.348E+04 NUBASE

0575 27-Co- 70 6.0- 0.119 s 5.04

β-:100.00

0

4.503E+06 4.503E+06 NUBASE

0576 27-Co- 70M 3.0+ 2.000E+05 0.5 s 36

β-:100.00

0

4.570E+06 4.570E+06 NUBASE

0577 27-Co- 71 3.5- 0.097 s 2.06

β-:100.00

0

3.777E+06 3.777E+06 NUBASE

0578 27-Co- 72 ? 0.09 s 22.22

β-:100.00

0

4.880E+06 4.880E+06 NUBASE

0579 27-Co- 73 3.5- 0.08 s 100

β-:100.00

0

4.273E+06 4.273E+06 NUBASE

0580 27-Co- 74 ? 0.05 s 100

β-:100.00

0

5.373E+06 5.373E+06 NUBASE

0581 27-Co- 75 3.5- 0.04 s 100

β-:100.00

0

4.800E+06 4.800E+06 NUBASE

0582 28-Ni- 48 0.0+ 0.01 s 100

2p:100.00

0

3.062E+06 NUBASE

0583 28-Ni- 49 3.5- 0.013 s 30.77

β+:100.00

0

6.193E+06 6.193E+06 NUBASE

0584 28-Ni- 50 0.0+ 9.1E-03 s 19.78

β+:100.00

0

4.470E+06 4.470E+06 NUBASE

0585 28-Ni- 51 3.5- 0.03 s 100

β+:100.00

0

5.277E+06 5.277E+06 NUBASE

0586 28-Ni- 52 0.0+ 0.038 s 13.16

β+m:83.00; β+,p:17.00

0

3.450E+06 3.450E+06 4.370E+05 NUBASE

0587 28-Ni- 53 3.5- 0.045 s 33.33

β+:55.00; β+,p:22.50;

β+,pm:22.50

0

3.364E+06 3.364E+06 9.302E+05 NUBASE

0588 28-Ni- 54 0.0+ 0.104 s 6.73

β+:100.00

0

2.933E+06 2.933E+06 NUBASE

0589 28-Ni- 55 3.5- 0.204 s 1.47

β+:100.00

4

3.599E+06 1.017E+06 1.294E+03 ENSDF

0590 28-Ni- 56 0.0+ 6.075 d 0.16

β+:100.00

0

7.118E+05 7.118E+05 NUBASE

0591 28-Ni- 57 1.5- 1.496 d 0.84

β+:100.00

4

1.566E+05 1.941E+06 LNHB

0592 28-Ni- 58 0.0+ 7E+20 y 100

2β+:100.00

0

1.926E+06 NUBASE

0593 28-Ni- 59 1.5- 7.6E+04 y 6.58

β+:100.00

3

4.622E+03 2.544E+03 UKPADD67

0594 28-Ni- 60 0.0+

NUBASE

0595 28-Ni- 61 1.5-

NUBASE

0596 28-Ni- 62 0.0+

NUBASE

0597 28-Ni- 63 0.5- 100.6 y 1.39

β-:100.00

1

1.742E+04 LNHB

0598 28-Ni- 64 0.0+

NUBASE

0599 28-Ni- 65 2.5- 2.52 h 0.04

β-:100.00

4

6.297E+05 5.499E+05 UKPADD67

0600 28-Ni- 66 0.0+ 2.267 d 0.92

β-:100.00

1

6.524E+04 UKPADD67

0601 28-Ni- 67 0.5- 21 s 4.76

β-:100.00

2

1.523E+06 5.025E+04 UKPADD67

0602 28-Ni- 68 0.0+ 29 s 6.90

β-:100.00

0

7.011E+05 7.011E+05 NUBASE

0603 28-Ni- 69 4.5+ 11.4 s 2.63

β-:100.00

2

1.174E+06 2.635E+06 ENSDF

0604 28-Ni- 69M 0.5- 3.210E+05 3.5 s 11.43

β-:100.00

0

2.026E+06 2.026E+06 NUBASE

0605 28-Ni- 70 0.0+ 6 s 5

β-n:100.00

0

1.194E+06 1.194E+06 NUBASE

0606 28-Ni- 71 0.5- 2.56 s 1.17

β-:100.00

0

2.504E+06 2.504E+06 NUBASE

0607 28-Ni- 72 0.0+ 1.57 s 3.18

β-:100.00

0

1.948E+06 1.948E+06 NUBASE

0608 28-Ni- 73 4.5+ 0.84 s 3.57

β-:100.00

0

3.042E+06 3.042E+06 NUBASE

0609 28-Ni- 74 0.0+ 0.68 s 17.65

β-:100.00

0

2.545E+06 2.545E+06 NUBASE

0610 28-Ni- 75 3.5+ 0.6 s 33.33

β-:98.40; β-,n:1.60

0

3.368E+06 3.368E+06 1.614E+04 NUBASE

0611 28-Ni- 76 0.0+ 0.47 s 82.98

β-:50.00; β-

m:50.00

0

3.122E+06 3.122E+06 NUBASE

0612 28-Ni- 77 4.5+ 0.3 s 100

β-:100.00

0

3.943E+06 3.943E+06 NUBASE

0613 28-Ni- 78 0.0+ 0.2 s 100

β-:100.00

0

3.483E+06 3.483E+06 NUBASE

66 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 67: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0614 29-Cu- 52 3.0+ 1E-09 s 100

p:100.00

0

1.521E+06 NUBASE

0615 29-Cu- 53 1.5- 3E-07 s 100

p:50.00; β+:50.00

0

2.652E+06 2.652E+06 9.505E+05 NUBASE

0616 29-Cu- 54 3.0+ 7.5E-08 s 100

p:100.00

0

3.910E+05 NUBASE

0617 29-Cu- 55 1.5- 0.04 s 100

β+:50.00; p:50.00

0

2.286E+06 2.286E+06 1.505E+05 NUBASE

0618 29-Cu- 56 4.0+ 0.093 s 3.23

β+:99.60; β+,p:0.40

0

5.089E+06 5.089E+06 8.139E+03 NUBASE

0619 29-Cu- 57 1.5- 0.196 s 0.36

β+:100.00

4

3.600E+06 1.140E+06 1.260E+03 ENSDF

0620 29-Cu- 58 1.0+ 3.204 s 0.22

β+:100.00

4

3.296E+06 1.541E+06 1.111E+03 ENSDF

0621 29-Cu- 59 1.5- 1.358 m 0.61

β+:100.00

4

1.488E+06 1.444E+06 ENSDF

0622 29-Cu- 60 2.0+ 23.7 m 1.69

β+:100.00

4

9.016E+05 3.912E+06 ENSDF

0623 29-Cu- 61 1.5- 3.333 h 0.15

β+:100.00

4

3.088E+05 8.235E+05 ENSDF

0624 29-Cu- 62 1.0+ 9.75 m 0.10

β+:100.00

4

1.283E+06 1.012E+06 UKPADD67

0625 29-Cu- 63 1.5-

NUBASE

0626 29-Cu- 64 1.0+ 12.701 h 0.02

β+:61.00; β-:39.00

5

1.259E+05 1.901E+05 LNHB

0627 29-Cu- 65 1.5-

NUBASE

0628 29-Cu- 66 1.0+ 5.1 m 0.20

β-:100.00

2

1.071E+06 8.186E+04 UKPADD67

0629 29-Cu- 67 1.5- 2.579 d 0.16

β-:100.00

4

1.557E+05 1.154E+05 UKPADD67

0630 29-Cu- 68 1.0+ 31.1 s 4.82

β-:100.00

4

1.481E+06 1.021E+06 ENSDF

0631 29-Cu- 68M 6.0- 7.216E+05 3.75 m 1.33

IT:84.00; β-:16.00

0

2.753E+05 8.814E+05 NUBASE

0632 29-Cu- 69 1.5- 2.85 m 5.26

β-:100.00

2

8.865E+05 5.250E+05 ENSDF

0633 29-Cu- 70 6.0- 44.5 s 0.45

β-:100.00

2

1.327E+06 3.492E+06 ENSDF

0634 29-Cu- 70M 3.0- 1.011E+05 33 s 6.06

β-:52.00; IT:48.00

0

1.160E+06 1.208E+06 NUBASE

0635 29-Cu- 70N 1.0+ 2.426E+05 6.6 s 3.03

β-:93.20; ITm:6.80

0

2.122E+06 2.132E+06 NUBASE

0636 29-Cu- 71 1.5- 19.4 s 7.22

β-:100.00

0

1.539E+06 1.539E+06 NUBASE

0637 29-Cu- 72 1.0+ 6.6 s 1.52

β-:100.00

2

3.121E+06 1.428E+06 ENSDF

0638 29-Cu- 73 1.5- 4.2 s 7.14

β-:100.00

2

3.056E+05 ENSDF

0639 29-Cu- 74 1.0+ 1.594 s 0.63

β-:100.00

0

3.235E+06 3.235E+06 NUBASE

0640 29-Cu- 75 1.5- 1.224 s 0.25

β-:96.50; β-,n:3.50

0

2.717E+06 2.717E+06 3.079E+04 NUBASE

0641 29-Cu- 76 ? 0.641 s 0.94

β-:97.00; β-,n:3.00

0

3.635E+06 3.635E+06 2.567E+04 NUBASE

0642 29-Cu- 76M ? 1.27 s 23.62

β-:100.00

0

3.721E+06 3.721E+06 NUBASE

0643 29-Cu- 77 1.5- 0.469 s 1.71

β-:100.00

0

3.380E+06 3.380E+06 NUBASE

0644 29-Cu- 78 ? 0.342 s 3.22

β-:100.00

0

4.197E+06 4.197E+06 NUBASE

0645 29-Cu- 79 1.5- 0.188 s 13.30

β-:45.00; β-,n:55.00

0

2.618E+06 2.618E+06 9.541E+05 NUBASE

0646 29-Cu- 80 ? 0.1 s 100

β-:100.00

0

5.130E+06 5.130E+06 NUBASE

0647 30-Zn- 54 0.0+ 1E-09 s 100

2p:100.00

0

1.502E+06 NUBASE

0648 30-Zn- 55 2.5- 0.02 s 100

β+:100.00

0

5.567E+06 5.567E+06 NUBASE

0649 30-Zn- 56 0.0+ 0.036 s 27.78

β+:100.00

0

4.290E+06 4.290E+06 NUBASE

0650 30-Zn- 57 3.5- 0.038 s 10.53

β+:35.00; β+,p:65.00

0

3.938E+06 3.938E+06 2.245E+06 NUBASE

0651 30-Zn- 58 0.0+ 0.084 s 10.71

β+:97.00; β+,p:3.00

0

3.076E+06 3.076E+06 4.870E+04 NUBASE

0652 30-Zn- 59 1.5- 0.182 s 0.99

β+:100.00

4

3.802E+06 1.056E+06 1.330E+03 ENSDF

0653 30-Zn- 60 0.0+ 2.38 m 2.10

β+:100.00

4

1.119E+06 1.506E+06 ENSDF

0654 30-Zn- 61 1.5- 1.485 m 0.22

β+:100.00

4

1.855E+06 1.525E+06 ENSDF

0655 30-Zn- 61M 0.5- 8.840E+04 0.43 s 100

IT:100.00

0

8.840E+04 NUBASE

0656 30-Zn- 61N 1.5- 4.181E+05 0.14 s 50

IT:100.00

0

4.181E+05 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 67

MAIN DATA TABLES

Page 68: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0657 30-Zn- 61O 2.5- 7.560E+05 0.13 s 100

IT:100.00

0

7.560E+05 NUBASE

0658 30-Zn- 62 0.0+ 9.26 h 0.22

β+:100.00

4

3.214E+04 4.432E+05 ENSDF

0659 30-Zn- 63 1.5- 38.4 m 0.26

β+:100.00

4

9.167E+05 1.104E+06 UKPADD67

0660 30-Zn- 64 0.0+ 2.3E+18 y 100

2β+:100.00

0

1.096E+06 NUBASE

0661 30-Zn- 65 2.5- 244.15 d 0.04

β+:100.00

4

6.693E+03 5.822E+05 LNHB

0662 30-Zn- 66 0.0+

NUBASE

0663 30-Zn- 67 2.5-

NUBASE

0664 30-Zn- 68 0.0+

NUBASE

0665 30-Zn- 69 0.5- 56.4 m 1.24

β-:100.00

4

3.229E+05 6.005E+00 UKPADD67

0666 30-Zn- 69M 4.5+ 4.386E+05 13.78 h 0.36

β-:0.03; IT:99.97

4

2.238E+04 4.164E+05 UKPADD67

0667 30-Zn- 70 0.0+

NUBASE

0668 30-Zn- 71 0.5- 2.45 m 4.08

β-:100.00

4

1.048E+06 3.149E+05 ENSDF

0669 30-Zn- 71M 4.5+ 1.577E+05 3.96 h 1.26

β-:100.00

4

5.370E+05 1.560E+06 ENSDF

0670 30-Zn- 72 0.0+ 1.938 d 0.22

β-:96.67; β-

m:3.33

4

1.029E+05 1.525E+05 ENSDF

0671 30-Zn- 73 0.5- 23.5 s 4.26

β-:100.00

4

1.844E+06 1.049E+05 ENSDF

0672 30-Zn- 73M 2.5+ 1.955E+05 13 s 1.54

IT:100.00

0

1.955E+05 NUBASE

0673 30-Zn- 73N 3.5+ 2.376E+05 5.8 s 13.79

ITm:50.00; β-:50.00

0

7.545E+05 7.755E+05 NUBASE

0674 30-Zn- 74 0.0+ 1.593 m 1.26

β-m:100.00

0

7.601E+05 7.601E+05 NUBASE

0675 30-Zn- 75 3.5+ 10.2 s 1.96

β-:100.00

2

1.940E+06 1.713E+06 ENSDF

0676 30-Zn- 76 0.0+ 5.7 s 5.26

β-:100.00

2

1.586E+06 5.230E+05 ENSDF

0677 30-Zn- 77 3.5+ 2.08 s 2.40

β-:100.00

0

2.424E+06 2.424E+06 NUBASE

0678 30-Zn- 77M 0.5- 7.724E+05 1.05 s 9.52

IT:50.00; β-:50.00

0

1.341E+06 1.727E+06 NUBASE

0679 30-Zn- 78 0.0+ 1.47 s 10.20

β-:100.00

0

2.122E+06 2.122E+06 NUBASE

0680 30-Zn- 79 4.5+ 0.995 s 1.91

β-:98.70; β-,n:1.30

0

2.998E+06 2.998E+06 7.200E+03 NUBASE

0681 30-Zn- 80 0.0+ 0.545 s 2.94

β-:100.00

2

2.594E+06 1.576E+06 ENSDF

0682 30-Zn- 81 2.5+ 0.29 s 17.24

β-:92.50; β-,n:7.50

0

3.746E+06 3.746E+06 9.260E+04 NUBASE

0683 30-Zn- 82 0.0+ 0.1 s 100

β-:100.00

0

3.547E+06 3.547E+06 NUBASE

0684 30-Zn- 83 2.5+ 0.08 s 100

β-:100.00

0

4.363E+06 4.363E+06 NUBASE

0685 31-Ga- 56 3.0+ 1E-09 s 100

p:100.00

0

2.891E+06 NUBASE

0686 31-Ga- 57 0.5- 1E-09 s 100

p:100.00

0

2.541E+06 NUBASE

0687 31-Ga- 58 2.0+ 1E-09 s 100

p:100.00

0

1.521E+06 NUBASE

0688 31-Ga- 59 1.5- 1E-09 s 100

p:100.00

0

8.910E+05 NUBASE

0689 31-Ga- 60 2.0+ 0.07 s 18.57

β+:100.00

4

4.600E+06 4.455E+06 2.450E+03 ENSDF

0690 31-Ga- 61 1.5- 0.168 s 1.79

β+:85.80; β+

m:9.00;

β+n:0.60; β+:4.60

0

3.070E+06 3.070E+06 NUBASE

0691 31-Ga- 62 0.0+ 0.116 s 0.26

β+:100.00

3

3.855E+06 1.021E+06 1.294E+03 ENSDF

0692 31-Ga- 63 1.5- 32.4 s 1.54

β+:100.00

4

1.890E+06 1.373E+06 ENSDF

0693 31-Ga- 64 0.0+ 2.627 m 0.46

β+:100.00

4

1.699E+06 3.352E+06 ENSDF

0694 31-Ga- 65 1.5- 15.2 m 1.32

β+:100.00

4

8.236E+05 1.168E+06 ENSDF

0695 31-Ga- 66 0.0+ 9.49 h 0.74

β+:100.00

4

9.760E+05 2.459E+06 LNHB

0696 31-Ga- 67 1.5- 3.261 d 0.02

β+:100.00

4

3.516E+04 1.596E+05 ENSDF

0697 31-Ga- 68 1.0+ 1.127 h 0.09

β+:100.00

4

7.399E+05 9.510E+05 LNHB

0698 31-Ga- 69 1.5-

NUBASE

68 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 69: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0699 31-Ga- 70 1.0+ 21.14 m 0.14

β+:0.41; β-:99.59

5

6.441E+05 7.282E+03 ENSDF

0700 31-Ga- 71 1.5-

NUBASE

0701 31-Ga- 72 3.0- 14.1 h 0.07

β-:100.00

4

5.067E+05 2.705E+06 ENSDF

0702 31-Ga- 72M 0.0+ 1.197E+05 0.04 s 0.33

IT:100.00

0

1.197E+05 NUBASE

0703 31-Ga- 73 1.5- 4.86 h 0.62

β-:1.47; β-

m:98.53

4

4.467E+05 3.410E+05 ENSDF

0704 31-Ga- 74 3.0- 8.12 m 1.48

β-:100.00

2

9.883E+05 3.006E+06 ENSDF

0705 31-Ga- 74M ? 5.957E+04 9.5 s 10.53

IT:75.00; β-:25.00

0

4.527E+05 4.973E+05 NUBASE

0706 31-Ga- 75 1.5- 2.1 m 1.59

β-:96.00; β-

m:4.00

0

1.129E+06 1.129E+06 NUBASE

0707 31-Ga- 76 ? 32.6 s 1.84

β-:100.00

2

1.801E+06 2.715E+06 ENSDF

0708 31-Ga- 77 1.5- 13 s 2.31

β-m:100.00

4

2.112E+06 4.570E+05 UKPADD67

0709 31-Ga- 78 3.0+ 5.09 s 0.98

β-:100.00

2

2.604E+06 2.500E+06 ENSDF

0710 31-Ga- 79 1.5- 2.847 s 0.11

β-:99.76; β-

m:0.15;

β-,n:0.09

0

2.325E+06 2.325E+06 2.850E+02 NUBASE

0711 31-Ga- 80 3.0+ 1.697 s 0.65

β-:100.00

2

3.456E+06 2.366E+06 1.096E+03 ENSDF

0712 31-Ga- 81 2.5- 1.217 s 0.41

β-:46.53; β-

m:41.57;

β-,n:11.90

0

2.452E+06 2.452E+06 1.030E+05 NUBASE

0713 31-Ga- 82 ? 0.599 s 0.33

β-:78.70; β-,n:10.65;

β-,nm:10.65

0

3.539E+06 3.539E+06 2.550E+05 NUBASE

0714 31-Ga- 83 1.5- 0.308 s 0.32

β-:63.00; β-,n:37.00

0

3.172E+06 3.172E+06 7.547E+05 NUBASE

0715 31-Ga- 84 ? 0.085 s 11.76

β-:30.00; β-,n:70.00

0

2.940E+06 2.940E+06 1.526E+06 NUBASE

0716 31-Ga- 85 1.5- 0.05 s 100

β-:100.00

0

4.340E+06 4.340E+06 NUBASE

0717 31-Ga- 86 ? 0.03 s 100

β-:100.00

0

5.163E+06 5.163E+06 NUBASE

0718 32-Ge- 58 0.0+ 1E-09 s 100

2p:100.00

0

2.782E+06 NUBASE

0719 32-Ge- 59 3.5- 1E-09 s 100

2p:100.00

0

1.222E+06 NUBASE

0720 32-Ge- 60 0.0+ 0.03 s 100

β+:100.00

0

4.077E+06 4.077E+06 NUBASE

0721 32-Ge- 61 1.5- 0.039 s 30.77

β+:20.00; β+,p:80.00

0

3.524E+06 3.524E+06 2.634E+06 NUBASE

0722 32-Ge- 62 0.0+ 0.13 s 30.77

β+:100.00

0

3.253E+06 3.253E+06 NUBASE

0723 32-Ge- 63 1.5- 0.142 s 5.63

β+:100.00

0

3.212E+06 3.212E+06 NUBASE

0724 32-Ge- 64 0.0+ 1.062 m 3.92

β+:100.00

0

1.495E+06 1.495E+06 NUBASE

0725 32-Ge- 65 1.5- 30.9 s 1.62

β+:99.99; β+,p:0.01

0

2.082E+06 2.082E+06 6.338E+01 NUBASE

0726 32-Ge- 66 0.0+ 2.26 h 2.21

β+:100.00

4

9.714E+04 6.745E+05 ENSDF

0727 32-Ge- 67 0.5- 18.9 m 1.59

β+:100.00

0

1.407E+06 1.407E+06 NUBASE

0728 32-Ge- 68 0.0- 270.95 d 0.06

β+:100.00

3

4.746E+03 4.143E+03 LNHB

0729 32-Ge- 69 2.5- 1.627 d 0.26

β+:100.00

4

1.200E+05 9.505E+05 ENSDF

0730 32-Ge- 70 0.0+

NUBASE

0731 32-Ge- 71 0.5- 11.43 d 0.26

β+:100.00

3

4.792E+03 4.195E+03 ENSDF

0732 32-Ge- 71M 4.5+ 1.984E+05 0.02 s 0.83

IT:100.00

3

3.292E+04 1.646E+05 ENSDF

0733 32-Ge- 72 0.0+

NUBASE

0734 32-Ge- 73 4.5+

NUBASE

0735 32-Ge- 73M 0.5- 6.673E+04 0.5 s 2

IT:100.00

3

5.561E+04 1.135E+04 UKPADD67

0736 32-Ge- 74 0.0+

NUBASE

0737 32-Ge- 75 0.5- 1.38 h 0.05

β-:100.00

2

4.204E+05 3.523E+04 ENSDF

0738 32-Ge- 75M 3.5+ 1.397E+05 47.7 s 1.05

IT:99.97; β-

m:0.03

0

1.012E+02 1.397E+05 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 69

MAIN DATA TABLES

Page 70: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0739 32-Ge- 76 0.0+ 1.58E+21 y 10.76

2β-:100.00

0

2.039E+06 NUBASE

0740 32-Ge- 77 3.5+ 11.3 h 0.09

β-:100.00

2

6.422E+05 1.078E+06 ENSDF

0741 32-Ge- 77M 0.5- 1.597E+05 52.9 s 1.13

β-:81.00; IT:19.00

4

9.660E+05 7.401E+04 ENSDF

0742 32-Ge- 78 0.0+ 1.467 h 1.14

β-:100.00

2

2.267E+05 2.781E+05 ENSDF

0743 32-Ge- 79 0.5- 18.98 s 0.16

β-:100.00

4

1.714E+06 2.597E+05 ENSDF

0744 32-Ge- 79M 3.5+ 1.860E+05 39 s 2.56

β-:96.00; IT:4.00

4

1.292E+06 1.196E+06 ENSDF

0745 32-Ge- 80 0.0+ 29.5 s 1.36

β-:100.00

2

1.050E+06 1.466E+05 ENSDF

0746 32-Ge- 81 4.5+ 8 s 25

β-:100.00

0

2.078E+06 2.078E+06 NUBASE

0747 32-Ge- 81M 0.5+ 6.791E+05 7.6 s 7.89

β-:100.00; IT:1.00

4

2.475E+06 1.495E+06 ENSDF

0748 32-Ge- 82 0.0+ 4.55 s 6.59

β-:100.00

2

1.575E+06 1.079E+06 ENSDF

0749 32-Ge- 83 2.5+ 1.85 s 3.24

β-:100.00

0

2.993E+06 2.993E+06 NUBASE

0750 32-Ge- 84 0.0+ 0.954 s 1.47

β-:44.60; β-

m:44.60;

β-,n:10.80

0

2.424E+06 2.424E+06 9.608E+04 NUBASE

0751 32-Ge- 85 2.5+ 0.54 s 9.26

β-:86.00; β-,n:7.00;

β-,nm:7.00

0

3.111E+06 3.111E+06 1.729E+05 NUBASE

0752 32-Ge- 86 0.0+ 0.3 s 100

β-:100.00

0

3.103E+06 3.103E+06 NUBASE

0753 32-Ge- 87 2.5+ 0.15 s 100

β-:100.00

0

3.913E+06 3.913E+06 NUBASE

0754 32-Ge- 88 0.0+ 0.08 s 100

β-:100.00

0

3.717E+06 3.717E+06 NUBASE

0755 32-Ge- 89 1.5+ 0.05 s 100

β-:100.00

0

4.483E+06 4.483E+06 NUBASE

0756 33-As- 60 5.0+ 1E-09 s 100

p:100.00

0

3.311E+06 NUBASE

0757 33-As- 60M 2.0+ 6.000E+04 1E-09 s 100

p:100.00

0

3.371E+06 NUBASE

0758 33-As- 61 1.5- 1E-09 s 100

p:100.00

0

2.431E+06 NUBASE

0759 33-As- 62 1.0+ 1E-09 s 100

p:100.00

0

1.481E+06 NUBASE

0760 33-As- 63 1.5- 1E-09 s 100

p:100.00

0

1.131E+06 NUBASE

0761 33-As- 64 0.0+ 0.04 s 75

β+:100.00

0

4.943E+06 4.943E+06 NUBASE

0762 33-As- 65 1.5- 0.17 s 17.65

β+:100.00

0

3.143E+06 3.143E+06 NUBASE

0763 33-As- 66 0.0+ 0.096 s 0.24

β+:100.00

0

3.373E+06 3.373E+06 NUBASE

0764 33-As- 67 2.5- 42.5 s 2.82

β+:100.00

4

2.068E+06 1.464E+06 ENSDF

0765 33-As- 68 3.0+ 2.527 m 0.53

β+:100.00

4

2.021E+06 3.693E+06 ENSDF

0766 33-As- 69 2.5- 15.23 m 1.05

β+:100.00

4

1.219E+06 1.135E+06 ENSDF

0767 33-As- 70 4.0+ 52.6 m 0.57

β+:100.00

4

8.407E+05 3.997E+06 ENSDF

0768 33-As- 71 2.5- 2.72 d 0.23

β+:100.00

4

1.158E+05 5.751E+05 ENSDF

0769 33-As- 72 2.0- 1.083 d 0.38

β+:100.00

4

1.040E+06 1.781E+06 ENSDF

0770 33-As- 73 1.5- 80.3 d 0.07

β+m:100.00

3

5.232E+03 4.763E+03 UKPADD67

0771 33-As- 74 2.0- 17.78 d 0.17

β-:34.00; β+:66.00

5

2.683E+05 7.597E+05 UKPADD67

0772 33-As- 75 1.5-

NUBASE

0773 33-As- 75M 4.5+ 3.039E+05 0.018 s 1.31

IT:100.00

0

3.039E+05 NUBASE

0774 33-As- 76 2.0- 1.093 d 0.31

β-:100.00

4

1.064E+06 4.198E+05 UKPADD67

0775 33-As- 77 1.5- 1.618 d 0.13

β-:100.00

2

2.255E+05 8.313E+03 ENSDF

0776 33-As- 78 2.0- 1.512 h 0.22

β-:100.00

2

1.256E+06 1.300E+06 ENSDF

0777 33-As- 79 1.5- 9.01 m 1.66

β-:2.37; β-

m:97.63

2

8.392E+05 3.378E+04 ENSDF

0778 33-As- 80 1.0+ 15.2 s 1.32

β-:100.00

2

2.148E+06 5.821E+05 ENSDF

0779 33-As- 81 1.5- 33.3 s 2.40

β-:96.41; β-

m:3.59

4

1.575E+06 2.303E+05 ENSDF

70 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 71: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0780 33-As- 82 1.0+ 19.1 s 2.62

β-:100.00

2

3.197E+06 3.078E+05 ENSDF

0781 33-As- 82M 5.0- 2.450E+05 13.6 s 2.21

β-:100.00

4

2.037E+06 2.970E+06 UKPADD67

0782 33-As- 83 1.5- 13.4 s 2.24

β-:36.00; β-

m:64.00

0

1.772E+06 1.772E+06 NUBASE

0783 33-As- 84 3.0+ 4.02 s 0.75

β-:99.72; β-,n:0.14;

β-,nm:0.14

0

3.282E+06 3.282E+06 7.528E+02 NUBASE

0784 33-As- 84M ? 0.65 s 23.08

β-:100.00

0

3.291E+06 3.291E+06 NUBASE

0785 33-As- 85 1.5- 2.04 s 0.98

β-:78.00; β-,n:22.00

5

3.381E+06 3.585E+05 1.518E+05 UKPADD67

0786 33-As- 86 ? 0.945 s 0.85

β-:67.00; β-,n:33.00

0

2.974E+06 2.974E+06 4.296E+05 NUBASE

0787 33-As- 87 1.5- 0.61 s 18.03

β-:84.60; β-,n:15.40

0

3.239E+06 3.239E+06 2.499E+05 NUBASE

0788 33-As- 88 ? 0.3 s 100

β-:100.00

0

4.197E+06 4.197E+06 NUBASE

0789 33-As- 89 1.5- 0.2 s 100

β-:100.00

0

4.020E+06 4.020E+06 NUBASE

0790 33-As- 90 ? 0.08 s 100

β-:100.00

0

4.827E+06 4.827E+06 NUBASE

0791 33-As- 91 1.5- 0.05 s 100

β-:100.00

0

4.493E+06 4.493E+06 NUBASE

0792 33-As- 92 ? 0.03 s 100

β-:100.00

0

5.240E+06 5.240E+06 NUBASE

0793 34-Se- 65 1.5- 0.05 s 100

β+:100.00

0

4.687E+06 4.687E+06 NUBASE

0794 34-Se- 66 0.0+ 0.033 s 36.36

β+:100.00

0

3.260E+06 3.260E+06 NUBASE

0795 34-Se- 67 2.5- 0.133 s 8.27

β+:99.50; β+,p:0.50

0

3.380E+06 3.380E+06 9.801E+03 NUBASE

0796 34-Se- 68 0.0+ 35.5 s 1.97

β+:100.00

0

1.563E+06 1.563E+06 NUBASE

0797 34-Se- 69 1.5- 27.4 s 0.73

β+:100.00

4

2.304E+06 1.865E+06 ENSDF

0798 34-Se- 70 0.0+ 41.1 m 0.73

β+:100.00

4

4.842E+05 9.928E+05 ENSDF

0799 34-Se- 71 2.5- 4.74 m 1.05

β+:100.00

4

1.397E+06 1.584E+06 ENSDF

0800 34-Se- 72 0.0+ 8.4 d 0.95

β+:100.00

4

2.246E+04 3.434E+04 ENSDF

0801 34-Se- 73 4.5+ 7.15 h 1.12

β+:100.00

4

3.865E+05 1.090E+06 ENSDF

0802 34-Se- 73M 1.5- 2.571E+04 39.8 m 3.27

IT:72.60; β+:27.40

0

2.525E+05 2.712E+05 NUBASE

0803 34-Se- 74 0.0+

NUBASE

0804 34-Se- 75 2.5+ 119.64 d 0.20

β+:100.00

4

1.465E+04 3.902E+05 UKPADD67

0805 34-Se- 76 0.0+

NUBASE

0806 34-Se- 77 0.5-

NUBASE

0807 34-Se- 77M 3.5+ 1.619E+05 17.55 s 0.85

IT:100.00

3

7.328E+04 8.881E+04 UKPADD67

0808 34-Se- 78 0.0+

NUBASE

0809 34-Se- 79 3.5+ 3.77E+05 y 5.04

β-:100.00

1

5.259E+04 UKPADD67

0810 34-Se- 79M 0.5- 9.577E+04 3.9 m 0.51

IT:99.94; β-:0.06

4

8.187E+04 1.396E+04 UKPADD67

0811 34-Se- 80 0.0+

NUBASE

0812 34-Se- 81 0.5- 18.39 m 0.71

β-:100.00

4

6.091E+05 8.546E+03 UKPADD67

0813 34-Se- 81M 3.5+ 1.030E+05 57.28 m 0.03

β-:0.07; IT:99.93

4

8.540E+04 1.803E+04 UKPADD67

0814 34-Se- 82 0.0+ 1.21E+20 y 14.05

2β-:100.00

0

2.995E+06 ENSDF

0815 34-Se- 83 4.5+ 22.3 m 1.35

β-:100.00

0

1.223E+06 1.223E+06 NUBASE

0816 34-Se- 83M 0.5- 2.287E+05 1.168 m 0.57

β-:100.00

2

1.273E+06 9.715E+05 ENSDF

0817 34-Se- 84 0.0+ 3.1 m 3.23

β-:100.00; β-

m:~

2

5.404E+05 4.082E+05 ENSDF

0818 34-Se- 85 2.5+ 31.7 s 2.84

β-:100.00

0

2.061E+06 2.061E+06 NUBASE

0819 34-Se- 86 0.0+ 15.3 s 5.88

β-:100.00

0

1.700E+06 1.700E+06 NUBASE

0820 34-Se- 87 2.5+ 5.5 s 2.18

β-:100.00

2

2.962E+06 6.619E+05 ENSDF

0821 34-Se- 88 0.0+ 1.53 s 3.92

β-:99.01; β-,n:0.99

0

2.265E+06 2.265E+06 4.717E+03 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 71

MAIN DATA TABLES

Page 72: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0822 34-Se- 89 2.5+ 0.41 s 9.76

β-:92.20; β-,n:7.80

0

2.947E+06 2.947E+06 6.744E+04 NUBASE

0823 34-Se- 90 0.0+ 0.3 s 100

β-:100.00

0

2.897E+06 2.897E+06 NUBASE

0824 34-Se- 91 0.5+ 0.27 s 18.52

β-:79.00; β-,n:21.00

0

3.267E+06 3.267E+06 3.260E+05 NUBASE

0825 34-Se- 92 0.0+ 0.1 s 100

β-:100.00

0

3.310E+06 3.310E+06 NUBASE

0826 34-Se- 93 0.5+ 0.05 s 100

β-:100.00

0

4.110E+06 4.110E+06 NUBASE

0827 34-Se- 94 0.0+ 0.02 s 100

β-:100.00

0

3.667E+06 3.667E+06 NUBASE

0828 35-Br- 67 0.5- 1E-09 s 100

p:100.00

0

1.631E+06 NUBASE

0829 35-Br- 68 3.0+ 1.5E-06 s 100

p:100.00

0

5.610E+05 NUBASE

0830 35-Br- 69 0.5- 2.4E-08 s 100

p:100.00

0

4.410E+05 NUBASE

0831 35-Br- 70 0.0+ 0.079 s 1.01

β+:100.00

0

3.540E+06 3.540E+06 NUBASE

0832 35-Br- 70M 9.0+ 2.292E+06 2.2 s 9.09

β+:50.00; IT:50.00

0

2.152E+06 3.298E+06 NUBASE

0833 35-Br- 71 2.5- 21.4 s 2.80

β+:100.00

0

2.020E+06 2.020E+06 NUBASE

0834 35-Br- 72 1.0+ 1.31 m 3.05

β+:100.00

4

2.717E+06 2.922E+06 UKPADD67

0835 35-Br- 72M 1.0- 1.011E+05 10.6 s 3.77

IT:100.00

3

5.088E+04 5.000E+04 UKPADD67

0836 35-Br- 73 0.5- 3.4 m 5.88

β+m:100.00

0

1.521E+06 1.521E+06 NUBASE

0837 35-Br- 74 0.0- 25.4 m 1.18

β+:100.00

4

1.055E+06 4.357E+06 ENSDF

0838 35-Br- 74M 4.0+ 1.380E+04 46 m 4.35

β+:100.00

4

1.243E+06 3.795E+06 ENSDF

0839 35-Br- 75 1.5- 1.612 h 1.34

β+:100.00

4

5.283E+05 1.194E+06 ENSDF

0840 35-Br- 76 1.0- 16.2 h 1.23

β+:100.00

4

6.481E+05 2.716E+06 ENSDF

0841 35-Br- 76M 4.0+ 1.026E+05 1.31 s 1.53

IT:99.40; β+:0.60

0

1.013E+04 1.121E+05 NUBASE

0842 35-Br- 77 1.5- 2.377 d 0.01

β+:100.00

4

6.034E+03 3.208E+05 ENSDF

0843 35-Br- 77M 4.5+ 1.059E+05 4.28 m 2.34

IT:100.00

3

8.479E+04 1.957E+04 ENSDF

0844 35-Br- 78 1.0+ 6.46 m 0.62

β+:100.00

4

1.024E+06 1.034E+06 ENSDF

0845 35-Br- 79 1.5-

NUBASE

0846 35-Br- 79M 4.5+ 2.072E+05 4.864 s 0.72

IT:100.00

3

4.701E+04 1.598E+05 ENSDF

0847 35-Br- 80 1.0+ 17.6 m 0.28

β-:91.70; β+:8.30

5

7.240E+05 7.700E+04 UKPADD67

0848 35-Br- 80M 5.0- 8.585E+04 4.41 h 0.23

IT:100.00

3

6.176E+04 2.426E+04 UKPADD67

0849 35-Br- 81 1.5-

NUBASE

0850 35-Br- 82 5.0- 1.472 d 0.08

β-:100.00

4

1.427E+05 2.638E+06 UKPADD67

0851 35-Br- 82M 2.0- 4.595E+04 6.09 m 1.15

β-:2.40; IT:97.60

4

7.009E+04 8.181E+03 UKPADD67

0852 35-Br- 83 1.5- 2.4 h 0.83

β-:0.09; β-

m:99.91

2

3.252E+05 6.874E+03 ENSDF

0853 35-Br- 84 2.0- 31.8 m 0.25

β-:100.00

2

1.240E+06 1.757E+06 ENSDF

0854 35-Br- 84M ? 3.200E+05 6 m 3.33

β-:100.00

2

9.100E+05 2.768E+06 ENSDF

0855 35-Br- 85 1.5- 2.9 m 2.07

β-:0.16; β-

m:99.84

2

1.041E+06 6.131E+04 ENSDF

0856 35-Br- 86 2.0- 55 s 1.45

β-:100.00

2

1.943E+06 3.297E+06 ENSDF

0857 35-Br- 87 1.5- 55.7 s 0.36

β-:97.49; β-,n:2.51

5

1.577E+06 3.089E+06 3.783E+03 UKPADD67

0858 35-Br- 88 2.0- 16.5 s 0.61

β-:93.30; β-,n:6.70

5

2.394E+06 3.112E+06 8.068E+03 UKPADD67

0859 35-Br- 89 1.5- 4.37 s 1.14

β-:85.90; β-,n:14.10

5

2.572E+06 1.711E+06 6.484E+03 UKPADD67

0860 35-Br- 90 1.0- 1.9 s 2.11

β-:75.40; β-,n:24.60

5

3.290E+06 1.538E+06 2.191E+04 UKPADD67

0861 35-Br- 91 1.5- 0.538 s 2.42

β-:80.00; β-,n:20.00

5

3.909E+06 4.512E+05 1.000E+04 UKPADD67

0862 35-Br- 92 2.0- 0.343 s 4.37

β-:66.90; β-,n:33.10

0

3.273E+06 3.273E+06 5.510E+05 NUBASE

0863 35-Br- 93 1.5- 0.102 s 9.80

β-:32.00; β-,n:68.00

0

2.473E+06 2.473E+06 1.303E+06 NUBASE

0864 35-Br- 94 ? 0.07 s 28.57

β-:30.00; β-,n:70.00

0

2.760E+06 2.760E+06 1.426E+06 NUBASE

72 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 73: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0865 35-Br- 95 1.5- 0.05 s 100

β-:100.00

0

4.047E+06 4.047E+06 NUBASE

0866 35-Br- 96 ? 0.02 s 100

β-:100.00

0

4.800E+06 4.800E+06 NUBASE

0867 35-Br- 97 1.5- 0.01 s 100

β-:100.00

0

4.423E+06 4.423E+06 NUBASE

0868 36-Kr- 69 2.5- 0.032 s 31.25

β+:100.00

0

4.680E+06 4.680E+06 NUBASE

0869 36-Kr- 70 0.0+ 0.052 s 32.69

β+m:100.00

0

2.486E+06 2.486E+06 NUBASE

0870 36-Kr- 71 2.5- 0.064 s 12.50

β+:100.00

2

4.314E+06 1.022E+06 1.393E+03 ENSDF

0871 36-Kr- 72 0.0+ 17.16 s 1.05

β+m:100.00

0

1.659E+06 1.659E+06 NUBASE

0872 36-Kr- 73 1.5- 27.3 s 3.66

β+:100.00

4

2.619E+06 1.478E+06 ENSDF

0873 36-Kr- 74 0.0+ 11.5 m 0.96

β+:100.00

0

9.915E+05 9.915E+05 NUBASE

0874 36-Kr- 75 2.5+ 4.29 m 3.96

β+:100.00

4

1.575E+06 1.281E+06 ENSDF

0875 36-Kr- 76 0.0+ 14.8 h 0.68

β+:100.00

0

4.250E+05 4.250E+05 NUBASE

0876 36-Kr- 77 2.5+ 1.24 h 0.81

β+:100.00

4

6.786E+05 1.038E+06 ENSDF

0877 36-Kr- 78 0.0+ 1.1E+20 y 100

2β+:100.00

0

2.846E+06 NUBASE

0878 36-Kr- 79 0.5- 1.46 d 0.29

β+:100.00

4

2.463E+04 2.578E+05 UKPADD67

0879 36-Kr- 79M 3.5+ 1.298E+05 50 s 6

IT:100.00

3

9.006E+04 3.980E+04 UKPADD67

0880 36-Kr- 80 0.0+

NUBASE

0881 36-Kr- 81 3.5+ 2.1E+05 y 4.76

β+:100.00

4

5.385E+03 7.369E+03 UKPADD67

0882 36-Kr- 81M 0.5- 1.905E+05 13.2 s 0.76

β+:~; IT:100.00

4

5.877E+04 1.317E+05 UKPADD67

0883 36-Kr- 82 0.0+

NUBASE

0884 36-Kr- 83 4.5+

NUBASE

0885 36-Kr- 83M 0.5- 4.154E+04 1.83 h 1.09

IT:100.00

3

3.910E+04 2.767E+03 ENSDF

0886 36-Kr- 84 0.0+

NUBASE

0887 36-Kr- 85 4.5+ 10.752 y 0.21

β-:100.00

4

2.281E+05 2.236E+03 LNHB

0888 36-Kr- 85M 0.5- 3.049E+05 4.48 h 0.18

β-:78.60; IT:21.40

4

2.542E+05 1.574E+05 ENSDF

0889 36-Kr- 86 0.0+

NUBASE

0890 36-Kr- 87 2.5+ 1.272 h 0.66

β-:100.00

4

1.331E+06 7.879E+05 ENSDF

0891 36-Kr- 88 0.0+ 2.84 h 1.06

β-:100.00

4

3.714E+05 1.950E+06 ENSDF

0892 36-Kr- 89 1.5+ 3.15 m 1.27

β-:100.00

2

1.377E+06 1.836E+06 ENSDF

0893 36-Kr- 90 0.0+ 32.32 s 0.28

β-:86.92; β-

m:13.08

0

1.459E+06 1.459E+06 NUBASE

0894 36-Kr- 91 2.5+ 8.57 s 0.47

β-:100.00

4

2.096E+06 1.733E+06 ENSDF

0895 36-Kr- 92 0.0+ 1.84 s 0.43

β-:100.00

4

1.998E+06 1.388E+06 ENSDF

0896 36-Kr- 93 0.5+ 1.286 s 0.78

β-:100.00

4

2.876E+06 2.131E+06 ENSDF

0897 36-Kr- 94 0.0+ 0.21 s 1.90

β-:98.89; β-,n:1.11

0

2.453E+06 2.453E+06 9.454E+03 NUBASE

0898 36-Kr- 95 0.5+ 0.114 s 2.63

β-:97.13; β-,n:2.87

0

3.209E+06 3.209E+06 3.187E+04 NUBASE

0899 36-Kr- 96 0.0+ 0.08 s 8.75

β-:48.15; β-

m:48.15;

β-,n:3.70

0

2.675E+06 2.675E+06 4.396E+04 NUBASE

0900 36-Kr- 97 1.5+ 0.063 s 6.35

β-:93.30; β-,n:3.35;

β-,nm:3.35

0

3.334E+06 3.334E+06 8.766E+04 NUBASE

0901 36-Kr- 98 0.0+ 0.046 s 17.39

β-m:93.00; β-,n:7.00

0

2.895E+06 2.895E+06 9.605E+04 NUBASE

0902 36-Kr- 99 1.5+ 0.04 s 27.50

β-:89.00; β-,n:5.50;

β-,nm:5.50

0

3.554E+06 3.554E+06 1.775E+05 NUBASE

0903 36-Kr-100 0.0+ 0.01 s 100

β-:100.00

0

3.500E+06 3.500E+06 NUBASE

0904 37-Rb- 71 2.5- 1E-09 s 100

p:100.00

0

2.091E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 73

MAIN DATA TABLES

Page 74: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0905 37-Rb- 72 3.0+ 1.5E-06 s 100

p:100.00

0

1.511E+06 NUBASE

0906 37-Rb- 73 1.5- 3E-08 s 100

p:100.00

0

6.020E+05 NUBASE

0907 37-Rb- 74 0.0+ 0.065 s 0.77

β+:100.00

3

4.473E+06 1.020E+06 1.421E+03 ENSDF

0908 37-Rb- 75 1.5- 19 s 6.32

β+:100.00

0

2.367E+06 2.367E+06 NUBASE

0909 37-Rb- 76 1.0- 36.5 s 1.64

β+:100.00

4

2.355E+06 3.330E+06 ENSDF

0910 37-Rb- 77 1.5- 3.77 m 1.06

β+:100.00

4

1.687E+06 1.516E+06 ENSDF

0911 37-Rb- 78 0.0+ 17.66 m 0.45

β+:100.00

4

1.216E+06 4.059E+06 ENSDF

0912 37-Rb- 78M 4.0- 1.033E+05 5.74 m 0.87

β+:90.00; IT:10.00

4

1.449E+06 3.212E+06 ENSDF

0913 37-Rb- 79 2.5+ 22.9 m 2.18

β+:100.00

4

8.071E+05 1.402E+06 ENSDF

0914 37-Rb- 80 1.0+ 34 s 11.76

β+:100.00

4

2.034E+06 1.184E+06 ENSDF

0915 37-Rb- 81 1.5- 4.576 h 0.11

β+:4.52; β+

m:95.48

0

6.857E+05 6.857E+05 NUBASE

0916 37-Rb- 81M 4.5+ 8.620E+04 30.25 m 0.83

IT:96.20; β+:3.77;

β+m:0.03

4

7.395E+04 2.835E+04 LNHB

0917 37-Rb- 82 1.0+ 1.273 m 0.16

β+:100.00

4

1.412E+06 1.108E+06 ENSDF

0918 37-Rb- 82M 5.0- 6.890E+04 6.472 h 0.09

β+:100.00

4

7.956E+04 2.904E+06 ENSDF

0919 37-Rb- 83 2.5- 86.2 d 0.12

β+:25.00; β+

m:75.00

4

8.636E+03 4.961E+05 UKPADD67

0920 37-Rb- 83M 4.5+ 4.211E+04 7.8E-03 s 8.97

IT:100.00

0

4.211E+04 NUBASE

0921 37-Rb- 84 2.0- 33.5 d 1.79

β-:3.20; β+:96.80

5

1.440E+05 8.872E+05 UKPADD67

0922 37-Rb- 84M 6.0- 4.636E+05 20.4 m 0.49

IT:100.00

3

8.018E+04 3.829E+05 UKPADD67

0923 37-Rb- 85 2.5-

NUBASE

0924 37-Rb- 86 2.0- 18.64 d 0.11

β+:0.01; β-:100.00

5

6.562E+05 9.378E+04 LNHB

0925 37-Rb- 86M 6.0- 5.560E+05 1.017 m 0.33

IT:100.00

3

9.960E+03 5.460E+05 UKPADD67

0926 37-Rb- 87 1.5- 4.81E+10 y 1.87

β-:100.00

1

8.170E+04 ENSDF

0927 37-Rb- 88 2.0- 17.8 m 0.56

β-:100.00

4

2.057E+06 6.672E+05 LNHB

0928 37-Rb- 89 1.5- 15.4 m 1.30

β-:100.00

4

9.292E+05 2.234E+06 UKPADD67

0929 37-Rb- 90 0.0- 2.633 m 3.16

β-:100.00

2

1.916E+06 2.271E+06 ENSDF

0930 37-Rb- 90M 3.0- 1.069E+05 4.3 m 1.55

β-:97.40; IT:2.60

4

1.118E+06 3.869E+06 ENSDF

0931 37-Rb- 91 1.5- 58.4 s 0.68

β-:100.00

4

1.368E+06 2.706E+06 ENSDF

0932 37-Rb- 92 0.0- 4.492 s 0.45

β-:100.00

2

2.875E+06 1.750E+06 ENSDF

0933 37-Rb- 93 2.5- 5.8 s 0.69

β-:98.60; β-,n:1.40

5

2.118E+06 2.602E+06 4.149E+03 UKPADD67

0934 37-Rb- 94 3.0- 2.702 s 0.26

β-:89.90; β-,n:10.10

5

3.102E+06 2.747E+06 1.005E+04 UKPADD67

0935 37-Rb- 95 2.5- 0.381 s 0.79

β-:91.40; β-,n:8.60

5

2.829E+06 2.642E+06 7.846E+03 UKPADD67

0936 37-Rb- 96 2.0+ 0.199 s 1.51

β-:86.60; β-,n:13.40

4

3.849E+06 2.089E+06 1.093E+03 ENSDF

0937 37-Rb- 96M 1.0- 0.2 s 100

β-:50.00; IT:50.00

0

1.952E+06 1.952E+06 NUBASE

0938 37-Rb- 97 1.5+ 0.17 s 0.41

β-:74.90; β-,n:25.10

4

3.775E+06 1.332E+06 ENSDF

0939 37-Rb- 98 ? 0.114 s 4.39

β-:86.15; β-,n:13.80;

β-,2n:0.05

0

3.793E+06 3.793E+06 2.245E+05 NUBASE

0940 37-Rb- 98M ? 3.900E+05 0.096 s 3.12

β-:100.00

0

4.272E+06 4.272E+06 NUBASE

0941 37-Rb- 99 2.5+ 0.05 s 1.39

β-:84.10; β-,n:15.90

0

3.476E+06 3.476E+06 3.059E+05 NUBASE

0942 37-Rb-100 3.0+ 0.051 s 15.69

β-:94.25; β-,n:5.60;

β-,2n:0.15

0

4.353E+06 4.353E+06 1.053E+05 NUBASE

0943 37-Rb-101 1.5+ 0.032 s 12.50

β-:100.00

4

5.106E+06 4.263E+05 1.410E+03 ENSDF

0944 37-Rb-102 ? 0.037 s 13.51

β-:82.00; β-,n:18.00

0

4.443E+06 4.443E+06 4.063E+05 NUBASE

74 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 75: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0945 38-Sr- 73 0.5- 0.025 s 100

β+:100.00

0

4.783E+06 4.783E+06 NUBASE

0946 38-Sr- 74 0.0+ 0.05 s 100

β+:100.00

0

3.739E+06 3.739E+06 NUBASE

0947 38-Sr- 75 1.5- 0.088 s 3.41

β+:94.80; β+,p:5.20

0

3.460E+06 3.460E+06 1.095E+05 NUBASE

0948 38-Sr- 76 0.0+ 8.9 s 3.37

β+:100.00

0

2.080E+06 2.080E+06 NUBASE

0949 38-Sr- 77 2.5+ 9 s 2.22

β+:100.00

4

2.612E+06 1.211E+06 ENSDF

0950 38-Sr- 78 0.0+ 2.65 m 5.03

β+:100.00

0

1.254E+06 1.254E+06 NUBASE

0951 38-Sr- 79 1.5- 2.25 m 4.44

β+:100.00

0

1.775E+06 1.775E+06 NUBASE

0952 38-Sr- 80 0.0+ 1.772 h 1.41

β+:100.00

4

6.339E+04 4.864E+05 ENSDF

0953 38-Sr- 81 0.5- 22.3 m 1.79

β+:99.90; β+

m:0.10

0

1.309E+06 1.309E+06 NUBASE

0954 38-Sr- 82 0.0+ 25.55 d 0.59

β+:100.00

3

5.041E+03 7.855E+03 ENSDF

0955 38-Sr- 83 3.5+ 1.35 d 0.09

β+:100.00

4

1.490E+05 7.762E+05 UKPADD67

0956 38-Sr- 83M 0.5- 2.592E+05 4.95 s 2.42

IT:100.00

3

3.117E+04 2.281E+05 UKPADD67

0957 38-Sr- 84 0.0+

NUBASE

0958 38-Sr- 85 4.5+ 64.849 d 0.01

β+:100.00

4

8.725E+03 5.187E+05 LNHB

0959 38-Sr- 85M 0.5- 2.387E+05 1.127 h 0.07

β+:13.40; IT:86.60

4

1.325E+04 2.159E+05 UKPADD67

0960 38-Sr- 86 0.0+

NUBASE

0961 38-Sr- 87 4.5+

NUBASE

0962 38-Sr- 87M 0.5- 3.885E+05 2.816 h 0.39

β+:0.30; IT:99.70

4

6.656E+04 3.209E+05 UKPADD67

0963 38-Sr- 88 0.0+

NUBASE

0964 38-Sr- 89 2.5+ 50.57 d 0.06

β-:99.99; β-

m:0.01

4

5.846E+05 8.691E+01 LNHB

0965 38-Sr- 90 0.0+ 28.79 y 0.21

β-:100.00

1

1.740E+05 LNHB

0966 38-Sr- 91 2.5+ 9.63 h 0.52

β-:41.16; β-

m:58.84

4

6.475E+05 7.072E+05 ENSDF

0967 38-Sr- 92 0.0+ 2.71 h 0.37

β-:100.00

4

1.799E+05 1.381E+06 UKPADD67

0968 38-Sr- 93 2.5+ 7.423 m 0.32

β-:74.98; β-

m:25.02

4

7.946E+05 2.218E+06 ENSDF

0969 38-Sr- 94 0.0+ 1.255 m 0.53

β-:100.00

4

8.332E+05 1.427E+06 UKPADD67

0970 38-Sr- 95 0.5+ 23.9 s 0.59

β-:100.00

4

1.901E+06 1.790E+06 ENSDF

0971 38-Sr- 96 0.0+ 1.06 s 2.83

β-:100.00

4

1.972E+06 9.249E+05 ENSDF

0972 38-Sr- 97 0.5+ 0.429 s 1.17

β-:85.08; β-

m:14.87;

β-,n:0.03; β-,nm:0.03

0

2.456E+06 2.456E+06 1.147E+02 NUBASE

0973 38-Sr- 98 0.0+ 0.653 s 0.31

β-:100.00

4

2.363E+06 5.774E+05 ENSDF

0974 38-Sr- 99 1.5+ 0.27 s 3.70

β-:100.00

4

3.200E+06 1.268E+06 ENSDF

0975 38-Sr-100 0.0+ 0.202 s 1.49

β-:99.22; β-,n:0.78

0

2.342E+06 2.342E+06 3.724E+03 NUBASE

0976 38-Sr-101 2.5- 0.118 s 2.54

β-:97.63; β-,n:1.19;

β-,nm:1.19

0

3.114E+06 3.114E+06 2.197E+04 NUBASE

0977 38-Sr-102 0.0+ 0.069 s 8.70

β-:47.25; β-

m:47.25;

β-,n:5.50

0

2.795E+06 2.795E+06 5.168E+04 NUBASE

0978 38-Sr-103 ? 0.05 s 100

β-:100.00

0

3.797E+06 3.797E+06 NUBASE

0979 38-Sr-104 0.0+ 0.03 s 100

β-:100.00

0

3.503E+06 3.503E+06 NUBASE

0980 38-Sr-105 ? 0.02 s 100

β-:100.00

0

4.257E+06 4.257E+06 NUBASE

0981 39-Y - 76 ? 5E-07 s 100

β+:50.00; p:50.00

0

2.590E+06 2.590E+06 3.155E+05 NUBASE

0982 39-Y - 77 2.5+ 0.063 s 26.98

β+:90.00; p:10.00

0

3.268E+06 3.268E+06 4.100E+03 NUBASE

0983 39-Y - 78 0.0+ 0.054 s 9.26

β+:100.00

0

3.548E+06 3.548E+06 NUBASE

0984 39-Y - 78M 5.0+ 5.8E-03 s 8.62

β+:100.00

0

3.548E+06 3.548E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 75

MAIN DATA TABLES

Page 76: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

0985 39-Y - 79 2.5+ 14.8 s 4.05

β+:100.00

0

2.372E+06 2.372E+06 NUBASE

0986 39-Y - 80 4.0- 35 s 5.71

β+:100.00

4

3.186E+06 2.204E+06 ENSDF

0987 39-Y - 80M 1.0- 2.285E+05 4.8 s 6.25

IT:81.00; β+:19.00

0

5.900E+05 7.751E+05 NUBASE

0988 39-Y - 81 2.5+ 1.173 m 1.42

β+:100.00

4

1.978E+06 1.177E+06 ENSDF

0989 39-Y - 82 1.0+ 8.3 s 2.41

β+:100.00

0

2.606E+06 2.606E+06 NUBASE

0990 39-Y - 83 4.5+ 7.08 m 0.85

β+:97.78; β+

m:2.22

0

1.486E+06 1.486E+06 NUBASE

0991 39-Y - 83M 1.5- 6.198E+04 2.85 m 0.70

β+m:60.00; IT:40.00

0

8.536E+05 8.784E+05 NUBASE

0992 39-Y - 84 1.0+ 4.6 s 4.35

β+:100.00

4

2.357E+06 1.279E+06 ENSDF

0993 39-Y - 84M 5.0- 5.000E+05 40 m 2.50

β+:100.00

4

1.222E+06 3.973E+06 ENSDF

0994 39-Y - 85 0.5- 2.68 h 1.87

β+m:100.00

0

1.007E+06 1.007E+06 NUBASE

0995 39-Y - 85M 4.5+ 1.980E+04 4.86 h 2.67

β+:88.82; β+

m:11.18;

IT:~

0

1.085E+06 1.085E+06 NUBASE

0996 39-Y - 86 4.0- 14.74 h 0.14

β+:100.00

4

2.175E+05 3.570E+06 ENSDF

0997 39-Y - 86M 8.0+ 2.183E+05 48 m 2.08

β+:0.69; IT:99.31

4

2.307E+04 2.201E+05 ENSDF

0998 39-Y - 87 0.5- 3.325 d 0.25

β+m:100.00

4

7.197E+03 4.617E+05 UKPADD67

0999 39-Y - 87M 4.5+ 3.808E+05 13.37 h 0.22

β+:1.57; IT:98.43

4

7.865E+04 3.082E+05 UKPADD67

1000 39-Y - 88 4.0- 106.629 d 0.02

β+:100.00

4

6.334E+03 2.695E+06 LNHB

1001 39-Y - 88M 8.0+ 6.746E+05 0.014 s 1.44

IT:100.00

0

6.746E+05 NUBASE

1002 39-Y - 89 0.5-

NUBASE

1003 39-Y - 89M 4.5+ 9.090E+05 15.663 s 0.03

IT:100.00

3

7.246E+03 9.014E+05 ENSDF

1004 39-Y - 90 2.0- 2.671 d 0.12

β-:100.00

4

9.338E+05 1.237E+00 ENSDF

1005 39-Y - 90M 7.0+ 6.820E+05 3.19 h 1.88

IT:100.00

3

4.527E+04 6.353E+05 ENSDF

1006 39-Y - 91 0.5- 58.51 d 0.10

β-:100.00

2

6.059E+05 3.133E+03 LNHB

1007 39-Y - 91M 4.5+ 5.556E+05 49.71 m 0.08

IT:100.00

3

2.628E+04 5.283E+05 ENSDF

1008 39-Y - 92 2.0- 3.54 h 0.56

β-:100.00

4

1.437E+06 2.516E+05 LNHB

1009 39-Y - 93 0.5- 10.18 h 0.79

β-:100.00

4

1.172E+06 9.518E+04 ENSDF

1010 39-Y - 93M 3.5+ 7.587E+05 0.82 s 4.88

IT:100.00

3

7.508E+04 6.796E+05 ENSDF

1011 39-Y - 94 2.0- 18.7 m 0.53

β-:100.00

2

1.814E+06 7.642E+05 ENSDF

1012 39-Y - 95 0.5- 10.3 m 0.97

β-:100.00

2

1.436E+06 1.092E+06 ENSDF

1013 39-Y - 96 0.0- 5.34 s 0.94

β-:100.00

4

3.205E+06 8.009E+04 ENSDF

1014 39-Y - 96M 8.0+ 1.600E+06 9.62 s 1.56

β-:100.00

4

1.851E+06 4.486E+06 UKPADD67

1015 39-Y - 97 0.5- 3.75 s 0.53

β-:99.95; β-,n:0.06

5

2.135E+06 1.846E+06 1.189E+02 UKPADD67

1016 39-Y - 97M 4.5+ 6.675E+05 1.17 s 2.56

β-:99.25; IT:0.70;

β-,n:0.05

5

2.317E+06 2.111E+06 1.425E+02 UKPADD67

1017 39-Y - 97N 13.5- 3.523E+06 0.142 s 5.63

β-:1.60; ITm:98.40

4

1.207E+05 2.807E+06 UKPADD67

1018 39-Y - 98 0.0- 0.59 s 5.08

β-:99.73; β-,n:0.27

5

2.780E+06 2.613E+06 1.039E+03 UKPADD67

1019 39-Y - 98M 5.0+ 1.000E+06 2 s 10

β-:96.56; β-,n:3.44

5

2.788E+06 3.294E+06 1.576E+04 UKPADD67

1020 39-Y - 99 2.5+ 1.477 s 0.34

β-:98.30; β-,n:1.70

5

2.949E+06 9.167E+05 7.357E+03 UKPADD67

1021 39-Y -100 ? 0.735 s 0.95

β-:99.08; β-,n:0.92

0

3.080E+06 3.080E+06 5.535E+03 NUBASE

1022 39-Y -100M ? 2.000E+05 0.94 s 3.19

β-:100.00

0

3.170E+06 3.170E+06 NUBASE

1023 39-Y -101 2.5+ 0.45 s 4.44

β-:100.00

4

3.553E+06 7.210E+05 ENSDF

1024 39-Y -102 ? 0.3 s 3.33

β-:95.10; β-,n:4.90

0

3.165E+06 3.165E+06 4.286E+04 NUBASE

1025 39-Y -102M ? 2.000E+05 0.36 s 11.11

β-:95.10; β-,n:4.90

0

3.231E+06 3.231E+06 4.531E+04 NUBASE

76 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 77: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1026 39-Y -103 2.5+ 0.224 s 8.48

β-:92.00; β-,n:8.00

0

2.986E+06 2.986E+06 9.457E+04 NUBASE

1027 39-Y -104 0.0- 0.13 s 15.38

β-:91.22; β-,n:8.78

3

3.494E+06 3.750E+06 4.948E+04 UKPADD67

1028 39-Y -105 2.5+ 0.15 s 13.33

β-:80.25; β-,n:19.75

3

3.325E+06 2.372E+06 1.235E+05 UKPADD67

1029 39-Y -106 ? 0.05 s 100

β-:100.00

0

4.310E+06 4.310E+06 NUBASE

1030 39-Y -107 2.5+ 0.03 s 100

β-:100.00

0

4.157E+06 4.157E+06 NUBASE

1031 39-Y -108 ? 0.02 s 100

β-:100.00

0

4.820E+06 4.820E+06 NUBASE

1032 40-Zr- 78 0.0+ 0.05 s 100

β+:100.00

0

3.610E+06 3.610E+06 NUBASE

1033 40-Zr- 79 2.5+ 0.056 s 53.57

β+:100.00

0

3.667E+06 3.667E+06 NUBASE

1034 40-Zr- 80 0.0+ 4.6 s 13.04

β+m:100.00

0

1.824E+06 1.824E+06 NUBASE

1035 40-Zr- 81 1.5- 5.5 s 7.27

β+:99.88; β+,p:0.12

0

2.508E+06 2.508E+06 1.359E+03 NUBASE

1036 40-Zr- 82 0.0+ 32 s 15.62

β+:100.00

0

1.333E+06 1.333E+06 NUBASE

1037 40-Zr- 83 0.5- 41.6 s 5.77

β+:3.90; β+

m:96.10

4

2.101E+06 1.188E+06 ENSDF

1038 40-Zr- 84 0.0+ 25.9 m 2.70

β+:100.00

0

8.900E+05 8.900E+05 NUBASE

1039 40-Zr- 85 3.5+ 7.86 m 0.51

β+:100.00

4

1.325E+06 1.456E+06 ENSDF

1040 40-Zr- 85M 0.5- 2.922E+05 10.9 s 2.75

IT:92.00; β+:8.00

0

1.329E+05 4.017E+05 NUBASE

1041 40-Zr- 86 0.0+ 16.5 h 0.61

β+:50.00; β+

m:50.00

0

4.583E+05 4.583E+05 NUBASE

1042 40-Zr- 87 4.5+ 1.68 h 0.60

β+:0.28; β+

m:99.72

4

8.256E+05 9.411E+05 ENSDF

1043 40-Zr- 87M 0.5- 3.363E+05 14 s 1.43

IT:100.00

3

9.819E+04 2.374E+05 ENSDF

1044 40-Zr- 88 0.0+ 83 d 0.48

β+:100.00

4

1.403E+04 3.919E+05 LNHB

1045 40-Zr- 89 4.5+ 3.267 d 0.26

β+:0.13; β+

m:99.87

4

9.278E+04 2.539E+05 UKPADD67

1046 40-Zr- 89M 0.5- 5.878E+05 4.18 m 0.24

β+:6.66; IT:93.34

4

3.274E+04 6.380E+05 UKPADD67

1047 40-Zr- 90 0.0+

NUBASE

1048 40-Zr- 90M 5.0- 2.319E+06 0.809 s 0.25

IT:100.00

3

1.705E+04 2.329E+06 ENSDF

1049 40-Zr- 91 2.5+

NUBASE

1050 40-Zr- 92 0.0+

NUBASE

1051 40-Zr- 93 2.5+ 1.53E+06 y 6.54

β-:2.50; β-

m:97.50

1

1.922E+04 ENSDF

1052 40-Zr- 94 0.0+ 6E+15 y 100

2β-:100.00

0

1.144E+06 ENSDF

1053 40-Zr- 95 2.5+ 64.032 d 0.01

β-:98.92; β-

m:1.08

4

1.200E+05 7.328E+05 LNHB

1054 40-Zr- 96 0.0+ 3.9E+19 y 23.08

2β-:100.00

0

3.350E+06 ENSDF

1055 40-Zr- 97 0.5+ 16.744 h 0.07

β-:4.95; β-

m:95.05

4

7.023E+05 1.591E+05 ENSDF

1056 40-Zr- 98 0.0+ 30.7 s 1.30

β-:100.00

1

9.100E+05 ENSDF

1057 40-Zr- 99 0.5+ 2.2 s 4.55

β-m:36.80; β-:63.20

4

1.539E+06 8.414E+05 UKPADD67

1058 40-Zr-100 0.0+ 7.1 s 5.63

β-:100.00

2

1.307E+06 2.413E+05 ENSDF

1059 40-Zr-101 1.5+ 2.3 s 4.35

β-:100.00

4

2.179E+06 5.582E+05 ENSDF

1060 40-Zr-102 0.0+ 2.9 s 6.90

β-:100.00

2

1.997E+06 2.369E+05 ENSDF

1061 40-Zr-103 2.5- 1.3 s 7.69

β-:100.00

0

2.317E+06 2.317E+06 NUBASE

1062 40-Zr-104 0.0+ 1.2 s 25

β-:100.00

0

1.960E+06 1.960E+06 NUBASE

1063 40-Zr-105 2.5+ 0.6 s 33.33

β-:98.60; β-,n:1.40

3

2.662E+06 1.764E+06 4.466E+03 UKPADD67

1064 40-Zr-106 0.0+ 0.9 s 22.22

β-:98.48; β-,n:1.52

3

2.138E+06 1.091E+06 5.801E+03 UKPADD67

1065 40-Zr-107 2.5+ 0.24 s 16.67

β-:96.29; β-,n:3.71

3

2.982E+06 2.201E+06 1.751E+04 UKPADD67

1066 40-Zr-108 0.0+ 0.08 s 100

β-:100.00

0

2.833E+06 2.833E+06 NUBASE

1067 40-Zr-109 ? 0.06 s 100

β-:100.00

0

3.607E+06 3.607E+06 NUBASE

1068 40-Zr-110 0.0+ 0.03 s 100

β-:100.00

0

3.240E+06 3.240E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 77

MAIN DATA TABLES

Page 78: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1069 41-Nb- 81 1.5- 4.4E-08 s 100

p:50.00; β+:50.00

0

1.835E+06 1.835E+06 3.755E+05 NUBASE

1070 41-Nb- 82 0.0+ 0.05 s 10

β+:100.00

3

4.839E+06 1.020E+06 1.496E+03 ENSDF

1071 41-Nb- 83 2.5+ 4.1 s 7.32

β+:100.00

0

2.500E+06 2.500E+06 NUBASE

1072 41-Nb- 84 3.0+ 12 s 25

β+:100.00

4

3.831E+06 1.728E+06 ENSDF

1073 41-Nb- 85 4.5+ 20.9 s 3.35

β+:100.00

0

2.000E+06 2.000E+06 NUBASE

1074 41-Nb- 85M 0.5- 7.590E+05 12 s 41.67

β+m:100.00

0

2.156E+06 2.156E+06 NUBASE

1075 41-Nb- 86 6.0+ 1.467 m 1.14

β+:100.00

0

2.657E+06 2.657E+06 NUBASE

1076 41-Nb- 86M ? 2.500E+05 56 s 14.29

β+:100.00

0

2.740E+06 2.740E+06 NUBASE

1077 41-Nb- 87 0.5- 3.75 m 2.40

β+:100.00

4

1.774E+06 1.220E+06 ENSDF

1078 41-Nb- 87M 4.5+ 3.840E+03 2.6 m 3.85

β+:100.00

4

1.390E+06 1.767E+06 ENSDF

1079 41-Nb- 88 8.0+ 14.5 m 0.69

β+:100.00

0

2.518E+06 2.518E+06 NUBASE

1080 41-Nb- 88M 4.0- 3.900E+05 7.8 m 1.28

β+:100.00

0

2.648E+06 2.648E+06 NUBASE

1081 41-Nb- 89 4.5+ 2.03 h 3.45

β+:98.77; β+

m:1.23

4

1.105E+06 1.365E+06 ENSDF

1082 41-Nb- 89M 0.5- 1.1 h 3.03

β+m:100.00

0

1.210E+06 1.210E+06 NUBASE

1083 41-Nb- 90 8.0+ 14.6 h 0.34

β+:1.81; β+

m:98.19

0

1.278E+06 1.278E+06 NUBASE

1084 41-Nb- 90M 4.0- 1.247E+05 18.81 s 0.32

IT:100.00

0

1.247E+05 NUBASE

1085 41-Nb- 90N 1.0+ 3.820E+05 6.19E-03 s 1.29

ITm:100.00

0

2.573E+05 NUBASE

1086 41-Nb- 91 4.5+ 680.016 y 19.12

β+:100.00

3

5.880E+03 1.257E+04 UKPADD67

1087 41-Nb- 91M 0.5- 1.045E+05 60.9 d 0.33

IT:97.60; β+:2.40

4

9.346E+04 3.803E+04 UKPADD67

1088 41-Nb- 92 7.0+ 3.5E+07 y 8.57

β+:100.00

4

7.932E+03 1.503E+06 UKPADD67

1089 41-Nb- 92M 2.0+ 1.355E+05 10.15 d 0.20

β+:100.00

4

6.447E+03 9.704E+05 UKPADD67

1090 41-Nb- 93 4.5+

NUBASE

1091 41-Nb- 93M 0.5- 3.080E+04 16.126 y 0.85

IT:100.00

3

2.896E+04 1.955E+03 UKPADD67

1092 41-Nb- 94 6.0+ 1.999E+04 y 12.33

β-:100.00

4

1.683E+05 1.572E+06 UKPADD67

1093 41-Nb- 94M 3.0+ 4.095E+04 6.26 m 0.16

β-:0.50; IT:99.50

4

3.509E+04 1.227E+04 UKPADD67

1094 41-Nb- 95 4.5+ 34.991 d 0.02

β-:100.00

4

4.452E+04 7.645E+05 LNHB

1095 41-Nb- 95M 0.5- 2.357E+05 3.608 d 0.92

β-:5.60; IT:94.40

4

1.787E+05 7.069E+04 ENSDF

1096 41-Nb- 96 6.0+ 23.35 h 0.21

β-:100.00

4

2.502E+05 2.446E+06 UKPADD67

1097 41-Nb- 97 4.5+ 1.202 h 0.97

β-:100.00

4

4.684E+05 6.642E+05 ENSDF

1098 41-Nb- 97M 0.5- 7.434E+05 52.7 s 3.42

IT:100.00

3

1.440E+04 7.280E+05 ENSDF

1099 41-Nb- 98 1.0+ 2.86 s 2.10

β-:100.00

4

1.965E+06 3.245E+05 ENSDF

1100 41-Nb- 98M 5.0+ 8.400E+04 51.3 m 0.78

β-:100.00

4

7.714E+05 2.782E+06 ENSDF

1101 41-Nb- 99 4.5+ 15 s 1.33

β-:100.00

4

1.514E+06 1.743E+05 ENSDF

1102 41-Nb- 99M 0.5- 3.653E+05 2.6 m 7.69

β-:98.00; IT:2.00

4

1.416E+06 6.504E+05 ENSDF

1103 41-Nb-100 1.0+ 1.5 s 13.33

β-:100.00

4

2.493E+06 7.082E+05 ENSDF

1104 41-Nb-100M 4.0+ 4.800E+05 2.9 s 6.90

β-:100.00

4

2.047E+06 2.064E+06 UKPADD67

1105 41-Nb-101 2.5+ 7.1 s 4.23

β-:100.00

4

1.863E+06 2.446E+05 ENSDF

1106 41-Nb-102 1.0+ 1.3 s 15.38

β-:100.00

0

2.402E+06 2.402E+06 NUBASE

1107 41-Nb-102M ? 1.300E+05 4.3 s 9.30

β-:100.00

2

2.276E+06 2.094E+06 ENSDF

1108 41-Nb-103 2.5+ 1.5 s 13.33

β-:100.00

0

1.843E+06 1.843E+06 NUBASE

1109 41-Nb-104 1.0+ 4.9 s 6.12

β-:99.94; β-,n:0.06

0

2.702E+06 2.702E+06 8.381E+01 NUBASE

1110 41-Nb-104M ? 2.200E+05 0.94 s 4.26

β-:99.95; β-,n:0.05

0

2.775E+06 2.775E+06 9.734E+01 NUBASE

1111 41-Nb-105 2.5+ 2.95 s 2.03

β-:98.30; β-,n:1.70

0

2.133E+06 2.133E+06 5.987E+03 NUBASE

78 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 79: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1112 41-Nb-106 2.0+ 0.92 s 4.35

β-:95.50; β-,n:4.50

0

2.939E+06 2.939E+06 2.440E+04 NUBASE

1113 41-Nb-107 2.5+ 0.3 s 3

β-:94.00; β-,n:6.00

0

2.562E+06 2.562E+06 4.896E+04 NUBASE

1114 41-Nb-108 2.0+ 0.193 s 8.81

β-:93.80; β-,n:6.20

0

3.379E+06 3.379E+06 6.461E+04 NUBASE

1115 41-Nb-109 2.5+ 0.19 s 31.58

β-:87.35; β-,n:12.65

3

3.158E+06 2.263E+06 6.840E+04 UKPADD67

1116 41-Nb-110 2.0+ 0.17 s 11.76

β-:60.00; β-,n:40.00

0

2.924E+06 2.924E+06 5.559E+05 NUBASE

1117 41-Nb-111 2.5+ 0.08 s 100

β-:100.00

0

3.490E+06 3.490E+06 NUBASE

1118 41-Nb-112 2.0+ 0.06 s 100

β-:100.00

0

4.343E+06 4.343E+06 NUBASE

1119 41-Nb-113 2.5+ 0.03 s 100

β-:100.00

0

3.980E+06 3.980E+06 NUBASE

1120 42-Mo- 83 1.5- 0.023 s 82.61

β+:100.00

0

3.737E+06 3.737E+06 NUBASE

1121 42-Mo- 84 0.0+ 3.8E-03 s 23.68

β+:100.00

0

2.023E+06 2.023E+06 NUBASE

1122 42-Mo- 85 0.5- 3.2 s 6.25

β+m:100.00

0

2.430E+06 2.430E+06 NUBASE

1123 42-Mo- 86 0.0+ 19.6 s 5.61

β+:50.00; β+

m:50.00

0

1.715E+06 1.715E+06 NUBASE

1124 42-Mo- 87 3.5+ 14.02 s 1.85

β+:100.00

4

2.322E+03 1.239E+06 ENSDF

1125 42-Mo- 88 0.0+ 8 m 2.50

β+:50.00; β+

m:50.00

0

1.058E+06 1.058E+06 NUBASE

1126 42-Mo- 89 4.5+ 2.11 m 4.74

β+:100.00

4

1.955E+06 1.226E+06 ENSDF

1127 42-Mo- 89M 0.5- 3.875E+05 0.19 s 7.89

IT:100.00

0

3.875E+05 NUBASE

1128 42-Mo- 90 0.0+ 5.56 h 1.62

β+:6.70; β+

n:93.30

0

7.109E+05 7.109E+05 NUBASE

1129 42-Mo- 91 4.5+ 15.49 m 0.06

β+:99.97; β+

m:0.03

4

1.451E+06 9.776E+05 ENSDF

1130 42-Mo- 91M 0.5- 6.529E+05 1.077 m 0.93

β+m:50.00; IT:50.00

4

5.563E+05 1.387E+06 ENSDF

1131 42-Mo- 92 0.0+ 1.9E+20 y 100

2β+:100.00

0

1.649E+06 NUBASE

1132 42-Mo- 93 2.5+ 4000.009 y 20

β+:12.00; β+

m:88.00

4

5.086E+03 1.073E+04 LNHB

1133 42-Mo- 93M 10.5+ 2.425E+06 6.85 h 1.02

β+:0.12; IT:99.88

4

1.072E+05 2.318E+06 UKPADD67

1134 42-Mo- 94 0.0+

NUBASE

1135 42-Mo- 95 2.5+

NUBASE

1136 42-Mo- 96 0.0+

NUBASE

1137 42-Mo- 97 2.5+

NUBASE

1138 42-Mo- 98 0.0+ 1E+14 y 100

2β-:100.00

0

1.120E+05 ENSDF

1139 42-Mo- 99 0.5+ 2.748 d 0.02

β-:11.94; β-

m:88.06

4

3.937E+05 1.484E+05 ENSDF

1140 42-Mo-100 0.0+ 9.9E+18 y 7.07

2β-:100.00

0

3.034E+06 ENSDF

1141 42-Mo-101 0.5+ 14.61 m 0.21

β-:100.00

4

5.433E+05 1.424E+06 ENSDF

1142 42-Mo-102 0.0+ 11.3 m 1.77

β-:100.00

2

3.491E+05 1.845E+04 ENSDF

1143 42-Mo-103 1.5+ 1.132 m 0.88

β-:100.00

4

1.316E+06 6.362E+05 UKPADD67

1144 42-Mo-104 0.0+ 1 m 3.33

β-:100.00

0

7.200E+05 7.200E+05 NUBASE

1145 42-Mo-105 2.5- 35.6 s 4.49

β-:100.00

4

1.922E+06 5.515E+05 ENSDF

1146 42-Mo-106 0.0+ 8.73 s 1.37

β-:100.00

0

1.173E+06 1.173E+06 NUBASE

1147 42-Mo-107 3.5- 3.5 s 14.29

β-:100.00

0

2.053E+06 2.053E+06 NUBASE

1148 42-Mo-108 0.0+ 1.09 s 1.83

β-:100.00

0

1.550E+06 1.550E+06 NUBASE

1149 42-Mo-109 2.5+ 0.5 s 40

β-:99.47; β-,n:0.53

3

2.675E+06 1.876E+06 9.118E+02 UKPADD67

1150 42-Mo-110 0.0+ 0.3 s 13.33

β-:100.00

0

1.833E+06 1.833E+06 NUBASE

1151 42-Mo-111 2.5+ 0.5 s 40

β-:98.97; β-,n:1.03

3

3.098E+06 2.413E+06 3.572E+03 UKPADD67

1152 42-Mo-112 0.0+ 1 s 20

β-:97.92; β-,n:2.08

3

2.552E+06 1.354E+06 7.960E+03 UKPADD67

1153 42-Mo-113 ? 0.1 s 100

β-:100.00

0

3.193E+06 3.193E+06 NUBASE

1154 42-Mo-114 0.0+ 0.08 s 100

β-:100.00

0

2.807E+06 2.807E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 79

MAIN DATA TABLES

Page 80: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1155 42-Mo-115 ? 0.06 s 100

β-:100.00

0

3.600E+06 3.600E+06 NUBASE

1156 43-Tc- 85 0.5- 1.1E-07 s 100

p:50.00; β+:50.00

0

1.905E+06 1.905E+06 4.255E+05 NUBASE

1157 43-Tc- 86 0.0+ 0.055 s 10.91

β+:100.00

0

3.783E+06 3.783E+06 NUBASE

1158 43-Tc- 87 0.5- 2.2 s 9.09

β+:100.00

0

2.857E+06 2.857E+06 NUBASE

1159 43-Tc- 87M 4.5+ 2.000E+04 2 s 100

β+:50.00; IT:50.00

0

1.432E+06 1.442E+06 NUBASE

1160 43-Tc- 88 ? 5.8 s 3.45

β+:100.00

0

3.330E+06 3.330E+06 NUBASE

1161 43-Tc- 88M ? 6.4 s 12.50

β+:100.00

0

3.330E+06 3.330E+06 NUBASE

1162 43-Tc- 89 4.5+ 12.8 s 7.03

β+:50.00; β+

m:50.00

0

2.323E+06 2.323E+06 NUBASE

1163 43-Tc- 89M 0.5- 6.260E+04 12.9 s 6.20

β+:49.99; β+

m:49.99;

IT:0.01

0

2.344E+06 2.344E+06 NUBASE

1164 43-Tc- 90 1.0+ 8.7 s 2.30

β+:100.00

4

3.348E+06 1.751E+06 ENSDF

1165 43-Tc- 90M 8.0+ 3.100E+05 49.2 s 0.81

β+:100.00

0

3.089E+06 3.089E+06 NUBASE

1166 43-Tc- 91 4.5+ 3.14 m 0.64

β+:99.32; β+

m:0.68

0

2.073E+06 2.073E+06 NUBASE

1167 43-Tc- 91M 0.5- 1.393E+05 3.3 m 3.03

β+:2.46; β+

m:96.54;

IT:1.00

0

1.890E+06 1.891E+06 NUBASE

1168 43-Tc- 92 8.0+ 4.25 m 3.53

β+:100.00

0

2.623E+06 2.623E+06 NUBASE

1169 43-Tc- 93 4.5+ 2.75 h 1.82

β+:100.00

4

4.309E+04 1.568E+06 ENSDF

1170 43-Tc- 93M 0.5- 3.918E+05 43.5 m 2.30

β+:23.40; IT:76.60

4

9.077E+04 8.077E+05 ENSDF

1171 43-Tc- 94 7.0+ 4.883 h 0.34

β+:100.00

4

4.314E+04 2.649E+06 ENSDF

1172 43-Tc- 94M 2.0+ 7.550E+04 52 m 1.92

β+:100.00

4

7.540E+05 1.930E+06 ENSDF

1173 43-Tc- 95 4.5+ 20 h 0.50

β+:100.00

4

6.296E+03 7.965E+05 ENSDF

1174 43-Tc- 95M 0.5- 3.890E+04 61 d 3.28

β+:96.12; IT:3.88

4

1.477E+04 6.885E+05 ENSDF

1175 43-Tc- 96 7.0+ 4.28 d 1.64

β+:100.00

4

5.306E+03 2.503E+06 ENSDF

1176 43-Tc- 96M 4.0+ 3.428E+04 51.5 m 1.94

IT:98.00; β+:2.00

0

2.005E+04 5.365E+04 NUBASE

1177 43-Tc- 97 4.5+ 2.6E+06 y 15.38

β+:100.00

3

5.653E+03 1.168E+04 UKPADD67

1178 43-Tc- 97M 0.5- 9.660E+04 90.2 d 1.22

IT:100.00

3

8.704E+04 9.496E+03 UKPADD67

1179 43-Tc- 98 6.0+ 4.2E+06 y 7.14

β-:100.00

2

1.180E+05 1.413E+06 ENSDF

1180 43-Tc- 99 4.5+ 2.14E+05 y 3.74

β-:100.00

4

8.540E+04 7.040E-01 LNHB

1181 43-Tc- 99M 0.5- 1.427E+05 6.01 h 0.17

IT:100.00; β-:~

4

1.549E+04 1.265E+05 ENSDF

1182 43-Tc-100 1.0+ 15.8 s 0.63

β-:100.00

4

1.315E+06 8.272E+04 ENSDF

1183 43-Tc-101 4.5+ 14.2 m 0.70

β-:100.00

4

4.786E+05 3.359E+05 ENSDF

1184 43-Tc-102 1.0+ 5.28 s 2.84

β-:100.00

2

1.945E+06 8.076E+04 ENSDF

1185 43-Tc-102M ? 2.000E+04 4.35 m 1.61

β-:100.00

2

7.798E+05 2.511E+06 ENSDF

1186 43-Tc-103 2.5+ 54.2 s 1.48

β-:100.00

4

9.794E+05 2.484E+05 ENSDF

1187 43-Tc-104 3.0+ 18.3 m 1.64

β-:100.00

4

1.595E+06 1.890E+06 ENSDF

1188 43-Tc-105 1.5- 7.6 m 1.32

β-:100.00

2

1.310E+06 6.684E+05 ENSDF

1189 43-Tc-106 ? 36 s 2.78

β-:100.00

4

1.943E+06 2.191E+06 ENSDF

1190 43-Tc-107 1.5- 21.2 s 0.94

β-:100.00

4

2.056E+06 5.148E+05 ENSDF

1191 43-Tc-108 2.0+ 5.17 s 1.35

β-:100.00

0

2.573E+06 2.573E+06 NUBASE

1192 43-Tc-109 1.5- 0.86 s 4.65

β-:99.92; β-,n:0.08

0

2.102E+06 2.102E+06 2.117E+02 NUBASE

1193 43-Tc-110 2.0+ 0.92 s 3.26

β-:99.96; β-,n:0.04

0

3.006E+06 3.006E+06 1.819E+02 NUBASE

1194 43-Tc-111 1.5- 0.29 s 6.90

β-:100.00

4

3.219E+06 4.054E+05 ENSDF

1195 43-Tc-112 2.0+ 0.29 s 6.90

β-:98.50; β-,n:1.50

0

3.122E+06 3.122E+06 9.745E+03 NUBASE

80 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 81: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1196 43-Tc-113 2.5+ 0.13 s 30.77

β-:92.81; β-,n:7.19

3

2.732E+06 1.822E+06 3.352E+04 UKPADD67

1197 43-Tc-114 2.0+ 0.2 s 20

β-:93.46; β-,n:6.54

3

3.578E+06 3.257E+06 3.288E+04 UKPADD67

1198 43-Tc-115 2.5+ 0.27 s 18.52

β-:85.66; β-,n:14.34

3

2.995E+06 2.162E+06 7.974E+04 UKPADD67

1199 43-Tc-116 2.0+ 0.12 s 16.67

β-:87.78; β-,n:12.22

3

3.693E+06 3.495E+06 7.173E+04 UKPADD67

1200 43-Tc-117 1.5- 0.04 s 100

β-:100.00

0

3.387E+06 3.387E+06 NUBASE

1201 43-Tc-118 2.0+ 0.03 s 100

β-:100.00

0

4.240E+06 4.240E+06 NUBASE

1202 44-Ru- 87 0.5- 0.05 s 100

β+:100.00

0

3.927E+06 3.927E+06 NUBASE

1203 44-Ru- 88 0.0+ 1.3 s 23.08

β+:50.00; β+

m:50.00

0

2.353E+06 2.353E+06 NUBASE

1204 44-Ru- 89 3.5+ 1.38 s 7.97

β+:50.00; β+

m:50.00

0

2.766E+06 2.766E+06 NUBASE

1205 44-Ru- 90 0.0+ 11 s 27.27

β+:50.00; β+

m:50.00

0

1.915E+06 1.915E+06 NUBASE

1206 44-Ru- 91 4.5+ 9 s 11.11

β+:100.00

0

2.440E+06 2.440E+06 NUBASE

1207 44-Ru- 91M 0.5- 4.000E+05 7.6 s 10.53

β+m:100.00

0

2.527E+06 2.527E+06 NUBASE

1208 44-Ru- 92 0.0+ 3.65 m 1.37

β+:100.00

0

1.508E+06 1.508E+06 NUBASE

1209 44-Ru- 93 4.5+ 59.7 s 1.01

β+:100.00

4

2.340E+06 1.131E+06 ENSDF

1210 44-Ru- 93M 0.5- 7.344E+05 10.8 s 2.78

β+m:77.97; IT:22.00;

β+,p:0.03

0

1.735E+06 1.897E+06 2.012E+02 NUBASE

1211 44-Ru- 94 0.0+ 51.8 m 1.16

β+m:100.00

4

5.005E+03 5.195E+05 ENSDF

1212 44-Ru- 95 2.5+ 1.643 h 0.85

β+:97.39; β+

m:2.61

4

8.172E+04 1.238E+06 ENSDF

1213 44-Ru- 96 0.0+ 6.7E+16 y 100

2β+:100.00

0

2.718E+06 NUBASE

1214 44-Ru- 97 2.5+ 2.9 d 3.45

β+:99.96; β+

m:0.04

4

1.233E+04 2.407E+05 ENSDF

1215 44-Ru- 98 0.0+

NUBASE

1216 44-Ru- 99 2.5+

NUBASE

1217 44-Ru-100 0.0+

NUBASE

1218 44-Ru-101 2.5+

NUBASE

1219 44-Ru-102 0.0+

NUBASE

1220 44-Ru-103 1.5+ 39.26 d 0.05

β-:1.20; β-

m:98.80

4

6.656E+04 4.961E+05 ENSDF

1221 44-Ru-103M 5.5- 2.380E+05 1.69E-03 s 4.14

IT:100.00

3

2.249E+04 2.159E+05 ENSDF

1222 44-Ru-104 0.0+

NUBASE

1223 44-Ru-105 1.5+ 4.44 h 0.45

β-:71.61; β-

m:28.39

4

4.400E+05 7.478E+05 ENSDF

1224 44-Ru-106 0.0+ 1.02 y 0.27

β-:100.00

1

1.010E+04 LNHB

1225 44-Ru-107 2.5+ 3.75 m 1.33

β-:100.00

4

1.084E+06 3.453E+05 ENSDF

1226 44-Ru-108 0.0+ 4.55 m 1.10

β-:100.00

0

4.500E+05 4.500E+05 NUBASE

1227 44-Ru-109 2.5+ 34.5 s 1.45

β-:100.00

4

1.044E+06 1.664E+06 ENSDF

1228 44-Ru-110 0.0+ 11.6 s 5.17

β-:100.00

4

1.157E+06 3.472E+04 ENSDF

1229 44-Ru-111 2.5+ 2.12 s 3.30

β-:100.00

0

1.896E+06 1.896E+06 NUBASE

1230 44-Ru-112 0.0+ 1.75 s 4

β-:100.00

0

1.420E+06 1.420E+06 NUBASE

1231 44-Ru-113 2.5+ 0.8 s 7.50

β-:100.00

4

2.695E+06 5.828E+05 ENSDF

1232 44-Ru-113M 5.5- 1.300E+05 0.51 s 5.88

IT:50.00; β-:50.00

0

1.102E+06 1.167E+06 NUBASE

1233 44-Ru-114 0.0+ 0.53 s 11.32

β-:100.00

0

1.700E+06 1.700E+06 NUBASE

1234 44-Ru-115 2.5+ 0.7 s 28.57

β-:99.77; β-,n:0.23

3

2.538E+06 1.806E+06 6.150E+02 UKPADD67

1235 44-Ru-116 0.0+ 1.7 s 17.65

β-:98.92; β-,n:1.08

3

1.843E+06 9.860E+05 3.609E+03 UKPADD67

1236 44-Ru-117 2.5+ 0.34 s 20.59

β-:97.95; β-,n:2.05

3

2.697E+06 2.026E+06 8.306E+03 UKPADD67

1237 44-Ru-118 0.0+ 0.7 s 28.57

β-:95.89; β-,n:4.11

3

2.094E+06 1.118E+06 1.780E+04 UKPADD67

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 81

MAIN DATA TABLES

Page 82: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1238 44-Ru-119 2.5+ 0.19 s 21.05

β-:95.64; β-,n:4.36

3

2.920E+06 2.311E+06 2.066E+04 UKPADD67

1239 44-Ru-120 0.0+ 0.08 s 100

β-:100.00

0

2.763E+06 2.763E+06 NUBASE

1240 45-Rh- 89 3.5+ 0.01 s 100

β+:100.00

0

3.950E+06 3.950E+06 NUBASE

1241 45-Rh- 90 0.0+ 0.015 s 46.67

β+:100.00

0

4.030E+06 4.030E+06 NUBASE

1242 45-Rh- 90M 9.0+ 1.1E-03 s 27.27

β+:100.00

0

4.030E+06 4.030E+06 NUBASE

1243 45-Rh- 91 3.5+ 1.74 s 8.05

β+:100.00

0

3.187E+06 3.187E+06 NUBASE

1244 45-Rh- 92 6.0+ 4.3 s 30.23

β+:100.00

0

3.683E+06 3.683E+06 NUBASE

1245 45-Rh- 93 4.5+ 13.9 s 11.51

β+:50.00; β+

m:50.00

0

2.578E+06 2.578E+06 NUBASE

1246 45-Rh- 94 3.0+ 1.177 m 0.85

β+:100.00

4

2.883E+06 3.307E+06 ENSDF

1247 45-Rh- 94M 8.0+ 3.000E+05 25.8 s 0.78

β+:100.00

4

2.812E+06 3.663E+06 ENSDF

1248 45-Rh- 95 4.5+ 5.02 m 1.99

β+:100.00

0

1.703E+06 1.703E+06 NUBASE

1249 45-Rh- 95M 0.5- 5.433E+05 1.96 m 2.04

IT:88.00; β+:12.00

0

2.261E+05 7.042E+05 NUBASE

1250 45-Rh- 96 6.0+ 9.9 m 1.01

β+:100.00

0

2.131E+06 2.131E+06 NUBASE

1251 45-Rh- 96M 3.0+ 5.200E+04 1.51 m 1.32

IT:60.00; β+:40.00

0

8.593E+05 8.905E+05 NUBASE

1252 45-Rh- 97 4.5+ 30.7 m 1.95

β+:100.00

4

5.208E+05 1.355E+06 ENSDF

1253 45-Rh- 97M 0.5- 2.588E+05 46.2 m 3.46

β+:94.40; IT:5.60

4

1.866E+05 2.092E+06 ENSDF

1254 45-Rh- 98 2.0+ 8.72 m 1.38

β+:100.00

4

1.321E+06 1.774E+06 ENSDF

1255 45-Rh- 98M 5.0+ 6.000E+04 3.6 m 5.56

IT:89.00; β+:11.00

0

1.873E+05 2.407E+05 NUBASE

1256 45-Rh- 99 0.5- 16.1 d 1.24

β+:100.00

0

6.810E+05 6.810E+05 NUBASE

1257 45-Rh- 99M 4.5+ 6.430E+04 4.7 h 2.13

β+:99.84; IT:0.16

0

7.013E+05 7.014E+05 NUBASE

1258 45-Rh-100 1.0- 20.8 h 0.48

β+:100.00

4

4.597E+04 2.742E+06 ENSDF

1259 45-Rh-100M 5.0+ 1.076E+05 4.6 m 4.35

IT:98.30; β+:1.70

0

2.121E+04 1.270E+05 NUBASE

1260 45-Rh-101 0.5- 3.2 y 9.38

β+:100.00

4

2.804E+04 3.123E+05 UKPADD67

1261 45-Rh-101M 4.5+ 1.573E+05 4.34 d 0.23

β+:92.56; IT:7.44

4

2.017E+04 3.056E+05 UKPADD67

1262 45-Rh-102 6.0+ 2.902 y 1.42

β+:100.00

4

1.216E+04 2.122E+06 UKPADD67

1263 45-Rh-102M 2.0- 7.000E+04 208 d 1.92

β-:20.00; β+:75.00;

IT:5.00

5

1.736E+05 4.932E+05 UKPADD67

1264 45-Rh-103 0.5-

NUBASE

1265 45-Rh-103M 3.5+ 3.976E+04 56.114 m 100

IT:100.00

3

3.581E+04 1.686E+03 LNHB

1266 45-Rh-104 1.0+ 42.3 s 0.95

β-:99.55; β+:0.45

5

9.805E+05 1.502E+04 UKPADD67

1267 45-Rh-104M 5.0+ 1.290E+05 4.34 m 0.69

β-:0.13; IT:99.87

4

8.620E+04 4.552E+04 UKPADD67

1268 45-Rh-105 3.5+ 1.473 d 0.17

β-:100.00

4

1.535E+05 7.727E+04 ENSDF

1269 45-Rh-105M 0.5- 1.296E+05 40 s 100

IT:100.00

3

9.242E+04 3.459E+04 ENSDF

1270 45-Rh-106 1.0+ 30 s 0.67

β-:100.00

4

1.411E+06 2.043E+05 LNHB

1271 45-Rh-106M 6.0+ 1.370E+05 2.2 h 2.27

β-:100.00

4

3.216E+05 2.759E+06 UKPADD67

1272 45-Rh-107 3.5+ 21.7 m 1.84

β-:100.00

4

4.321E+05 3.119E+05 ENSDF

1273 45-Rh-108 1.0+ 16.8 s 2.98

β-:100.00

2

1.854E+06 3.171E+05 ENSDF

1274 45-Rh-108M 5.0+ 6 m 5

β-:100.00

0

1.501E+06 1.501E+06 NUBASE

1275 45-Rh-109 3.5+ 1.333 m 2.50

β-:50.00; β-

m:50.00

0

8.338E+05 8.338E+05 NUBASE

1276 45-Rh-110 4.0+ 28.5 s 5.26

β-:100.00

4

1.182E+06 2.554E+06 UKPADD67

1277 45-Rh-110M 1.0+ 1.000E+05 3.2 s 6.25

β-:100.00

4

2.266E+06 3.360E+05 UKPADD67

1278 45-Rh-111 3.5+ 12 s 8.33

β-:100.00

4

1.389E+06 3.570E+05 UKPADD67

1279 45-Rh-112 1.0+ 2.1 s 14.29

β-:100.00

2

2.873E+06 1.924E+05 ENSDF

82 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

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Page 83: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1280 45-Rh-112M ? 3.600E+05 6.8 s 2.94

β-:100.00

2

1.909E+06 2.261E+06 ENSDF

1281 45-Rh-113 3.5+ 2.8 s 4.29

β-:100.00

0

1.670E+06 1.670E+06 NUBASE

1282 45-Rh-114 1.0+ 1.85 s 2.70

β-:100.00

4

1.957E+06 4.068E+05 ENSDF

1283 45-Rh-114M ? 2.000E+05 1.85 s 2.70

β-:100.00

0

2.689E+06 2.689E+06 NUBASE

1284 45-Rh-115 3.5+ 0.99 s 5.05

β-:85.48; β-

m:14.52

0

2.059E+06 2.059E+06 NUBASE

1285 45-Rh-116 1.0+ 0.68 s 8.82

β-:100.00

4

3.445E+06 7.345E+05 ENSDF

1286 45-Rh-116M 6.0- 1.500E+05 0.57 s 8.77

β-:100.00

2

2.611E+06 2.167E+06 ENSDF

1287 45-Rh-117 3.5+ 0.44 s 9.09

β-:100.00

0

2.527E+06 2.527E+06 NUBASE

1288 45-Rh-118 1.0+ 0.32 s 18.75

β-:97.08; β-,n:2.92

3

3.094E+06 2.494E+06 1.216E+04 UKPADD67

1289 45-Rh-119 3.5+ 0.3 s 100

β-:100.00

0

2.793E+06 2.793E+06 NUBASE

1290 45-Rh-120 3.5+ 0.17 s 17.65

β-:94.07; β-,n:5.93

3

3.261E+06 2.837E+06 2.919E+04 UKPADD67

1291 45-Rh-121 3.5+ 0.25 s 20

β-:86.43; β-,n:13.57

3

2.671E+06 1.852E+06 7.406E+04 UKPADD67

1292 45-Rh-122 ? 0.05 s 100

β-:100.00

0

3.930E+06 3.930E+06 NUBASE

1293 46-Pd- 91 3.5+ 0.01 s 100

β+:100.00

0

3.900E+06 3.900E+06 NUBASE

1294 46-Pd- 92 0.0+ 1.1 s 27.27

β+:100.00

0

2.620E+06 2.620E+06 NUBASE

1295 46-Pd- 93 4.5+ 1.07 s 11.21

β+:100.00

0

3.157E+06 3.157E+06 NUBASE

1296 46-Pd- 94 0.0+ 9 s 5.56

β+:100.00

0

2.197E+06 2.197E+06 NUBASE

1297 46-Pd- 95 4.5+ 10 s 100

β+:50.00; β+

m:50.00

0

2.639E+06 2.639E+06 NUBASE

1298 46-Pd- 95M 10.5+ 1.870E+06 13.3 s 2.26

β+:94.10; IT:5.00;

β+,p:0.90

0

3.171E+06 3.265E+06 1.575E+04 NUBASE

1299 46-Pd- 96 0.0+ 2.033 m 1.64

β+m:100.00

4

2.213E+05 1.436E+06 ENSDF

1300 46-Pd- 97 2.5+ 3.1 m 2.90

β+:98.31; β+

m:1.69

4

7.700E+05 2.205E+06 ENSDF

1301 46-Pd- 98 0.0+ 17.7 m 1.69

β+:100.00

4

4.382E+04 4.160E+05 ENSDF

1302 46-Pd- 99 2.5+ 21.4 m 0.93

β+:2.95; β+

m:97.05

4

4.243E+05 1.260E+06 ENSDF

1303 46-Pd-100 0.0+ 3.63 d 2.48

β+:100.00

4

4.327E+04 1.228E+05 ENSDF

1304 46-Pd-101 2.5+ 8.47 h 0.71

β+:0.27; β+

m:99.73

4

3.117E+04 3.509E+05 ENSDF

1305 46-Pd-102 0.0+

NUBASE

1306 46-Pd-103 2.5+ 16.98 d 0.12

β+:0.03; β+

m:99.97

4

5.883E+03 1.468E+04 UKPADD67

1307 46-Pd-104 0.0+

NUBASE

1308 46-Pd-105 2.5+

NUBASE

1309 46-Pd-106 0.0+

NUBASE

1310 46-Pd-107 2.5+ 6.5E+06 y 4.62

β-:100.00

1

9.300E+03 ENSDF

1311 46-Pd-107M 5.5- 2.149E+05 21.3 s 2.35

IT:100.00

3

6.269E+04 1.518E+05 ENSDF

1312 46-Pd-108 0.0+

NUBASE

1313 46-Pd-109 2.5+ 13.701 h 0.02

β-:0.05; β-

m:99.95

4

3.608E+05 6.445E+02 ENSDF

1314 46-Pd-109M 5.5- 1.889E+05 4.69 m 0.21

IT:100.00

3

7.622E+04 1.113E+05 ENSDF

1315 46-Pd-110 0.0+ 6E+17 y 100

2β-:100.00

0

2.000E+06 ENSDF

1316 46-Pd-111 2.5+ 23.4 m 0.85

β-:0.70; β-

m:99.30

4

8.319E+05 4.625E+04 ENSDF

1317 46-Pd-111M 5.5- 1.722E+05 5.5 h 1.82

IT:73.00; β-:7.81;

β-m:19.19

0

2.112E+05 3.369E+05 NUBASE

1318 46-Pd-112 0.0+ 20.3 h 0.99

β-:100.00

4

8.990E+04 5.248E+03 UKPADD67

1319 46-Pd-113 2.5+ 1.517 m 2.20

β-m:95.00; β-:5.00

4

1.330E+06 1.275E+05 UKPADD67

1320 46-Pd-113M 4.5- 8.110E+04 0.3 s 33.33

IT:100.00

3

5.942E+04 2.140E+04 UKPADD67

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 83

MAIN DATA TABLES

Page 84: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1321 46-Pd-114 0.0+ 2.42 m 2.48

β-:100.00

4

5.329E+05 2.590E+04 ENSDF

1322 46-Pd-115 2.5+ 25 s 8

β-:73.00; β-

m:27.00

0

1.526E+06 1.526E+06 NUBASE

1323 46-Pd-115M 5.5- 8.918E+04 50 s 6

β-m:92.00; IT:8.00

0

1.422E+06 1.429E+06 NUBASE

1324 46-Pd-116 0.0+ 11.8 s 3.39

β-:100.00

4

1.003E+06 1.571E+05 ENSDF

1325 46-Pd-117 2.5+ 4.3 s 6.98

β-:50.00; β-

m:50.00

0

1.909E+06 1.909E+06 NUBASE

1326 46-Pd-117M 5.5- 2.032E+05 0.019 s 3.66

IT:100.00

3

7.585E+04 1.302E+05 ENSDF

1327 46-Pd-118 0.0+ 1.9 s 5.26

β-:85.70; β-

m:14.30

4

1.580E+06 4.217E+05 ENSDF

1328 46-Pd-119 ? 0.92 s 14.13

β-:50.00; β-

m:50.00

0

2.310E+06 2.310E+06 NUBASE

1329 46-Pd-120 0.0+ 0.5 s 20

β-:50.00; β-

m:50.00

0

1.800E+06 1.800E+06 NUBASE

1330 46-Pd-121 2.5+ 0.6 s 16.67

β-:99.73; β-,n:0.27

3

2.335E+06 1.638E+06 7.481E+02 UKPADD67

1331 46-Pd-122 0.0+ 0.3 s 100

β-:100.00

0

2.180E+06 2.180E+06 NUBASE

1332 46-Pd-123 ? 0.2 s 100

β-:100.00

0

3.117E+06 3.117E+06 NUBASE

1333 46-Pd-124 0.0+ 0.1 s 100

β-:100.00

0

2.557E+06 2.557E+06 NUBASE

1334 47-Ag- 93 4.5+ 5E-03 s 100

p:50.00; β+:50.00

0

2.153E+06 2.153E+06 7.155E+05 NUBASE

1335 47-Ag- 94 0.0+ 0.037 s 48.65

β+:100.00

0

4.350E+06 4.350E+06 NUBASE

1336 47-Ag- 94M 7.0+ 1.350E+06 0.422 s 3.79

β+:100.00

0

4.800E+06 4.800E+06 NUBASE

1337 47-Ag- 94N 21.0+ 6.500E+06 0.3 s 66.67

β+:100.00

0

6.517E+06 6.517E+06 NUBASE

1338 47-Ag- 95 4.5+ 1.74 s 7.47

β+:100.00

0

3.350E+06 3.350E+06 NUBASE

1339 47-Ag- 95M 0.5- 3.442E+05 0.5 s 100

IT:100.00

0

3.442E+05 NUBASE

1340 47-Ag- 95N 11.5+ 2.531E+06 0.016 s 100

IT:100.00

0

2.531E+06 NUBASE

1341 47-Ag- 95O 18.5+ 4.859E+06 0.04 s 100

ITn:100.00

0

2.328E+06 NUBASE

1342 47-Ag- 96 ? 4.45 s 0.90

β+:90.30; β+,p:4.85;

β+,pm:4.85

0

3.660E+06 3.660E+06 1.506E+05 NUBASE

1343 47-Ag- 96M 2.0+ 6.9 s 8.70

β+:82.00; β+,p:9.00;

β+,pm:9.00

0

3.466E+06 3.466E+06 2.794E+05 NUBASE

1344 47-Ag- 97 4.5+ 25.3 s 1.19

β+:100.00

1

3.138E+06 ENSDF

1345 47-Ag- 98 6.0+ 47.5 s 0.63

β+:100.00

4

1.390E+06 4.616E+06 ENSDF

1346 47-Ag- 99 4.5+ 2.067 m 2.42

β+:100.00

0

1.809E+06 1.809E+06 NUBASE

1347 47-Ag- 99M 0.5- 5.061E+05 10.5 s 4.76

IT:100.00

0

5.061E+05 NUBASE

1348 47-Ag-100 5.0+ 2.01 m 4.48

β+:100.00

0

2.359E+06 2.359E+06 NUBASE

1349 47-Ag-100M 2.0+ 1.552E+04 2.24 m 5.80

β+:50.00; IT:50.00

0

1.182E+06 1.190E+06 NUBASE

1350 47-Ag-101 4.5+ 11.1 m 2.70

β+:100.00

4

8.322E+05 1.544E+06 ENSDF

1351 47-Ag-101M 0.5- 2.741E+05 3.1 s 3.23

IT:100.00

0

2.741E+05 NUBASE

1352 47-Ag-102 5.0+ 12.9 m 2.33

β+:100.00

4

9.615E+05 2.981E+06 ENSDF

1353 47-Ag-102M 2.0+ 9.300E+03 7.7 m 6.49

β+:51.00; IT:49.00

0

9.638E+05 9.684E+05 NUBASE

1354 47-Ag-103 3.5+ 1.095 h 1.07

β+:100.00

4

1.860E+05 8.362E+05 ENSDF

1355 47-Ag-103M 0.5- 1.344E+05 5.7 s 5.26

IT:100.00

0

1.344E+05 NUBASE

1356 47-Ag-104 5.0+ 1.153 h 1.45

β+:100.00

0

1.426E+06 1.426E+06 NUBASE

1357 47-Ag-104M 2.0+ 6.900E+03 33.5 m 5.97

β+:99.93; IT:0.07

0

1.428E+06 1.428E+06 NUBASE

1358 47-Ag-105 0.5- 41.3 d 0.24

β+:100.00

4

1.993E+04 5.304E+05 UKPADD67

1359 47-Ag-105M 3.5+ 2.546E+04 7.23 m 2.21

β+:0.34; IT:99.66

4

2.534E+04 1.221E+03 UKPADD67

1360 47-Ag-106 1.0+ 24 m 0.42

β-:0.50; β+:99.50

5

5.035E+05 7.060E+05 UKPADD67

1361 47-Ag-106M 6.0+ 8.966E+04 8.46 d 1.18

β+:100.00

4

1.227E+04 2.754E+06 UKPADD67

84 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 85: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1362 47-Ag-107 0.5-

NUBASE

1363 47-Ag-107M 3.5+ 9.312E+04 44.3 s 0.45

IT:100.00

3

7.918E+04 1.273E+04 ENSDF

1364 47-Ag-108 1.0+ 2.4 m 0.83

β-:97.10; β+:2.90

5

6.055E+05 2.283E+04 UKPADD67

1365 47-Ag-108M 6.0+ 1.095E+05 418.01 y 3.59

β+:91.30; IT:8.70

4

1.604E+04 1.630E+06 UKPADD67

1366 47-Ag-109 0.5-

NUBASE

1367 47-Ag-109M 3.5+ 8.803E+04 39.7 s 0.50

IT:100.00

3

7.674E+04 1.130E+04 UKPADD67

1368 47-Ag-110 1.0+ 24.56 s 0.45

β+:0.30; β-:99.70

5

1.181E+06 3.134E+04 LNHB

1369 47-Ag-110M 6.0+ 1.176E+05 249.78 d 0.01

IT:1.36; β-:98.64

4

7.223E+04 2.762E+06 LNHB

1370 47-Ag-111 0.5- 7.45 d 0.13

β-:100.00

4

3.509E+05 2.648E+04 ENSDF

1371 47-Ag-111M 3.5+ 5.982E+04 1.08 m 1.23

β-:0.50; IT:99.50

4

5.601E+04 6.878E+03 UKPADD67

1372 47-Ag-112 2.0- 3.13 h 0.29

β-:100.00

0

1.319E+06 1.319E+06 NUBASE

1373 47-Ag-113 0.5- 5.37 h 0.93

β-:98.27; β-

m:1.73

4

7.613E+05 7.154E+04 ENSDF

1374 47-Ag-113M 3.5+ 4.320E+04 1.145 m 7.28

IT:64.00; β-:36.00

4

2.211E+05 2.123E+05 ENSDF

1375 47-Ag-114 1.0+ 4.6 s 2.17

β-:100.00

2

2.150E+06 2.581E+05 ENSDF

1376 47-Ag-114M 4.0+ 1.990E+05 1.5E-03 s 3.33

IT:100.00

3

1.019E+05 9.712E+04 UKPADD67

1377 47-Ag-115 0.5- 20 m 2.50

β-:94.24; β-

m:5.76

4

1.082E+06 4.495E+05 ENSDF

1378 47-Ag-115M 3.5+ 4.110E+04 18.6 s 4.30

β-:76.70; β-

m:2.30;

IT:21.00

4

8.441E+05 4.550E+05 UKPADD67

1379 47-Ag-116 2.0- 2.68 m 3.73

β-:100.00

2

1.751E+06 2.094E+06 ENSDF

1380 47-Ag-116M 5.0+ 8.190E+04 8.6 s 3.49

β-:94.00; IT:6.00

4

1.661E+06 1.688E+06 ENSDF

1381 47-Ag-117 0.5- 1.227 m 1.90

β-:83.07; β-

m:16.93

0

1.377E+06 1.377E+06 NUBASE

1382 47-Ag-117M 3.5+ 2.860E+04 5.34 s 0.94

β-:70.72; β-

m:23.28;

IT:6.00

0

1.300E+06 1.302E+06 NUBASE

1383 47-Ag-118 1.0- 3.76 s 3.99

β-:100.00

0

2.380E+06 2.380E+06 NUBASE

1384 47-Ag-118M 4.0+ 1.275E+05 2 s 10

β-:59.00; IT:41.00

0

1.429E+06 1.481E+06 NUBASE

1385 47-Ag-119 0.5- 6 s 8.33

β-:50.00; β-

m:50.00

0

1.759E+06 1.759E+06 NUBASE

1386 47-Ag-119M 3.5+ 2.000E+04 2.1 s 4.76

β-:100.00

0

1.790E+06 1.790E+06 NUBASE

1387 47-Ag-120 3.0+ 1.23 s 3.25

β-:100.00; β-,n:~;

β-,nm:~

0

2.775E+06 2.775E+06 8.657E-01 NUBASE

1388 47-Ag-120M 6.0- 2.030E+05 0.371 s 6.47

β-:63.00; IT:37.00

0

1.791E+06 1.866E+06 NUBASE

1389 47-Ag-121 3.5+ 0.78 s 1.28

β-:89.05; β-

m:10.95

4

2.301E+06 1.167E+06 ENSDF

1390 47-Ag-122 3.0+ 0.48 s 16.67

β-:100.00

2

3.567E+06 1.081E+06 ENSDF

1391 47-Ag-122M 8.0- 8.000E+04 1.5 s 33.33

β-:100.00

0

3.193E+06 3.193E+06 NUBASE

1392 47-Ag-123 3.5+ 0.31 s 3.23

β-:81.82; β-

m:18.18

4

2.919E+06 8.440E+05 ENSDF

1393 47-Ag-124 3.0+ 0.172 s 2.91

β-:99.90; β-,n:0.05;

β-,nm:0.05

0

3.411E+06 3.411E+06 6.526E+02 NUBASE

1394 47-Ag-124M 8.0- 0.2 s 100

β-:50.00; IT:50.00

0

1.707E+06 1.707E+06 NUBASE

1395 47-Ag-125 3.5+ 0.166 s 4.22

β-:50.00; β-

m:50.00

0

2.845E+06 2.845E+06 NUBASE

1396 47-Ag-126 3.0+ 0.107 s 11.21

β-:100.00

0

3.773E+06 3.773E+06 NUBASE

1397 47-Ag-127 3.5+ 0.079 s 3.80

β-:100.00

0

3.207E+06 3.207E+06 NUBASE

1398 47-Ag-128 ? 0.058 s 8.62

β-:100.00

0

4.163E+06 4.163E+06 NUBASE

1399 47-Ag-129 3.5+ 0.044 s 15.91

β-:50.00; β-

m:50.00

0

3.583E+06 3.583E+06 NUBASE

1400 47-Ag-130 ? 0.05 s 100

β-:100.00

0

5.137E+06 5.137E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 85

MAIN DATA TABLES

Page 86: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1401 48-Cd- 95 4.5+ 5E-03 s 100

β+:100.00

0

4.467E+06 4.467E+06 NUBASE

1402 48-Cd- 96 0.0+ 1 s 100

β+m:100.00

0

2.823E+06 2.823E+06 NUBASE

1403 48-Cd- 97 4.5+ 2.8 s 21.43

β+:100.00

0

3.407E+06 3.407E+06 NUBASE

1404 48-Cd- 98 0.0+ 9.2 s 3.26

β+:100.00

4

1.035E+06 2.464E+06 ENSDF

1405 48-Cd- 99 2.5+ 16 s 18.75

β+:49.90; β+

m:49.90;

β+,p:0.21; β+,n:~;

β+,nm:~

0

2.217E+06 2.217E+06 2.186E+03 NUBASE

1406 48-Cd-100 0.0+ 49.1 s 1.02

β+:100.00

4

4.492E+05 1.630E+06 ENSDF

1407 48-Cd-101 2.5+ 1.36 m 3.68

β+:88.95; β+

m:11.05

4

9.790E+05 2.449E+06 ENSDF

1408 48-Cd-102 0.0+ 5.5 m 9.09

β+:5.77; β+

m:94.23

4

7.264E+04 8.285E+05 ENSDF

1409 48-Cd-103 2.5+ 7.3 m 1.37

β+:81.31; β+

m:18.69

0

1.372E+06 1.372E+06 NUBASE

1410 48-Cd-104 0.0+ 57.7 m 1.73

β+m:100.00

0

3.764E+05 3.764E+05 NUBASE

1411 48-Cd-105 2.5+ 55.5 m 0.72

β+:17.79; β+

m:82.21

0

9.057E+05 9.057E+05 NUBASE

1412 48-Cd-106 0.0+ 6.6E+18 y 100

2β+:100.00

0

2.770E+06 NUBASE

1413 48-Cd-107 2.5+ 6.52 h 0.31

β+:0.06; β+

m:99.94

4

6.274E+03 2.124E+04 UKPADD67

1414 48-Cd-108 0.0+ 4.1E+17 y 100

2β+:100.00

0

2.720E+05 NUBASE

1415 48-Cd-109 2.5+ 1.267 y 0.15

β+m:100.00

3

5.712E+03 1.515E+04 UKPADD67

1416 48-Cd-110 0.0+

NUBASE

1417 48-Cd-111 0.5+

NUBASE

1418 48-Cd-111M 5.5- 3.962E+05 48.54 m 0.10

IT:100.00

3

1.054E+05 2.842E+05 ENSDF

1419 48-Cd-112 0.0+

NUBASE

1420 48-Cd-113 0.5+ 7.7E+15 y 3.90

β-:100.00

1

9.330E+04 ENSDF

1421 48-Cd-113M 5.5- 2.637E+05 14.1 y 3.55

IT:0.14; β-:99.86

4

1.856E+05 7.070E+01 ENSDF

1422 48-Cd-114 0.0+ 6E+17 y 100

2β-:100.00

0

5.360E+05 ENSDF

1423 48-Cd-115 0.5+ 2.228 d 0.19

β-:~; β-

m:100.00

4

3.187E+05 1.925E+05 ENSDF

1424 48-Cd-115M 5.5- 1.810E+05 44.6 d 0.67

β-:99.99; β-

m:0.01

4

6.044E+05 3.292E+04 ENSDF

1425 48-Cd-116 0.0+ 3.4E+19 y 8.82

2β-:100.00

0

2.804E+06 ENSDF

1426 48-Cd-117 0.5+ 2.49 h 1.61

β-:8.36; β-

m:91.64

4

4.311E+05 1.078E+06 ENSDF

1427 48-Cd-117M 5.5- 1.364E+05 3.36 h 1.49

β-:98.48; β-

m:1.52

2

2.075E+05 2.034E+06 ENSDF

1428 48-Cd-118 0.0+ 50.3 m 0.40

β-:100.00

1

1.610E+05 ENSDF

1429 48-Cd-119 1.5+ 2.69 m 0.74

β-:9.72; β-

m:90.28

4

8.132E+05 1.485E+06 ENSDF

1430 48-Cd-119M 5.5- 1.465E+05 2.2 m 0.91

β-:99.78; β-

m:0.22

4

6.975E+05 2.162E+06 ENSDF

1431 48-Cd-120 0.0+ 50.8 s 0.41

β-:100.00

1

6.770E+05 ENSDF

1432 48-Cd-121 1.5+ 13.5 s 2.22

β-:32.56; β-

m:67.44

4

1.206E+06 1.662E+06 ENSDF

1433 48-Cd-121M 5.5- 2.149E+05 8.3 s 9.64

β-:100.00

4

1.191E+06 2.124E+06 ENSDF

1434 48-Cd-122 0.0+ 5.24 s 0.57

β-:100.00

1

1.247E+06 ENSDF

1435 48-Cd-123 1.5+ 2.1 s 0.95

β-:30.97; β-

m:69.03

4

1.729E+06 1.883E+06 ENSDF

1436 48-Cd-123M 5.5- 3.165E+05 1.82 s 1.65

β-:98.78; β-

m:1.22

4

1.609E+06 2.331E+06 ENSDF

1437 48-Cd-124 0.0+ 1.25 s 1.60

β-:100.00

0

1.390E+06 1.390E+06 NUBASE

1438 48-Cd-125 1.5+ 0.65 s 3.08

β-:47.86; β-

m:52.14

2

2.217E+06 1.860E+06 ENSDF

1439 48-Cd-125M 5.5- 5.000E+04 0.48 s 6.25

β-:100.00

2

2.088E+06 2.332E+06 ENSDF

1440 48-Cd-126 0.0+ 0.515 s 3.30

β-:100.00

0

1.827E+06 1.827E+06 NUBASE

1441 48-Cd-127 1.5+ 0.37 s 18.92

β-m:100.00

0

2.670E+06 2.670E+06 NUBASE

86 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 87: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1442 48-Cd-128 0.0+ 0.28 s 14.29

β-m:100.00

0

2.274E+06 2.274E+06 NUBASE

1443 48-Cd-129 1.5+ 0.242 s 3.31

β-m:100.00

0

3.120E+06 3.120E+06 NUBASE

1444 48-Cd-129M 5.5- 0.104 s 5.77

β-:100.00

0

3.247E+06 3.247E+06 NUBASE

1445 48-Cd-130 0.0+ 0.162 s 4.32

β-:96.50; β-,n:1.75;

β-,nm:1.75

0

2.703E+06 2.703E+06 2.720E+04 NUBASE

1446 48-Cd-131 3.5- 0.068 s 4.41

β-:96.50; β-,n:3.50

0

4.196E+06 4.196E+06 5.730E+04 NUBASE

1447 48-Cd-132 0.0+ 0.097 s 10.31

β-:40.00; β-,nm:60.00

0

2.909E+06 2.909E+06 1.349E+06 NUBASE

1448 49-In- 97 4.5+ 5E-03 s 100

p:50.00; β+:50.00

0

2.267E+06 2.267E+06 9.055E+05 NUBASE

1449 49-In- 98 0.0+ 0.045 s 51.11

β+:100.00

0

4.577E+06 4.577E+06 NUBASE

1450 49-In- 98M ? 1.7 s 47.06

β+:100.00

0

4.577E+06 4.577E+06 NUBASE

1451 49-In- 99 4.5+ 3.1 s 25.81

β+:100.00

0

2.860E+06 2.860E+06 NUBASE

1452 49-In- 99M 0.5- 4.000E+05 1 s 100

β+:50.00; IT:50.00

0

1.497E+06 1.697E+06 NUBASE

1453 49-In-100 6.0+ 5.9 s 3.39

β+:96.10; β+,p:1.95;

β+,pm:1.95

0

3.278E+06 3.278E+06 4.922E+04 NUBASE

1454 49-In-101 4.5+ 15.1 s 7.28

β+:100.00

0

2.380E+06 2.380E+06 NUBASE

1455 49-In-101M 0.5- 5.500E+05 10 s 100

β+:95.00; IT:5.00

0

2.435E+06 2.463E+06 NUBASE

1456 49-In-102 6.0+ 22 s 4.55

β+:100.00

4

2.719E+06 3.258E+06 ENSDF

1457 49-In-103 4.5+ 1 m 1.67

β+:100.00

0

2.017E+06 2.017E+06 NUBASE

1458 49-In-103M 0.5- 6.317E+05 34 s 5.88

β+:67.00; IT:33.00

0

1.492E+06 1.701E+06 NUBASE

1459 49-In-104 ? 1.8 m 1.67

β+:100.00

0

2.622E+06 2.622E+06 NUBASE

1460 49-In-104M 3.0+ 9.348E+04 15.7 s 3.18

IT:80.00; β+:20.00

0

5.306E+05 6.054E+05 NUBASE

1461 49-In-105 4.5+ 5.07 m 1.38

β+:100.00

4

9.830E+05 1.814E+06 ENSDF

1462 49-In-105M 0.5- 6.741E+05 48 s 12.50

IT:100.00

3

3.131E+04 6.360E+05 ENSDF

1463 49-In-106 7.0+ 6.2 m 1.61

β+:100.00

0

2.175E+06 2.175E+06 NUBASE

1464 49-In-106M 3.0+ 2.860E+04 5.2 m 1.92

β+:100.00

0

2.185E+06 2.185E+06 NUBASE

1465 49-In-107 4.5+ 32.4 m 0.93

β+:100.00

4

3.470E+05 1.498E+06 ENSDF

1466 49-In-107M 0.5- 6.785E+05 50.4 s 1.19

IT:100.00

3

3.732E+04 6.407E+05 ENSDF

1467 49-In-108 7.0+ 58 m 2.07

β+:100.00

0

1.712E+06 1.712E+06 NUBASE

1468 49-In-108M 2.0+ 2.975E+04 39.6 m 1.77

β+:100.00

0

1.722E+06 1.722E+06 NUBASE

1469 49-In-109 4.5+ 4.2 h 2.38

β+:100.00

4

3.131E+04 6.335E+05 ENSDF

1470 49-In-109M 0.5- 6.501E+05 1.34 m 5.22

IT:100.00

3

3.666E+04 6.103E+05 ENSDF

1471 49-In-109N 9.5+ 2.101E+06 0.209 s 2.87

IT:100.00

3

1.703E+04 2.085E+06 ENSDF

1472 49-In-110 7.0+ 4.9 h 2.04

β+:100.00

0

1.293E+06 1.293E+06 NUBASE

1473 49-In-110M 2.0+ 6.210E+04 1.152 h 0.72

β+:100.00

4

6.526E+05 1.572E+06 ENSDF

1474 49-In-111 4.5+ 2.805 d 0.02

β+:100.00; β+

m:0.01

4

3.251E+04 4.059E+05 LNHB

1475 49-In-111M 0.5- 5.372E+05 7.9 m 5.06

IT:100.00

3

6.784E+04 4.696E+05 UKPADD67

1476 49-In-112 1.0+ 14.7 m 4.76

β-:44.00; β+:56.00

5

2.452E+05 2.902E+05 UKPADD67

1477 49-In-112M 4.0+ 1.566E+05 20.7 m 0.48

IT:100.00

3

1.222E+05 3.456E+04 UKPADD67

1478 49-In-113 4.5+

NUBASE

1479 49-In-113M 0.5- 3.917E+05 1.658 h 0.23

IT:100.00

3

1.309E+05 2.605E+05 LNHB

1480 49-In-114 1.0+ 1.198 m 0.14

β-:99.50; β+:0.50

5

7.692E+05 4.370E+03 UKPADD67

1481 49-In-114M 5.0+ 1.903E+05 50 d 0.40

β+:3.50; IT:96.50

4

1.409E+05 8.899E+04 UKPADD67

1482 49-In-114N 8.0- 5.020E+05 0.043 s 2.33

ITm:100.00

3

3.396E+04 2.777E+05 UKPADD67

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 87

MAIN DATA TABLES

Page 88: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1483 49-In-115 4.5+ 4.41E+14 y 5.67

β-:100.00

1

1.520E+05 ENSDF

1484 49-In-115M 0.5- 3.262E+05 4.486 h 0.09

IT:95.00; β-:5.00

4

1.734E+05 1.626E+05 ENSDF

1485 49-In-116 1.0+ 14.2 s 2.11

β-:100.00

4

1.357E+06 5.265E+03 UKPADD67

1486 49-In-116M 5.0+ 1.273E+05 54.6 m 0.55

β-:100.00

4

3.126E+05 2.491E+06 UKPADD67

1487 49-In-116N 8.0- 2.897E+05 2.17 s 2.30

ITm:100.00

3

9.412E+04 6.817E+04 UKPADD67

1488 49-In-117 4.5+ 43.2 m 0.69

β-:99.66; β-

m:0.34

4

2.641E+05 6.942E+05 ENSDF

1489 49-In-117M 0.5- 3.153E+05 1.937 h 0.60

IT:47.10; β-:52.90

4

4.336E+05 9.093E+04 ENSDF

1490 49-In-118 1.0+ 5 s 6

β-:100.00

4

1.879E+06 7.782E+04 ENSDF

1491 49-In-118M 5.0+ 1.000E+05 4.45 m 1.12

β-:100.00

4

6.065E+05 2.766E+06 ENSDF

1492 49-In-118N 8.0- 2.400E+05 8.5 s 3.53

ITm:98.60; β-:1.40

0

2.178E+04 1.598E+05 NUBASE

1493 49-In-119 4.5+ 2.4 m 4.17

β-:9.66; β-

m:90.34

0

7.612E+05 7.612E+05 NUBASE

1494 49-In-119M 0.5- 3.114E+05 18 m 1.67

β-:94.40; IT:5.60

0

8.420E+05 8.594E+05 NUBASE

1495 49-In-120 1.0+ 3.08 s 2.60

β-:100.00

2

2.244E+06 2.566E+05 ENSDF

1496 49-In-120M 5.0+ 7.000E+04 46.2 s 1.73

β-:100.00

4

9.989E+05 2.985E+06 ENSDF

1497 49-In-120N 8.0- 3.000E+05 47.3 s 1.06

β-:100.00

0

1.888E+06 1.888E+06 NUBASE

1498 49-In-121 4.5+ 23.1 s 2.60

β-:88.67; β-

m:11.33

4

9.867E+05 9.229E+05 ENSDF

1499 49-In-121M 0.5- 3.136E+05 3.88 m 2.58

β-:98.80; IT:1.20

4

1.517E+06 6.329E+04 ENSDF

1500 49-In-122 1.0+ 1.5 s 20

β-:100.00

2

2.535E+06 6.311E+05 ENSDF

1501 49-In-122M 8.0- 2.000E+05 10.8 s 3.70

β-:100.00

4

1.363E+06 3.460E+06 ENSDF

1502 49-In-122N 8.0- 2.000E+05 10.8 s 3.70

β-:100.00

4

1.363E+06 3.460E+06 ENSDF

1503 49-In-123 4.5+ 5.98 s 1

β-:7.62; β-

m:92.38

4

1.406E+06 1.046E+06 ENSDF

1504 49-In-123M 0.5- 3.272E+05 47.8 s 1.05

β-:~; β-

m:100.00

4

2.032E+06 6.250E+04 ENSDF

1505 49-In-124 3.0+ 3.11 s 3.22

β-:100.00

4

2.052E+06 2.650E+06 ENSDF

1506 49-In-124M 8.0- 5.000E+04 3.7 s 5.41

β-:100.00

4

1.623E+06 3.531E+06 ENSDF

1507 49-In-125 4.5+ 2.36 s 1.69

β-:16.89; β-

m:83.11

4

1.810E+06 1.202E+06 ENSDF

1508 49-In-125M 0.5- 3.601E+05 12.2 s 1.64

β-m:100.00

0

1.917E+06 1.917E+06 NUBASE

1509 49-In-126 3.0+ 1.53 s 0.65

β-:100.00

2

2.399E+06 2.764E+06 ENSDF

1510 49-In-126M 8.0- 1.000E+05 1.64 s 3.05

β-:100.00

0

2.770E+06 2.770E+06 NUBASE

1511 49-In-127 4.5+ 1.09 s 0.92

β-:38.98; β-

m:61.02

4

2.418E+06 1.136E+06 ENSDF

1512 49-In-127M 0.5- 4.600E+05 3.67 s 1.09

β-m:99.31; β-,n:0.69

0

2.308E+06 2.308E+06 2.447E+03 NUBASE

1513 49-In-128 3.0+ 0.84 s 7.14

β-:100.00

2

2.643E+06 3.017E+06 ENSDF

1514 49-In-128M 1.0- 2.479E+05 0.01 s 70

IT:100.00

0

2.479E+05 NUBASE

1515 49-In-128N 8.0- 3.200E+05 0.72 s 13.89

β-m:100.00

0

2.401E+06 2.401E+06 NUBASE

1516 49-In-129 4.5+ 0.61 s 1.64

β-:89.35; β-

m:10.65

4

2.506E+06 1.975E+06 ENSDF

1517 49-In-129M 0.5- 3.800E+05 1.23 s 2.44

β-:99.70

4

3.469E+06 3.584E+05 ENSDF

1518 49-In-130 1.0- 0.29 s 6.90

β-:71.06; β-

m:28.94

4

2.951E+06 3.427E+06 ENSDF

1519 49-In-130M 10.0- 5.000E+04 0.54 s 1.85

β-m:100.00

4

2.825E+06 1.995E+06 ENSDF

1520 49-In-130N 5.0+ 4.000E+05 0.54 s 1.85

β-:100.00

4

3.332E+06 2.991E+06 ENSDF

1521 49-In-131 4.5+ 0.28 s 10.71

β-:94.69; β-

m:5.31

2

2.987E+06 2.413E+06 ENSDF

1522 49-In-131M 0.5- 3.500E+05 0.35 s 14.29

β-:97.98; β-,n:1.00;

β-,nm:1.00; IT:0.02

0

3.128E+06 3.128E+06 1.654E+04 NUBASE

1523 49-In-131N ? 4.100E+06 0.32 s 18.75

β-m:98.97; β-,n:0.01;

β-,nm:0.01; IT:1.00

0

4.354E+06 4.395E+06 4.940E+02 NUBASE

88 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 89: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1524 49-In-132 7.0- 0.201 s 6.47

β-:100.00

4

3.478E+06 5.704E+06 ENSDF

1525 49-In-133 4.5+ 0.165 s 1.82

β-:15.00; β-,n:85.00

0

2.893E+06 2.893E+06 2.242E+06 NUBASE

1526 49-In-133M 0.5- 3.300E+05 0.18 s 55.56

IT:100.00

0

3.300E+05 NUBASE

1527 49-In-134 ? 0.14 s 2.86

β-:31.00; β-,n:65.00;

β-,2n:4.00

0

3.376E+06 3.376E+06 1.848E+06 NUBASE

1528 49-In-135 4.5+ 0.092 s 10.87

β-:100.00

0

4.533E+06 4.533E+06 NUBASE

1529 50-Sn- 99 4.5+ 5E-03 s 100

β+:100.00

0

4.690E+06 4.690E+06 NUBASE

1530 50-Sn-100 0.0+ 1.1 s 36.36

β+:83.00; β+,p:17.00

0

2.290E+06 2.290E+06 2.457E+05 NUBASE

1531 50-Sn-101 2.5+ 3 s 33.33

β+:50.00; β+

m:50.00

0

2.925E+06 2.925E+06 NUBASE

1532 50-Sn-102 0.0+ 4.6 s 30.43

β+:100.00

0

1.927E+06 1.927E+06 NUBASE

1533 50-Sn-103 2.5+ 7 s 42.86

β+:50.00; β+

m:50.00

0

2.438E+06 2.438E+06 NUBASE

1534 50-Sn-104 0.0+ 20.8 s 2.40

β+:9.32; β+

m:90.68

4

7.262E+05 1.884E+06 ENSDF

1535 50-Sn-105 2.5+ 34 s 2.94

β+:50.00; β+

m:50.00

0

1.961E+06 1.961E+06 NUBASE

1536 50-Sn-106 0.0+ 1.917 m 4.35

β+m:100.00

4

1.096E+05 1.200E+06 ENSDF

1537 50-Sn-107 2.5+ 2.9 m 1.72

β+:50.00; β+

m:50.00

0

1.547E+06 1.547E+06 NUBASE

1538 50-Sn-108 0.0+ 10.3 m 0.78

β+m:100.00

4

3.070E+04 6.716E+05 ENSDF

1539 50-Sn-109 2.5+ 18 m 1.11

β+:69.15; β+

m:30.85

0

1.216E+06 1.216E+06 NUBASE

1540 50-Sn-110 0.0+ 4.1 h 2.44

β+m:100.00

4

1.417E+04 2.904E+05 UKPADD67

1541 50-Sn-111 3.5+ 35.3 m 1.70

β+:99.80; β+

m:0.20

0

8.166E+05 8.166E+05 NUBASE

1542 50-Sn-112 0.0+

NUBASE

1543 50-Sn-113 0.5+ 115.09 d 0.03

β+:0.01; β+

m:99.99

4

6.272E+03 2.325E+04 UKPADD67

1544 50-Sn-113M 3.5+ 7.739E+04 20.9 m 2.39

β+:8.90; IT:91.10

4

5.858E+04 1.448E+04 UKPADD67

1545 50-Sn-114 0.0+

NUBASE

1546 50-Sn-115 0.5+

NUBASE

1547 50-Sn-116 0.0+

NUBASE

1548 50-Sn-117 0.5+

NUBASE

1549 50-Sn-117M 5.5- 3.146E+05 13.6 d 0.29

IT:100.00

3

1.557E+05 1.575E+05 ENSDF

1550 50-Sn-118 0.0+

NUBASE

1551 50-Sn-119 0.5+

NUBASE

1552 50-Sn-119M 5.5- 8.953E+04 293 d 0.44

IT:100.00

3

7.826E+04 1.136E+04 UKPADD67

1553 50-Sn-120 0.0+

NUBASE

1554 50-Sn-121 1.5+ 1.126 d 0.15

β-:100.00

1

1.156E+05 ENSDF

1555 50-Sn-121M 5.5- 6.300E+03 55.001 y 9.09

β-:22.40; IT:77.60

4

3.533E+04 5.096E+03 UKPADD67

1556 50-Sn-122 0.0+

NUBASE

1557 50-Sn-123 5.5- 129.2 d 0.31

β-:100.00

4

5.228E+05 6.892E+03 ENSDF

1558 50-Sn-123M 1.5+ 2.460E+04 40.06 m 0.02

β-:100.00

4

4.785E+05 1.407E+05 ENSDF

1559 50-Sn-124 0.0+ 1E+17 y 100

2β-:100.00

0

2.288E+06 ENSDF

1560 50-Sn-125 5.5- 9.64 d 0.31

β-:100.00

4

8.034E+05 3.336E+05 ENSDF

1561 50-Sn-125M 1.5+ 2.750E+04 9.52 m 0.53

β-:100.00

4

8.063E+05 3.460E+05 ENSDF

1562 50-Sn-126 0.0+ 2.3E+05 y 6.09

β-m:33.07; β-

n:66.93

4

1.221E+05 5.665E+04 ENSDF

1563 50-Sn-127 5.5- 2.1 h 1.90

β-:100.00

0

1.067E+06 1.067E+06 NUBASE

1564 50-Sn-127M 1.5+ 4.700E+03 4.13 m 0.73

β-:100.00

0

1.069E+06 1.069E+06 NUBASE

1565 50-Sn-128 0.0+ 59.07 m 0.24

β-:100.00; β-

m:~

4

2.510E+05 6.034E+05 ENSDF

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 89

MAIN DATA TABLES N

Page 90: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1566 50-Sn-128M 7.0- 2.092E+06 6.5 s 7.69

IT:100.00

3

7.860E+04 2.012E+06 ENSDF

1567 50-Sn-129 1.5+ 2.23 m 1.35

β-:100.00

4

1.098E+06 1.350E+06 UKPADD67

1568 50-Sn-129M 5.5- 3.520E+04 7.2 m 4.17

β-m:31.00; β-:69.00

4

7.055E+05 1.707E+06 UKPADD67

1569 50-Sn-130 0.0+ 3.73 m 1.88

β-m:100.00

4

4.621E+05 9.376E+05 UKPADD67

1570 50-Sn-130M 7.0- 1.947E+06 1.7 m 5.88

β-m:16.00; β-:84.00

4

1.388E+06 8.130E+05 UKPADD67

1571 50-Sn-131 1.5+ 56 s 0.89

β-:100.00

0

1.558E+06 1.558E+06 NUBASE

1572 50-Sn-131M 5.5- 8.000E+04 58.4 s 0.86

β-:100.00; IT:~

0

1.585E+06 1.585E+06 NUBASE

1573 50-Sn-132 0.0+ 39.7 s 1.26

β-:100.00; β-

m:~

4

6.987E+05 1.301E+06 ENSDF

1574 50-Sn-133 3.5- 1.45 s 2.07

β-:100.00

2

3.396E+06 2.725E+05 ENSDF

1575 50-Sn-134 0.0+ 1.05 s 1.05

β-:83.00; β-,n:17.00

0

2.212E+06 2.212E+06 1.730E+05 NUBASE

1576 50-Sn-135 3.5- 0.53 s 3.77

β-:79.00; β-,n:10.50;

β-,nm:10.50

0

2.622E+06 2.622E+06 2.761E+05 NUBASE

1577 50-Sn-136 0.0+ 0.25 s 12

β-:70.00; β-,n:30.00

0

2.341E+06 2.341E+06 3.854E+05 NUBASE

1578 50-Sn-137 2.5- 0.19 s 31.58

β-:42.00; β-,n:58.00

0

2.335E+06 2.335E+06 9.423E+05 NUBASE

1579 51-Sb-103 2.5+ 0.1 s 100

β+:100.00

0

3.597E+06 3.597E+06 NUBASE

1580 51-Sb-104 ? 0.47 s 27.66

β+:39.50; β+,p:3.50;

β+,pm:3.50; p:7.00;

α:46.50

0

1.771E+06 1.771E+06 1.365E+06 NUBASE

1581 51-Sb-105 2.5+ 1.12 s 14.29

β+:99.00; p:1.00

0

3.115E+06 3.115E+06 4.810E+03 NUBASE

1582 51-Sb-106 4.0+ 0.6 s 33.33

β+:100.00

0

3.700E+06 3.700E+06 NUBASE

1583 51-Sb-107 2.5+ 4.6 s 17.39

β+:100.00

0

2.643E+06 2.643E+06 NUBASE

1584 51-Sb-108 4.0+ 7.4 s 4.05

β+:100.00

0

3.177E+06 3.177E+06 NUBASE

1585 51-Sb-109 2.5+ 16.67 s 0.90

β+:100.00

4

1.950E+06 1.894E+06 ENSDF

1586 51-Sb-110 4.0+ 23 s 1.74

β+:100.00

4

1.961E+06 3.692E+06 ENSDF

1587 51-Sb-111 2.5+ 1.25 m 1.33

β+:100.00

4

1.352E+06 1.475E+06 ENSDF

1588 51-Sb-112 3.0+ 51.4 s 1.95

β+:100.00

4

1.754E+06 2.755E+06 ENSDF

1589 51-Sb-113 2.5+ 6.67 m 1.05

β+:80.20; β+

m:19.80

0

1.299E+06 1.299E+06 NUBASE

1590 51-Sb-114 3.0+ 3.49 m 0.86

β+:100.00

4

1.152E+06 2.632E+06 ENSDF

1591 51-Sb-115 2.5+ 32.1 m 0.93

β+:100.00

4

2.333E+05 8.875E+05 ENSDF

1592 51-Sb-116 3.0+ 15.8 m 5.06

β+:100.00

4

5.217E+05 2.287E+06 ENSDF

1593 51-Sb-116M 8.0- 3.830E+05 1.005 h 1

β+:100.00

4

2.142E+05 3.187E+06 ENSDF

1594 51-Sb-117 2.5+ 2.8 h 0.36

β+:100.00

4

2.813E+04 1.848E+05 ENSDF

1595 51-Sb-118 1.0+ 3.6 m 2.78

β+:100.00

4

8.731E+05 8.041E+05 ENSDF

1596 51-Sb-118M 8.0- 2.500E+05 5 h 0.40

β+:100.00

4

3.519E+04 2.599E+06 ENSDF

1597 51-Sb-119 2.5+ 1.596 d 0.52

β+:100.00

4

2.597E+04 2.342E+04 UKPADD67

1598 51-Sb-119M 13.5+ 2.852E+06 0.85 s 10.59

IT:100.00

0

2.852E+06 NUBASE

1599 51-Sb-120 1.0+ 15.9 m 0.63

β+:100.00

4

3.068E+05 4.600E+05 UKPADD67

1600 51-Sb-120M 8.0- 2.000E+05 5.76 d 0.52

β+:100.00

4

4.505E+04 2.462E+06 UKPADD67

1601 51-Sb-121 2.5+

NUBASE

1602 51-Sb-122 2.0- 2.7 d 0.37

β+:2.60; β-:97.40

5

5.626E+05 4.429E+05 LNHB

1603 51-Sb-122M 8.0- 1.636E+05 4.19 m 2.15

IT:100.00

3

9.306E+04 7.053E+04 UKPADD67

1604 51-Sb-123 3.5+

NUBASE

1605 51-Sb-124 3.0- 60.2 d 0.05

β-:100.00

4

3.921E+05 1.840E+06 LNHB

90 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 91: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1606 51-Sb-124M 5.0+ 1.086E+04 1.55 m 5.38

β-:25.00; IT:75.00

4

1.141E+05 4.375E+05 UKPADD67

1607 51-Sb-124N 8.0- 3.685E+04 20.2 m 0.99

ITm:100.00

3

2.577E+04 3.380E+02 UKPADD67

1608 51-Sb-125 3.5+ 2.759 y 0.01

β-:77.62; β-

m:22.38

4

1.002E+05 4.370E+05 ENSDF

1609 51-Sb-126 8.0- 12.4 d 0.81

β-:100.00

4

3.367E+05 2.777E+06 LNHB

1610 51-Sb-126M 5.0+ 1.770E+04 19.1 m 1.05

IT:14.00; β-:86.00

4

6.248E+05 1.576E+06 UKPADD67

1611 51-Sb-126N 3.0- 4.040E+04 11 s 18.18

ITm:100.00

3

2.244E+04 3.785E+02 UKPADD67

1612 51-Sb-127 3.5+ 3.85 d 1.30

β-:83.52; β-

m:16.48

4

3.129E+05 6.921E+05 ENSDF

1613 51-Sb-128 8.0- 9.01 h 0.33

β-:100.00

4

4.777E+05 3.048E+06 ENSDF

1614 51-Sb-128M 5.0+ 1.000E+04 10.4 m 1.92

IT:3.60; β-:96.40

2

9.448E+05 1.881E+06 ENSDF

1615 51-Sb-129 3.5+ 4.36 h 0.69

β-:83.40; β-

m:16.60

4

3.548E+05 1.380E+06 UKPADD67

1616 51-Sb-129M 9.5- 1.851E+06 17.7 m 0.56

β-:2.00; β-

m:83.00;

IT:15.00

4

9.989E+05 1.478E+06 UKPADD67

1617 51-Sb-130 8.0- 39.5 m 2.03

β-:100.00

4

7.139E+05 3.126E+06 ENSDF

1618 51-Sb-130M ? 4.800E+03 6.3 m 3.17

β-:100.00

0

1.688E+06 1.688E+06 NUBASE

1619 51-Sb-131 3.5+ 23.03 m 0.17

β-:91.99; β-

m:8.01

4

5.762E+05 1.736E+06 ENSDF

1620 51-Sb-132 4.0+ 2.79 m 1.79

β-:100.00

4

1.255E+06 2.496E+06 ENSDF

1621 51-Sb-132M 8.0- 2.000E+05 4.1 m 1.71

β-:100.00

4

1.276E+06 2.408E+06 ENSDF

1622 51-Sb-133 3.5+ 2.5 m 4

β-:82.71; β-

m:17.29

2

6.571E+05 2.184E+06 ENSDF

1623 51-Sb-134 0.0- 0.78 s 7.69

β-:100.00

4

3.743E+06 6.465E+04 ENSDF

1624 51-Sb-134M 7.0- 8.000E+04 10.07 s 0.50

β-:99.91; β-,n:0.05;

β-,nm:0.05

0

2.821E+06 2.821E+06 1.403E+02 NUBASE

1625 51-Sb-135 3.5+ 1.74 s 1.72

β-:84.30; β-,n:15.70

5

2.967E+06 6.881E+05 1.771E+05 UKPADD67

1626 51-Sb-136 1.0- 0.923 s 1.52

β-:83.42; β-,n:16.30;

β-,2n:0.28

0

2.855E+06 2.855E+06 1.999E+05 NUBASE

1627 51-Sb-137 3.5+ 0.45 s 11.11

β-:51.00; β-,n:49.00

0

2.328E+06 2.328E+06 7.471E+05 NUBASE

1628 51-Sb-138 2.0- 0.5 s 100

β-:100.00

0

3.593E+06 3.593E+06 NUBASE

1629 51-Sb-139 3.5+ 0.3 s 100

β-:100.00

0

3.493E+06 3.493E+06 NUBASE

1630 52-Te-105 2.5+ 1E-06 s 100

α:50.00; β+:50.00

0

1.887E+06 1.887E+06 2.318E+06 NUBASE

1631 52-Te-106 0.0+ 6E-05 s 50

α:100.00

1

4.290E+06 ENSDF

1632 52-Te-107 2.5+ 3.1E-03 s 3.23

α:70.00; β+:30.00

0

1.011E+06 1.011E+06 2.804E+06 NUBASE

1633 52-Te-108 0.0+ 2.1 s 4.76

β+:48.54; α:49.00;

β+,p:2.40; β+,n:0.03;

β+,nm:0.03

0

1.133E+06 1.133E+06 1.723E+06 NUBASE

1634 52-Te-109 2.5+ 4.6 s 6.52

β+:86.69; α:3.90;

β+,p:9.40; β+,n:~;

β+,nm:~

0

2.667E+06 2.667E+06 2.937E+05 NUBASE

1635 52-Te-110 0.0+ 18.6 s 4.30

β+:100.00; α:~

0

1.753E+06 1.753E+06 8.175E+01 NUBASE

1636 52-Te-111 2.5+ 19.3 s 2.07

β+:100.00

0

2.469E+06 2.469E+06 NUBASE

1637 52-Te-112 0.0+ 2 m 10

β+:100.00

0

1.434E+06 1.434E+06 NUBASE

1638 52-Te-113 3.5+ 1.7 m 11.76

β+:100.00

4

1.683E+06 1.888E+06 ENSDF

1639 52-Te-114 0.0+ 15.2 m 4.61

β+:100.00

4

1.789E+05 1.086E+06 ENSDF

1640 52-Te-115 3.5+ 5.8 m 3.45

β+:100.00

4

6.395E+05 2.019E+06 ENSDF

1641 52-Te-115M 0.5+ 2.000E+04 6.7 m 5.97

β+:100.00

4

5.029E+05 2.088E+06 ENSDF

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 91

MAIN DATA TABLES

Page 92: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1642 52-Te-116 0.0+ 2.49 h 1.61

β+:100.00

4

5.823E+04 1.128E+05 ENSDF

1643 52-Te-117 0.5+ 1.033 h 3.23

β+:100.00

4

2.114E+05 1.540E+06 ENSDF

1644 52-Te-117M 5.5- 2.961E+05 0.103 s 2.91

IT:100.00

3

3.421E+04 2.650E+05 ENSDF

1645 52-Te-118 0.0+ 6 d 0.33

β+:100.00

3

4.964E+03 1.988E+04 ENSDF

1646 52-Te-119 0.5+ 16.05 h 0.31

β+:100.00

4

1.304E+04 7.669E+05 ENSDF

1647 52-Te-119M 5.5- 2.610E+05 4.7 d 0.85

β+:100.00

4

1.654E+04 1.498E+06 ENSDF

1648 52-Te-120 0.0+

NUBASE

1649 52-Te-121 0.5+ 19.16 d 0.26

β+:100.00

4

9.840E+03 5.775E+05 UKPADD67

1650 52-Te-121M 5.5- 2.940E+05 154 d 4.55

β+:11.30; IT:88.70

4

8.009E+04 2.169E+05 UKPADD67

1651 52-Te-122 0.0+

NUBASE

1652 52-Te-123 0.5+ 9.2E+16 y 100

β+:100.00

3

2.002E+03 2.595E+02 ENSDF

1653 52-Te-123M 5.5- 2.474E+05 119.5 d 0.08

IT:100.00

3

9.604E+04 1.477E+05 LNHB

1654 52-Te-124 0.0+

NUBASE

1655 52-Te-125 0.5+

NUBASE

1656 52-Te-125M 5.5- 1.448E+05 57.4 d 0.26

IT:100.00

3

1.053E+05 3.513E+04 LNHB

1657 52-Te-126 0.0+

NUBASE

1658 52-Te-127 1.5+ 9.35 h 0.64

β-:100.00

4

2.244E+05 4.847E+03 UKPADD67

1659 52-Te-127M 5.5- 8.826E+04 109 d 1.83

IT:97.60; β-:2.40

4

8.214E+04 1.158E+04 UKPADD67

1660 52-Te-128 0.0+ 2.2E+24 y 13.64

2β-:100.00

0

8.672E+05 ENSDF

1661 52-Te-129 1.5+ 1.16 h 0.29

β-:100.00

4

5.428E+05 6.237E+04 ENSDF

1662 52-Te-129M 5.5- 1.055E+05 33.6 d 0.30

β-:37.00; IT:63.00

4

2.630E+05 3.766E+04 ENSDF

1663 52-Te-130 0.0+ 7.9E+23 y 12.66

2β-:100.00

0

2.528E+06 ENSDF

1664 52-Te-131 1.5+ 25 m 0.40

β-:100.00

4

7.369E+05 4.457E+05 LNHB

1665 52-Te-131M 5.5- 1.823E+05 1.25 d 0.64

IT:21.00; β-:79.00

4

1.932E+05 1.456E+06 LNHB

1666 52-Te-132 0.0+ 3.204 d 0.41

β-:100.00

4

1.014E+05 2.340E+05 ENSDF

1667 52-Te-133 1.5+ 12.45 m 2.41

β-:100.00

4

6.780E+05 1.182E+06 LNHB

1668 52-Te-133M 5.5- 3.343E+05 55.4 m 0.72

β-:82.50; IT:17.50

4

3.761E+05 1.823E+06 ENSDF

1669 52-Te-134 0.0+ 41.8 m 1.91

β-:100.00

4

2.248E+05 8.773E+05 LNHB

1670 52-Te-135 3.5- 19 s 1.05

β-:100.00

2

2.442E+06 3.844E+05 ENSDF

1671 52-Te-136 0.0+ 17.5 s 1.14

β-:100.00

4

1.302E+06 1.987E+06 ENSDF

1672 52-Te-137 1.5- 2.49 s 2.01

β-:97.01; β-,n:1.49;

β-,nm:1.49

0

2.257E+06 2.257E+06 1.154E+04 NUBASE

1673 52-Te-138 0.0+ 1.4 s 28.57

β-:93.70; β-,n:6.30

0

2.038E+06 2.038E+06 3.940E+04 NUBASE

1674 52-Te-139 2.5- 0.5 s 100

β-:100.00

0

2.680E+06 2.680E+06 NUBASE

1675 52-Te-140 0.0+ 0.3 s 100

β-:100.00

0

2.437E+06 2.437E+06 NUBASE

1676 52-Te-141 2.5- 0.1 s 100

β-:100.00

0

2.987E+06 2.987E+06 NUBASE

1677 52-Te-142 0.0+ 0.05 s 100

β-:100.00

0

2.763E+06 2.763E+06 NUBASE

1678 53-I -108 1.0+ 0.036 s 16.67

α:90.00; β+:9.00;

p:1.00

0

3.921E+05 3.921E+05 3.701E+06 NUBASE

1679 53-I -109 2.5+ 1.03E-04 s 4.85

p:100.00

0

8.210E+05 NUBASE

1680 53-I -110 1.0+ 0.65 s 3.08

β+:70.90; α:17.00;

β+,p:11.00; β+,n:1.10

0

3.105E+06 3.105E+06 8.877E+05 NUBASE

1681 53-I -111 2.5+ 2.5 s 8

β+:99.91; α:0.09

0

2.841E+06 2.841E+06 2.882E+03 NUBASE

92 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 93: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1682 53-I -112 1.0+ 3.42 s 3.22

β+:99.02; α:~;

β+,p:0.88; β+,n:0.10

0

3.384E+06 3.384E+06 1.746E+04 NUBASE

1683 53-I -113 2.5+ 6.6 s 3.03

β+:100.00; α:~

0

2.406E+06 2.406E+06 8.951E-03 NUBASE

1684 53-I -114 1.0+ 2.1 s 9.52

β+:100.00

0

3.030E+06 3.030E+06 NUBASE

1685 53-I -114M ? 2.659E+05 6.2 s 8.06

β+:91.00; IT:9.00

0

2.838E+06 2.862E+06 NUBASE

1686 53-I -115 2.5+ 1.3 m 15.38

β+:50.00; β+

m:50.00

0

1.907E+06 1.907E+06 NUBASE

1687 53-I -116 1.0+ 2.91 s 5.15

β+:100.00

0

2.593E+06 2.593E+06 NUBASE

1688 53-I -117 2.5+ 2.22 m 1.80

β+:50.00; β+

m:50.00

0

1.505E+06 1.505E+06 NUBASE

1689 53-I -118 2.0- 13.7 m 3.65

β+:100.00

4

2.107E+06 1.961E+06 ENSDF

1690 53-I -118M 7.0- 1.901E+05 8.5 m 5.88

β+:100.00

4

1.148E+06 3.701E+06 ENSDF

1691 53-I -119 2.5+ 19.1 m 2.09

β+:99.05; β+

m:0.95

4

4.829E+05 8.780E+05 ENSDF

1692 53-I -120 2.0- 1.36 h 0.25

β+:100.00

4

1.168E+06 2.099E+06 ENSDF

1693 53-I -120M 7.0- 3.200E+05 53 m 7.55

β+:100.00

0

1.978E+06 1.978E+06 NUBASE

1694 53-I -121 2.5+ 2.12 h 0.47

β+:99.71; β+

m:0.29

4

6.716E+04 3.966E+05 ENSDF

1695 53-I -122 1.0+ 3.63 m 1.65

β+:100.00

4

1.107E+06 9.616E+05 ENSDF

1696 53-I -123 2.5+ 13.223 h 0.03

β+:100.00

4

2.621E+04 1.719E+05 LNHB

1697 53-I -124 2.0- 4.176 d 0.01

β+:100.00

4

1.924E+05 1.111E+06 ENSDF

1698 53-I -125 2.5+ 59.407 d 0.02

β+:100.00

4

1.648E+04 4.224E+04 LNHB

1699 53-I -126 2.0- 12.98 d 0.39

β-:43.70; β+:56.30

5

1.438E+05 4.356E+05 UKPADD67

1700 53-I -127 2.5+

NUBASE

1701 53-I -128 1.0+ 24.99 m 0.08

β+:6.90; β-:93.10

5

7.401E+05 8.609E+04 LNHB

1702 53-I -129 3.5+ 1.61E+07 y 4.35

β-:100.00

4

6.233E+04 2.451E+04 LNHB

1703 53-I -130 5.0+ 12.36 h 0.08

β-:100.00

4

2.789E+05 2.136E+06 ENSDF

1704 53-I -130M 2.0+ 3.995E+04 8.84 m 0.68

IT:84.00; β-:16.00

0

1.594E+05 1.930E+05 NUBASE

1705 53-I -131 3.5+ 8.023 d 0.02

β-:98.91; β-

m:1.09

4

1.924E+05 3.815E+05 LNHB

1706 53-I -132 4.0+ 2.295 h 0.57

β-:100.00

4

4.968E+05 2.255E+06 ENSDF

1707 53-I -132M 8.0- 1.200E+05 1.383 h 1.20

IT:86.00; β-:14.00

4

1.627E+05 3.448E+05 UKPADD67

1708 53-I -133 3.5+ 20.8 h 0.48

β-:97.15; β-

m:2.85

4

4.089E+05 6.115E+05 ENSDF

1709 53-I -133M 9.5- 1.632E+06 9 s 22.22

IT:100.00

3

4.908E+04 1.581E+06 ENSDF

1710 53-I -134 4.0+ 52.5 m 0.38

β-:100.00

4

6.232E+05 2.523E+06 ENSDF

1711 53-I -134M 8.0- 3.165E+05 3.6 m 2.78

IT:97.70; β-

m:2.30

4

8.671E+04 2.425E+05 ENSDF

1712 53-I -135 3.5+ 6.57 h 0.30

β-:83.49; β-

m:16.51

4

3.663E+05 1.578E+06 ENSDF

1713 53-I -136 1.0- 1.39 m 1.20

β-:100.00

4

1.986E+06 2.349E+06 ENSDF

1714 53-I -136M 6.0- 6.500E+05 46.9 s 2.13

β-:100.00

0

2.525E+06 2.525E+06 NUBASE

1715 53-I -137 3.5+ 24.51 s 0.24

β-:93.50; β-,n:6.50

5

1.862E+06 1.220E+06 3.938E+04 UKPADD67

1716 53-I -138 2.0- 6.46 s 0.93

β-:94.70; β-,n:5.30

5

2.720E+06 1.325E+06 5.288E+03 UKPADD67

1717 53-I -139 3.5+ 2.3 s 1.30

β-:90.20; β-,n:9.80

5

2.533E+06 6.723E+05 1.112E+04 UKPADD67

1718 53-I -140 3.0- 0.86 s 4.65

β-:90.70; β-,n:9.30

0

2.713E+06 2.713E+06 7.679E+04 NUBASE

1719 53-I -141 3.5+ 0.43 s 4.65

β-:79.00; β-,n:21.00

0

2.288E+06 2.288E+06 2.309E+05 NUBASE

1720 53-I -142 2.0- 0.2 s 100

β-:75.00; β-,n:25.00

0

2.724E+06 2.724E+06 2.837E+05 NUBASE

1721 53-I -143 3.5+ 0.1 s 100

β-:60.00; β-,n:40.00

0

2.339E+06 2.339E+06 5.769E+05 NUBASE

1722 53-I -144 1.0- 0.05 s 100

β-:60.00; β-,n:40.00

0

2.720E+06 2.720E+06 5.799E+05 NUBASE

1723 54-Xe-110 0.0+ 0.31 s 61.29

α:64.00; β+:36.00

0

1.010E+06 1.010E+06 2.486E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 93

MAIN DATA TABLES

Page 94: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1724 54-Xe-111 2.5+ 0.74 s 27.03

β+:90.00; α:10.00

0

3.165E+06 3.165E+06 3.715E+05 NUBASE

1725 54-Xe-112 0.0+ 2.7 s 29.63

β+:99.10; α:0.90

0

2.355E+06 2.355E+06 2.993E+04 NUBASE

1726 54-Xe-113 2.5+ 2.74 s 2.92

β+:92.98; α:0.01;

β+,p:7.00; β+,n:0.01

0

2.941E+06 2.941E+06 1.392E+05 NUBASE

1727 54-Xe-114 0.0+ 10 s 4

β+:100.00

0

1.905E+06 1.905E+06 NUBASE

1728 54-Xe-115 2.5+ 18 s 22.22

β+:99.66; β+,p:0.34;

β+,n:~

0

2.557E+06 2.557E+06 5.059E+03 NUBASE

1729 54-Xe-116 0.0+ 59 s 3.39

β+:100.00

0

1.481E+06 1.481E+06 NUBASE

1730 54-Xe-117 2.5+ 1.017 m 3.28

β+:100.00; β+,p:~

0

2.083E+06 2.083E+06 2.751E+01 NUBASE

1731 54-Xe-118 0.0+ 3.8 m 23.68

β+:100.00

0

9.640E+05 9.640E+05 NUBASE

1732 54-Xe-119 2.5+ 5.8 m 5.17

β+:100.00

0

1.657E+06 1.657E+06 NUBASE

1733 54-Xe-120 0.0+ 40 m 2.50

β+:100.00

4

5.087E+04 4.239E+05 ENSDF

1734 54-Xe-121 2.5+ 40.1 m 0.50

β+:100.00

4

5.434E+05 1.400E+06 ENSDF

1735 54-Xe-122 0.0+ 20.1 h 0.50

β+:100.00

4

8.675E+03 6.820E+04 ENSDF

1736 54-Xe-123 0.5+ 2.08 h 0.96

β+:100.00

4

1.822E+05 6.372E+05 ENSDF

1737 54-Xe-124 0.0+ 2E+14 y 100

2β+:100.00

0

2.864E+06 NUBASE

1738 54-Xe-125 0.5+ 16.9 h 1.18

β+:100.00

4

3.451E+04 2.705E+05 UKPADD67

1739 54-Xe-125M 4.5- 2.526E+05 56 s 5.36

IT:100.00

3

1.364E+05 1.161E+05 UKPADD67

1740 54-Xe-126 0.0+

NUBASE

1741 54-Xe-127 0.5+ 36.4 d 0.27

β+:100.00

4

2.987E+04 2.806E+05 LNHB

1742 54-Xe-127M 4.5- 2.971E+05 1.16 m 1.29

IT:100.00

3

1.287E+05 1.685E+05 UKPADD67

1743 54-Xe-128 0.0+

NUBASE

1744 54-Xe-129 0.5+

NUBASE

1745 54-Xe-129M 5.5- 2.361E+05 8.88 d 0.23

IT:100.00

3

1.814E+05 5.122E+04 ENSDF

1746 54-Xe-130 0.0+

NUBASE

1747 54-Xe-131 1.5+

NUBASE

1748 54-Xe-131M 5.5- 1.639E+05 11.93 d 0.13

IT:100.00

3

1.424E+05 2.007E+04 LNHB

1749 54-Xe-132 0.0+

NUBASE

1750 54-Xe-132M 10.0+ 2.752E+06 8.39E-03 s 1.31

IT:100.00

3

5.330E+04 2.709E+06 ENSDF

1751 54-Xe-133 1.5+ 5.244 d 0.08

β-:100.00

4

1.335E+05 4.612E+04 LNHB

1752 54-Xe-133M 5.5- 2.332E+05 2.188 d 0.50

IT:100.00

3

1.895E+05 4.160E+04 LNHB

1753 54-Xe-134 0.0+ 1.1E+16 y 100

2β-:100.00

0

8.300E+05 ENSDF

1754 54-Xe-134M 7.0- 1.966E+06 0.29 s 5.86

IT:100.00

3

6.794E+04 1.901E+06 ENSDF

1755 54-Xe-135 1.5+ 9.14 h 0.22

β-:100.00

4

3.150E+05 2.482E+05 ENSDF

1756 54-Xe-135M 5.5- 5.266E+05 15.29 m 0.33

IT:99.40; β-:0.60

4

9.369E+04 4.256E+05 ENSDF

1757 54-Xe-136 0.0+ 2.1E+20 y 100

2β-:100.00

0

2.467E+06 ENSDF

1758 54-Xe-137 3.5- 3.818 m 0.34

β-:100.00

4

1.695E+06 1.905E+05 ENSDF

1759 54-Xe-138 0.0+ 14.08 m 0.57

β-:100.00

4

6.419E+05 1.124E+06 ENSDF

1760 54-Xe-139 1.5- 39.68 s 0.35

β-:100.00

0

1.686E+06 1.686E+06 NUBASE

1761 54-Xe-140 0.0+ 13.6 s 0.74

β-:100.00

0

1.354E+06 1.354E+06 NUBASE

1762 54-Xe-141 2.5- 1.73 s 0.58

β-:99.96; β-,n:0.04

0

2.048E+06 2.048E+06 7.147E+01 NUBASE

1763 54-Xe-142 0.0+ 1.22 s 1.64

β-:99.64; β-,n:0.36

0

1.673E+06 1.673E+06 8.331E+02 NUBASE

1764 54-Xe-143 2.5- 0.511 s 1.17

β-:99.00; β-,n:1.00

0

2.388E+06 2.388E+06 4.984E+03 NUBASE

94 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 95: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1765 54-Xe-144 0.0+ 0.388 s 1.80

β-:97.00; β-,n:3.00

0

1.954E+06 1.954E+06 1.740E+04 NUBASE

1766 54-Xe-145 1.5- 0.188 s 2.13

β-:95.00; β-,n:2.50;

β-,nm:2.50

0

2.557E+06 2.557E+06 3.686E+04 NUBASE

1767 54-Xe-146 0.0+ 0.146 s 4.11

β-:93.10; β-,n:6.90

0

2.214E+06 2.214E+06 5.720E+04 NUBASE

1768 54-Xe-147 1.5- 0.13 s 61.54

β-:96.00; β-,n:4.00

0

2.846E+06 2.846E+06 4.289E+04 NUBASE

1769 55-Cs-112 1.0+ 5E-04 s 20

p:100.00

0

8.210E+05 NUBASE

1770 55-Cs-113 2.5+ 1.67E-05 s 4.19

p:100.00

0

9.810E+05 NUBASE

1771 55-Cs-114 1.0+ 0.57 s 3.51

β+:91.09; β+,p:8.70;

β+,n:0.19; α:0.02

0

4.019E+06 4.019E+06 2.102E+05 NUBASE

1772 55-Cs-115 4.5+ 1.4 s 57.14

β+:99.93; β+,p:0.03;

β+,pm:0.03

0

2.985E+06 2.985E+06 9.937E+02 NUBASE

1773 55-Cs-116 1.0+ 0.7 s 5.71

β+:99.67; β+,p:0.28;

β+,n:0.05

0

3.653E+06 3.653E+06 6.454E+03 NUBASE

1774 55-Cs-116M ? 1.000E+05 3.85 s 3.38

β+:99.48; β+,p:0.51;

β+,n:0.01

0

3.682E+06 3.682E+06 9.284E+03 NUBASE

1775 55-Cs-117 4.5+ 8.4 s 7.14

β+:100.00

0

2.582E+06 2.582E+06 NUBASE

1776 55-Cs-117M 1.5+ 1.500E+05 6.5 s 6.15

β+:100.00

0

2.632E+06 2.632E+06 NUBASE

1777 55-Cs-118 ? 14 s 14.29

β+:99.98; β+,p:0.02;

β+,n:~

0

3.223E+06 3.223E+06 2.819E+02 NUBASE

1778 55-Cs-118M 7.0- 1.000E+05 17 s 17.65

β+:99.98; β+,p:0.02;

β+,n:~

0

3.256E+06 3.256E+06 2.874E+02 NUBASE

1779 55-Cs-119 4.5+ 43 s 0.47

β+:100.00; β+,n:~;

β+,nm:~

0

2.163E+06 2.163E+06 3.664E-02 NUBASE

1780 55-Cs-119M 1.5+ 5.000E+04 30.4 s 0.33

β+:100.00

0

2.180E+06 2.180E+06 NUBASE

1781 55-Cs-120 2.0+ 1.02 m 2.94

β+:100.00; β+,n:~;

β+,p:~

0

2.761E+06 2.761E+06 4.930E-01 NUBASE

1782 55-Cs-120M 7.0- 1.000E+05 57 s 10.53

β+:100.00; β+,n:~;

β+,p:~

0

2.794E+06 2.794E+06 4.998E-01 NUBASE

1783 55-Cs-121 1.5+

2.583 m 2.58

β+:100.00

4

1.736E+06

1.067E+06

ENSDF

1784 55-Cs-121M 4.5+ 6.850E+04

2.033 m 2.46

β+:83.00; IT:17.00

0

1.505E+06

1.517E+06

NUBASE

1785 55-Cs-122 1.0+

21.2 s 0.94

β+:100.00

4

2.518E+06

1.298E+06

ENSDF

1786 55-Cs-122M 8.0- 1.260E+05

3.7 m 2.97

β+:100.00

0

2.447E+06

2.447E+06

NUBASE

1787 55-Cs-122N 5.0- 1.270E+05

0.36 s 5.56

IT:50.00; ITm:50.00

0

6.400E+04

NUBASE

1788 55-Cs-123 0.5+

5.91 m 0.85

β+:100.00

4

9.424E+05

1.068E+06

UKPADD67

1789 55-Cs-123M 5.5- 1.563E+05

1.7 s 11.76

IT:100.00

3

1.121E+05

4.413E+04

UKPADD67

1790 55-Cs-124 1.0+

30.9 s 1.29

β+:100.00

0

1.976E+06

1.976E+06

NUBASE

1791 55-Cs-124M 7.0+ 4.626E+05

6.3 s 3.17

IT:100.00

0

4.626E+05

NUBASE

1792 55-Cs-125 0.5+

46.7 m 0.21

β+:100.00

4

3.497E+05

6.888E+05

ENSDF

1793 55-Cs-125M 5.5- 2.666E+05

0.9 s 3.33

IT:100.00

0

2.666E+05

NUBASE

1794 55-Cs-126 1.0+

1.64 m 1.22

β+:100.00

4

1.318E+06

1.140E+06

ENSDF

1795 55-Cs-127 0.5+

6.25 h 1.60

β+:100.00

4

2.774E+04

4.312E+05

ENSDF

1796 55-Cs-128 1.0+

3.62 m 0.55

β+:100.00

4

8.748E+05

8.917E+05

ENSDF

1797 55-Cs-129 0.5+

1.342 d 0.62

β+:100.00

4

1.742E+04

2.832E+05

UKPADD67

1798 55-Cs-130 1.0+

29.21 m 0.14

β+:98.40; β-:1.60

5

3.867E+05

5.028E+05

ENSDF

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 95

MAIN DATA TABLES

Page 96: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1799 55-Cs-130M 5.0- 1.632E+05 3.46 m 1.73

IT:99.84; β+:0.16

0

1.677E+03 1.647E+05 NUBASE

1800 55-Cs-131 2.5+ 9.69 d 0.21

β+:100.00

3

6.370E+03 2.312E+04 UKPADD67

1801 55-Cs-132 2.0+ 6.53 d 0.31

β-:1.80; β+:98.20

5

1.411E+04 7.152E+05 UKPADD67

1802 55-Cs-133 3.5+

NUBASE

1803 55-Cs-134 4.0+ 2.065 y 0.03

β+:~; β-:100.00

5

1.636E+05 1.555E+06 LNHB

1804 55-Cs-134M 8.0- 1.387E+05 2.908 h 0.10

IT:100.00

3

1.118E+05 2.708E+04 UKPADD67

1805 55-Cs-135 3.5+ 2.3E+06 y 13.04

β-:100.00

1

7.590E+04 ENSDF

1806 55-Cs-135M 9.5- 1.633E+06 53 m 3.77

IT:100.00

3

3.370E+04 1.600E+06 ENSDF

1807 55-Cs-136 5.0+ 13.03 d 0.54

β-:100.00

4

1.419E+05 2.146E+06 UKPADD67

1808 55-Cs-136M 8.0- 6.000E+05 19 s 10.53

β-:50.00; IT:50.00

0

6.167E+05 6.167E+05 UKPADD67

1809 55-Cs-137 3.5+ 30.041 y 0.10

β-:5.60; β-

m:94.40

2

1.879E+05 1.644E+00 ENSDF

1810 55-Cs-138 3.0- 33.41 m 0.54

β-:100.00

4

1.244E+06 2.355E+06 ENSDF

1811 55-Cs-138M 6.0- 7.990E+04 2.91 m 2.75

IT:81.00; β-:19.00

4

3.239E+05 4.148E+05 ENSDF

1812 55-Cs-139 3.5+ 9.27 m 0.54

β-:100.00

4

1.671E+06 3.050E+05 ENSDF

1813 55-Cs-140 1.0- 1.062 m 0.47

β-:100.00

4

1.964E+06 1.675E+06 ENSDF

1814 55-Cs-141 3.5+ 24.84 s 0.68

β-:100.00

4

1.506E+06 1.701E+06 ENSDF

1815 55-Cs-142 0.0- 1.684 s 0.83

β-:100.00

4

2.899E+06 6.753E+05 ENSDF

1816 55-Cs-143 1.5+ 1.791 s 0.39

β-:98.36; β-,n:1.64

0

2.063E+06 2.063E+06 8.531E+03 NUBASE

1817 55-Cs-144 1.0- 0.994 s 0.40

β-:96.80; β-,n:3.20

0

2.763E+06 2.763E+06 2.076E+04 NUBASE

1818 55-Cs-144M ? 3.000E+05 1 s 100

β-:50.00; IT:50.00

0

1.466E+06 1.616E+06 NUBASE

1819 55-Cs-145 1.5+ 0.594 s 2.19

β-:85.70; β-,n:14.30

4

2.956E+06 7.149E+05 ENSDF

1820 55-Cs-146 1.0- 0.323 s 1.86

β-:85.80; β-,n:14.20

0

2.815E+06 2.815E+06 1.320E+05 NUBASE

1821 55-Cs-147 1.5+ 0.225 s 2.22

β-:71.50; β-,n:28.50

0

2.395E+06 2.395E+06 3.497E+05 NUBASE

1822 55-Cs-148 ? 0.146 s 4.11

β-:74.90; β-,n:25.10

0

3.002E+06 3.002E+06 3.281E+05 NUBASE

1823 55-Cs-149 1.5+ 0.15 s 100

β-:100.00

0

3.213E+06 3.213E+06 NUBASE

1824 55-Cs-150 ? 0.1 s 100

β-:100.00

0

3.880E+06 3.880E+06 NUBASE

1825 55-Cs-151 1.5+ 0.06 s 100

β-:100.00

0

3.533E+06 3.533E+06 NUBASE

1826 56-Ba-114 0.0+ 0.53 s 43.40

β+:79.10; β+,p:20.00;

α:0.90

0

2.707E+06 2.707E+06 4.743E+05 NUBASE

1827 56-Ba-115 2.5+ 0.45 s 11.11

β+:85.00; β+,p:15.00

0

3.427E+06 3.427E+06 4.038E+05 NUBASE

1828 56-Ba-116 0.0+ 1.3 s 15.38

β+:97.00; β+,p:3.00

0

2.466E+06 2.466E+06 5.076E+04 NUBASE

1829 56-Ba-117 1.5+ 1.75 s 4

β+m:86.98; β+,p:13.00;

β+,n:0.02

0

2.885E+06 2.885E+06 2.759E+05 NUBASE

1830 56-Ba-118 0.0+ 5.2 s 3.85

β+:100.00

0

2.013E+06 2.013E+06 NUBASE

1831 56-Ba-119 2.5+ 5.4 s 5.56

β+:37.50; β+

m:37.50;

β+,p:25.00

0

2.310E+06 2.310E+06 3.875E+05 NUBASE

1832 56-Ba-120 0.0+ 24 s 8.33

β+:100.00

0

1.666E+06 1.666E+06 NUBASE

1833 56-Ba-121 2.5+ 29.7 s 5.05

β+:49.99; β+

m:49.99;

β+,p:0.02

0

2.108E+06 2.108E+06 2.072E+02 NUBASE

1834 56-Ba-122 0.0+ 1.95 m 7.69

β+:100.00

0

1.177E+06 1.177E+06 NUBASE

1835 56-Ba-123 2.5+ 2.7 m 14.81

β+:50.00; β+

m:50.00

0

1.770E+06 1.770E+06 NUBASE

1836 56-Ba-124 0.0+ 11 m 4.55

β+:100.00

4

1.621E+05 5.500E+05 ENSDF

1837 56-Ba-125 0.5+ 3.5 m 11.43

β+:100.00

0

1.473E+06 1.473E+06 NUBASE

96 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

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Page 97: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1838 56-Ba-126 0.0+ 1.667 h 2

β+:100.00

4

1.813E+04 5.651E+05 UKPADD67

1839 56-Ba-127 0.5+ 12.7 m 3.15

β+:100.00

4

5.928E+05 7.123E+05 ENSDF

1840 56-Ba-127M 3.5- 8.033E+04 1.9 s 10.53

IT:100.00

0

8.033E+04 NUBASE

1841 56-Ba-128 0.0+ 2.43 d 2.06

β+:100.00

4

7.054E+03 6.599E+04 ENSDF

1842 56-Ba-129 0.5+ 2.38 h 4.62

β+:100.00

4

1.273E+05 4.665E+05 UKPADD67

1843 56-Ba-129M 3.5+ 8.420E+03 2.14 h 2.34

β+:100.00

4

6.910E+04 1.207E+06 UKPADD67

1844 56-Ba-130 0.0+

NUBASE

1845 56-Ba-130M 8.0- 2.475E+06 9.54E-03 s 1.47

IT:100.00

0

2.475E+06 NUBASE

1846 56-Ba-131 0.5+ 11.55 d 0.43

β+:100.00

4

4.625E+04 4.595E+05 UKPADD67

1847 56-Ba-131M 4.5- 1.875E+05 14.6 m 1.37

IT:100.00

3

1.101E+05 7.715E+04 UKPADD67

1848 56-Ba-132 0.0+

NUBASE

1849 56-Ba-133 0.5+ 10.54 y 0.09

β+:100.00

4

5.348E+04 4.017E+05 LNHB

1850 56-Ba-133M 5.5- 2.882E+05 1.592 d 0.79

β+:0.01; IT:99.99

4

2.216E+05 6.691E+04 UKPADD67

1851 56-Ba-134 0.0+

NUBASE

1852 56-Ba-135 1.5+

NUBASE

1853 56-Ba-135M 5.5- 2.682E+05 1.196 d 0.70

IT:100.00

3

2.059E+05 6.108E+04 ENSDF

1854 56-Ba-136 0.0+

NUBASE

1855 56-Ba-136M 7.0- 2.031E+06 0.308 s 0.62

IT:100.00

3

1.020E+05 1.927E+06 ENSDF

1856 56-Ba-137 1.5+

NUBASE

1857 56-Ba-137M 5.5- 6.617E+05 2.552 m 0.04

IT:100.00

3

6.073E+04 5.984E+05 LNHB

1858 56-Ba-138 0.0+

NUBASE

1859 56-Ba-139 3.5- 1.384 h 0.34

β-:100.00

3

8.928E+05 4.401E+04 ENSDF

1860 56-Ba-140 0.0+ 12.765 d 0.12

β-:100.00

4

3.106E+05 1.801E+05 LNHB

1861 56-Ba-141 1.5- 18.27 m 0.38

β-:100.00

4

9.457E+05 8.712E+05 ENSDF

1862 56-Ba-142 0.0+ 10.6 m 1.89

β-:100.00

4

3.991E+05 1.045E+06 ENSDF

1863 56-Ba-143 2.5- 14.5 s 2.07

β-:100.00

0

1.195E+06 1.341E+06 NUBASE

1864 56-Ba-144 0.0+ 11.5 s 1.74

β-:100.00

0

9.298E+05 7.847E+05 NUBASE

1865 56-Ba-145 2.5- 4.31 s 3.71

β-:100.00

0

1.285E+06 1.833E+06 NUBASE

1866 56-Ba-146 0.0+ 2.22 s 3.15

β-:100.00

0

1.373E+06 1.373E+06 NUBASE

1867 56-Ba-147 1.5+ 0.893 s 0.11

β-:99.98

4

2.379E+06 2.888E+05 ENSDF

1868 56-Ba-148 0.0+ 0.612 s 2.78

β-:99.60; β-,n:0.40

0

1.701E+06 1.701E+06 7.687E+02 NUBASE

1869 56-Ba-149 1.5- 0.344 s 2.03

β-:99.57; β-,n:0.43

0

2.428E+06 2.428E+06 1.686E+03 NUBASE

1870 56-Ba-150 0.0+ 0.3 s 100

β-:100.00

0

2.147E+06 2.147E+06 NUBASE

1871 56-Ba-151 1.5- 0.2 s 100

β-:100.00

0

2.823E+06 2.823E+06 NUBASE

1872 56-Ba-152 0.0+ 0.1 s 100

β-:100.00

0

2.490E+06 2.490E+06 NUBASE

1873 56-Ba-153 2.5- 0.08 s 100

β-:100.00

0

3.103E+06 3.103E+06 NUBASE

1874 57-La-117 ? 0.024 s 11.06

p:94.00; β+:6.00

0

2.156E+05 2.156E+05 7.529E+05 NUBASE

1875 57-La-117M 4.5+ 1.380E+05 0.01 s 50

p:97.00; β+:3.00

0

1.092E+05 1.092E+05 9.108E+05 NUBASE

1876 57-La-118 ? 0.2 s 100

β+:100.00

0

4.250E+06 4.250E+06 NUBASE

1877 57-La-119 5.5- 1 s 100

β+:100.00

0

3.207E+06 3.207E+06 NUBASE

1878 57-La-120 ? 2.8 s 7.14

β+:100.00

0

3.733E+06 3.733E+06 NUBASE

1879 57-La-121 5.5- 5.3 s 3.77

β+:100.00

0

2.780E+06 2.780E+06 NUBASE

1880 57-La-122 ? 8.7 s 8.05

β+:100.00

0

3.356E+06 3.356E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 97

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Page 98: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1881 57-La-123 5.5- 17 s 17.65

β+:100.00

0

2.315E+06 2.315E+06 NUBASE

1882 57-La-124 ? 29.21 s 0.58

β+:100.00

0

2.943E+06 2.943E+06 NUBASE

1883 57-La-124M 0.0+ 1.000E+05 21 s 19.05

β+:100.00

0

2.977E+06 2.977E+06 NUBASE

1884 57-La-125 5.5- 1.08 m 1.85

β+:100.00

0

1.970E+06 1.970E+06 NUBASE

1885 57-La-125M 1.5+ 1.070E+05 0.39 s 10.26

IT:100.00

0

1.070E+05 NUBASE

1886 57-La-126 5.0+ 54 s 3.70

β+:100.00

0

2.567E+06 2.567E+06 NUBASE

1887 57-La-126M ? 1.000E+05 20 s 100

β+:100.00

0

2.600E+06 2.600E+06 NUBASE

1888 57-La-127 5.5- 5.1 m 1.96

β+m:100.00

0

1.613E+06 1.613E+06 NUBASE

1889 57-La-127M 1.5+ 1.480E+04 3.7 m 10.81

β+:100.00

0

1.645E+06 1.645E+06 NUBASE

1890 57-La-128 5.0+ 5.18 m 2.70

β+:100.00

0

2.257E+06 2.257E+06 NUBASE

1891 57-La-128M ? 1.000E+05 1.4 m 100

β+:100.00

0

2.291E+06 2.291E+06 NUBASE

1892 57-La-129 1.5+ 11.6 m 1.72

β+:92.61; β+

m:7.39

4

6.212E+05 9.217E+05 ENSDF

1893 57-La-129M 5.5- 1.721E+05 0.56 s 8.93

IT:100.00

0

1.721E+05 NUBASE

1894 57-La-130 3.0+ 8.7 m 1.15

β+:100.00

4

1.113E+06 2.199E+06 ENSDF

1895 57-La-131 1.5+ 59 m 3.39

β+:100.00

4

2.115E+05 6.586E+05 ENSDF

1896 57-La-132 2.0- 4.8 h 4.17

β+:100.00

4

5.561E+05 1.944E+06 ENSDF

1897 57-La-132M 6.0- 1.882E+05 24.3 m 2.06

IT:76.00; β+:24.00

0

3.906E+05 5.337E+05 NUBASE

1898 57-La-133 2.5+ 3.912 h 0.20

β+:100.00

4

3.758E+04 1.275E+05 ENSDF

1899 57-La-134 1.0+ 6.45 m 2.48

β+:100.00

4

7.580E+05 7.161E+05 ENSDF

1900 57-La-135 2.5+ 19.5 h 1.03

β+:100.00

4

5.152E+03 3.574E+04 ENSDF

1901 57-La-136 1.0+ 9.87 m 0.30

β+:100.00

4

3.030E+05 4.146E+05 ENSDF

1902 57-La-136M ? 2.550E+05 0.114 s 2.63

IT:100.00

0

2.550E+05 NUBASE

1903 57-La-137 3.5+ 6E+04 y 33.33

β+:100.00

3

6.552E+03 2.559E+04 UKPADD67

1904 57-La-138 5.0+ 1.02E+11 y 0.98

β+:65.60; β-:34.40

5

3.650E+04 1.226E+06 ENSDF

1905 57-La-139 3.5+

NUBASE

1906 57-La-140 3.0- 1.679 d 0.01

β-:100.00

4

5.351E+05 2.313E+06 UKPADD67

1907 57-La-141 3.5+ 3.92 h 0.77

β-:100.00

2

9.625E+05 2.678E+04 ENSDF

1908 57-La-142 2.0- 1.518 h 0.55

β-:100.00

4

9.619E+05 2.121E+06 ENSDF

1909 57-La-143 3.5+ 14.14 m 1.13

β-:100.00

2

1.235E+06 4.394E+05 ENSDF

1910 57-La-144 3.0- 40.8 s 0.98

β-:100.00

4

9.862E+05 3.085E+06 ENSDF

1911 57-La-145 2.5+ 24.8 s 8.06

β-:100.00

4

7.618E+05 2.144E+06 ENSDF

1912 57-La-146 2.0- 6.27 s 1.59

β-:100.00

4

2.345E+06 1.195E+06 ENSDF

1913 57-La-146M 6.0- 1.300E+05 10 s 1

β-:100.00

0

2.230E+06 2.230E+06 NUBASE

1914 57-La-147 2.5+ 4.015 s 0.20

β-:100.00

4

2.059E+06 1.837E+05 ENSDF

1915 57-La-148 2.0- 1.26 s 6.35

β-:100.00

4

2.672E+06 1.194E+06 ENSDF

1916 57-La-149 2.5+ 1.05 s 2.86

β-:98.60; β-,n:1.40

0

1.944E+06 1.944E+06 5.319E+03 NUBASE

1917 57-La-150 3.0+ 0.51 s 5.88

β-:97.30; β-,n:2.70

0

2.534E+06 2.534E+06 1.072E+04 NUBASE

1918 57-La-151 2.5+ 0.3 s 100

β-:100.00

0

2.403E+06 2.403E+06 NUBASE

1919 57-La-152 2.0- 0.28 s 21.43

β-:93.96; β-,n:6.04

3

2.355E+06 2.885E+06 2.396E+04 UKPADD67

1920 57-La-153 2.5+ 0.15 s 100

β-:100.00

0

2.807E+06 2.807E+06 NUBASE

1921 57-La-154 ? 0.1 s 100

β-:100.00

0

3.440E+06 3.440E+06 NUBASE

1922 57-La-155 2.5+ 0.06 s 100

β-:100.00

0

3.200E+06 3.200E+06 NUBASE

1923 58-Ce-119 2.5+ 0.2 s 100

β+:100.00

0

3.657E+06 3.657E+06 NUBASE

98 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 99: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1924 58-Ce-120 0.0+ 0.25 s 60

β+:100.00

0

2.660E+06 2.660E+06 NUBASE

1925 58-Ce-121 2.5+ 1.1 s 9.09

β+:99.00; β+,p:1.00

0

3.223E+06 3.223E+06 2.225E+04 NUBASE

1926 58-Ce-122 0.0+ 2 s 100

β+:100.00

0

2.233E+06 2.233E+06 NUBASE

1927 58-Ce-123 2.5+ 3.8 s 5.26

β+:100.00

0

2.843E+06 2.843E+06 NUBASE

1928 58-Ce-124 0.0+ 9.1 s 13.19

β+m:100.00

0

1.780E+06 1.780E+06 NUBASE

1929 58-Ce-125 3.5- 9.3 s 3.23

β+m:100.00

0

2.331E+06 2.331E+06 NUBASE

1930 58-Ce-126 0.0+ 51 s 0.59

β+m:100.00

0

1.350E+06 1.350E+06 NUBASE

1931 58-Ce-127 2.5+ 29 s 6.90

β+:50.00; β+

m:50.00

0

1.970E+06 1.970E+06 NUBASE

1932 58-Ce-127M 0.5+ 34 s 5.88

β+m:100.00

0

1.967E+06 1.967E+06 NUBASE

1933 58-Ce-128 0.0+ 3.93 m 0.51

β+m:100.00

0

9.987E+05 9.987E+05 NUBASE

1934 58-Ce-129 2.5+ 3.5 m 14.29

β+:50.00; β+

m:50.00

0

1.651E+06 1.651E+06 NUBASE

1935 58-Ce-130 0.0+ 22.9 m 2.18

β+:100.00

4

2.538E+04 4.929E+05 ENSDF

1936 58-Ce-131 3.5+ 10.2 m 2.94

β+:100.00

0

1.350E+06 1.350E+06 NUBASE

1937 58-Ce-131M 0.5+ 6.180E+04 5 m 20

β+:100.00

0

1.370E+06 1.370E+06 NUBASE

1938 58-Ce-132 0.0+ 3.51 h 3.13

β+:100.00

4

1.490E+04 2.722E+05 ENSDF

1939 58-Ce-132M 8.0- 2.341E+06 9.4E-03 s 3.19

IT:100.00

0

2.341E+06 NUBASE

1940 58-Ce-133 0.5+ 1.617 h 4.12

β+:100.00

4

3.487E+05 4.562E+05 ENSDF

1941 58-Ce-133M 4.5- 3.710E+04 4.9 h 8.16

β+:100.00

0

1.036E+06 1.036E+06 NUBASE

1942 58-Ce-134 0.0+ 3.16 d 1.27

β+:100.00

4

5.426E+03 2.798E+04 ENSDF

1943 58-Ce-135 0.5+ 17.7 h 1.69

β+:100.00

4

2.727E+04 8.220E+05 ENSDF

1944 58-Ce-135M 5.5- 4.458E+05 20 s 5

IT:100.00

3

1.568E+05 2.917E+05 ENSDF

1945 58-Ce-136 0.0+ 7E+13 y 100

2β+:100.00

0

2.419E+06 NUBASE

1946 58-Ce-137 1.5+ 9 h 3.33

β+:100.00

4

1.247E+04 3.809E+04 ENSDF

1947 58-Ce-137M 5.5- 2.543E+05 1.433 d 0.87

β+:0.78; IT:99.22

4

2.027E+05 5.544E+04 ENSDF

1948 58-Ce-138 0.0+

NUBASE

1949 58-Ce-138M 7.0- 2.129E+06 8.65E-03 s 2.31

IT:100.00

0

2.129E+06 NUBASE

1950 58-Ce-139 1.5+ 137.641 d 0.01

β+:100.00

4

3.221E+04 1.605E+05 LNHB

1951 58-Ce-139M 5.5- 7.542E+05 56.1 s 1.07

IT:100.00

3

5.509E+04 6.991E+05 UKPADD67

1952 58-Ce-140 0.0+

NUBASE

1953 58-Ce-141 3.5- 32.5 d 0.03

β-:100.00

4

1.684E+05 7.651E+04 LNHB

1954 58-Ce-142 0.0+ 5E+16 y 100

2β-:100.00

0

1.417E+06 ENSDF

1955 58-Ce-143 1.5- 1.377 d 0.02

β-:100.00

4

4.306E+05 2.791E+05 ENSDF

1956 58-Ce-144 0.0+ 285 d 0.07

β-:98.62; β-

m:1.38

4

9.123E+04 1.905E+04 LNHB

1957 58-Ce-145 1.5- 2.95 m 2.03

β-:100.00

4

7.626E+05 6.010E+05 UKPADD67

1958 58-Ce-146 0.0+ 13.52 m 0.96

β-:100.00

4

1.948E+05 3.145E+05 ENSDF

1959 58-Ce-147 2.5- 57 s 3.51

β-:100.00

4

1.282E+06 1.742E+05 UKPADD67

1960 58-Ce-148 0.0+ 56 s 1.79

β-:100.00

0

5.857E+05 4.858E+05 NUBASE

1961 58-Ce-149 1.5- 5.3 s 3.77

β-:100.00

4

1.818E+06 8.456E+04 UKPADD67

1962 58-Ce-150 0.0+ 4 s 15

β-:100.00

0

1.161E+06 1.161E+06 NUBASE

1963 58-Ce-151 1.5- 1.02 s 5.88

β-:100.00

0

1.757E+06 1.757E+06 NUBASE

1964 58-Ce-152 0.0+ 1.1 s 27.27

β-:100.00

0

1.567E+06 1.567E+06 NUBASE

1965 58-Ce-153 1.5- 1.5 s 20

β-:99.38; β-,n:0.62

3

1.680E+06 1.125E+06 1.573E+03 UKPADD67

1966 58-Ce-154 0.0+ 2 s 20

β-:99.36; β-,n:0.64

3

1.694E+06 9.587E+05 1.619E+03 UKPADD67

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 99

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Page 100: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

1967 58-Ce-155 2.5- 0.2 s 100

β-:100.00

0

2.460E+06 2.460E+06 NUBASE

1968 58-Ce-156 0.0+ 0.15 s 100

β-:100.00

0

2.170E+06 2.170E+06 NUBASE

1969 58-Ce-157 3.5+ 0.05 s 100

β-:100.00

0

2.767E+06 2.767E+06 NUBASE

1970 59-Pr-121 1.5- 0.6 s 50

p:50.00; β+:50.00

0

1.853E+06 1.853E+06 4.205E+05 NUBASE

1971 59-Pr-122 ? 0.5 s 100

β+:100.00

0

4.317E+06 4.317E+06 NUBASE

1972 59-Pr-123 1.5+ 0.8 s 100

β+:100.00

0

3.280E+06 3.280E+06 NUBASE

1973 59-Pr-124 ? 1.2 s 16.67

β+:100.00

0

3.897E+06 3.897E+06 NUBASE

1974 59-Pr-125 1.5+ 3.3 s 21.21

β+:100.00

0

2.917E+06 2.917E+06 NUBASE

1975 59-Pr-126 ? 3.12 s 5.77

β+:100.00

0

3.520E+06 3.520E+06 NUBASE

1976 59-Pr-127 1.5+ 4.2 s 7.14

β+:50.00; β+

m:50.00

0

2.517E+06 2.517E+06 NUBASE

1977 59-Pr-127M 5.5- 6.000E+05 0.05 s 100

β+:25.00; β+

m:25.00;

IT:50.00

0

1.358E+06 1.658E+06 NUBASE

1978 59-Pr-128 4.0- 2.85 s 3.16

β+:100.00

4

3.454E+06 1.567E+06 ENSDF

1979 59-Pr-129 1.5+ 30 s 13.33

β+:100.00

0

2.171E+06 2.171E+06 NUBASE

1980 59-Pr-129M 5.5- 3.827E+05 1E-03 s 100

IT:100.00

0

3.827E+05 NUBASE

1981 59-Pr-130 ? 40 s 1

β+:100.00

0

2.748E+06 2.748E+06 NUBASE

1982 59-Pr-130M 2.0+ 1.000E+05 10 s 100

β+:100.00

0

2.781E+06 2.781E+06 NUBASE

1983 59-Pr-131 1.5+ 1.5 m 2

β+:50.00; β+

m:50.00

0

1.803E+06 1.803E+06 NUBASE

1984 59-Pr-131M 5.5- 1.524E+05 5.7 s 3.51

IT:96.40; β+:3.60

0

6.711E+04 2.140E+05 NUBASE

1985 59-Pr-132 2.0+ 1.49 m 7.38

β+:100.00

0

2.421E+06 2.421E+06 NUBASE

1986 59-Pr-132M 5.0+ 20 s 100

β+:50.00; β+

m:50.00

0

2.031E+06 2.031E+06 NUBASE

1987 59-Pr-133 1.5+ 6.5 m 4.62

β+:100.00

0

1.495E+06 1.495E+06 NUBASE

1988 59-Pr-134 2.0- 17 m 11.76

β+:100.00

4

1.192E+06 2.066E+06 ENSDF

1989 59-Pr-134M 2.0- 17 m 11.76

β+:100.00

0

2.109E+06 2.109E+06 NUBASE

1990 59-Pr-135 1.5+ 24 m 8.33

β+:100.00

0

1.230E+06 1.230E+06 NUBASE

1991 59-Pr-136 2.0+ 13.1 m 0.76

β+:100.00

4

7.535E+05 2.065E+06 ENSDF

1992 59-Pr-137 2.5+ 1.28 h 1.56

β+:100.00

4

1.930E+05 3.639E+05 ENSDF

1993 59-Pr-138 1.0+ 1.45 m 3.45

β+:100.00

4

1.161E+06 8.150E+05 ENSDF

1994 59-Pr-138M 7.0- 3.640E+05 2.12 h 1.89

β+:100.00

4

2.227E+05 2.443E+06 ENSDF

1995 59-Pr-139 2.5+ 4.41 h 0.91

β+:99.98; β+

m:0.02

4

4.621E+04 1.294E+05 ENSDF

1996 59-Pr-140 1.0+ 3.39 m 0.29

β+:100.00

4

5.465E+05 5.425E+05 ENSDF

1997 59-Pr-141 2.5+

NUBASE

1998 59-Pr-142 2.0- 19.12 h 0.21

β+:0.02; β-:99.98

5

8.093E+05 5.811E+04 ENSDF

1999 59-Pr-142M 5.0- 3.694E+03 14.6 m 3.42

IT:100.00

0

3.694E+03 NUBASE

2000 59-Pr-143 3.5+ 13.56 d 0.07

β-:100.00

3

3.146E+05 8.904E-03 UKPADD67

2001 59-Pr-144 0.0- 17.28 m 0.12

β-:100.00

4

1.201E+06 3.376E+04 UKPADD67

2002 59-Pr-144M 3.0- 5.903E+04 6.9 m 10.14

IT:99.93; β-:0.07

4

4.717E+04 1.366E+04 UKPADD67

2003 59-Pr-145 3.5+ 5.984 h 0.17

β-:100.00

4

6.573E+05 1.859E+04 ENSDF

2004 59-Pr-146 2.0- 24.15 m 0.75

β-:100.00

2

1.317E+06 9.874E+05 ENSDF

2005 59-Pr-147 1.5+ 13.4 m 2.99

β-:100.00

0

6.685E+05 9.285E+05 NUBASE

2006 59-Pr-148 1.0- 2.29 m 0.87

β-:100.00

4

1.348E+06 1.776E+06 ENSDF

2007 59-Pr-148M 4.0+ 9.000E+04 2.02 m 4.46

β-:100.00

2

1.239E+06 2.050E+06 ENSDF

2008 59-Pr-149 2.5+ 2.26 m 3.10

β-:100.00

4

8.107E+05 1.332E+06 ENSDF

100 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

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Page 101: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2009 59-Pr-150 1.0- 6.1 s 6.56

β-:100.00

4

2.230E+06 5.542E+05 UKPADD67

2010 59-Pr-151 1.5- 18.9 s 0.37

β-:100.00

0

1.114E+06 1.362E+06 NUBASE

2011 59-Pr-152 4.0- 3.63 s 3.31

β-:100.00

4

2.116E+06 1.685E+06 ENSDF

2012 59-Pr-153 2.5- 4.28 s 2.57

β-:100.00

0

1.906E+06 1.906E+06 NUBASE

2013 59-Pr-154 ? 2.3 s 4.35

β-:100.00

0

2.497E+06 2.497E+06 NUBASE

2014 59-Pr-155 2.5- 1 s 100

β-:100.00

0

2.230E+06 2.230E+06 NUBASE

2015 59-Pr-156 2.0- 0.5 s 20

β-:97.28; β-,n:2.72

3

2.149E+06 2.688E+06 8.930E+03 UKPADD67

2016 59-Pr-157 2.5- 0.3 s 20

β-:93.61; β-,n:6.39

3

2.387E+06 1.881E+06 2.372E+04 UKPADD67

2017 59-Pr-158 ? 0.2 s 100

β-:100.00

0

3.223E+06 3.223E+06 NUBASE

2018 59-Pr-159 2.5- 0.1 s 100

β-:100.00

0

2.923E+06 2.923E+06 NUBASE

2019 60-Nd-124 0.0+ 0.5 s 100

β+:100.00

0

2.877E+06 2.877E+06 NUBASE

2020 60-Nd-125 2.5+ 0.6 s 25

β+:100.00

0

3.430E+06 3.430E+06 NUBASE

2021 60-Nd-126 0.0+ 1 s 100

β+:100.00

0

2.457E+06 2.457E+06 NUBASE

2022 60-Nd-127 2.5+ 1.8 s 22.22

β+:100.00

0

3.003E+06 3.003E+06 NUBASE

2023 60-Nd-128 0.0+ 5 s 100

β+:100.00

0

2.050E+06 2.050E+06 NUBASE

2024 60-Nd-129 2.5+ 4.9 s 4.08

β+:100.00

0

2.511E+06 2.511E+06 NUBASE

2025 60-Nd-130 0.0+ 21 s 14.29

β+m:100.00

0

1.495E+06 1.495E+06 NUBASE

2026 60-Nd-131 2.5+ 33 s 9.09

β+:100.00

0

2.170E+06 2.170E+06 NUBASE

2027 60-Nd-132 0.0+ 1.467 m 7.95

β+:100.00

4

4.833E+05 9.320E+05 ENSDF

2028 60-Nd-133 3.5+ 1.167 m 14.29

β+:100.00

0

1.869E+06 1.869E+06 NUBASE

2029 60-Nd-133M 0.5+ 1.280E+05 1.167 m 100

β+:100.00

0

1.912E+06 1.912E+06 NUBASE

2030 60-Nd-134 0.0+ 8.5 m 17.65

β+:100.00

4

1.316E+05 5.106E+05 ENSDF

2031 60-Nd-135 4.5- 12.4 m 4.84

β+:100.00

0

1.574E+06 1.574E+06 NUBASE

2032 60-Nd-135M 0.5+ 6.500E+04 5.5 m 9.09

β+:99.97; IT:0.03

0

1.595E+06 1.595E+06 NUBASE

2033 60-Nd-136 0.0+ 50.65 m 0.65

β+:100.00

4

6.093E+04 2.804E+05 ENSDF

2034 60-Nd-137 0.5+ 38.5 m 3.90

β+:100.00

0

1.199E+06 1.199E+06 NUBASE

2035 60-Nd-137M 5.5- 5.194E+05 1.6 s 9.37

IT:100.00

0

5.194E+05 NUBASE

2036 60-Nd-138 0.0+ 5.04 h 1.79

β+:100.00

0

3.713E+05 3.713E+05 NUBASE

2037 60-Nd-139 1.5+ 29.7 m 1.68

β+:100.00

4

2.075E+05 4.211E+05 ENSDF

2038 60-Nd-139M 5.5- 2.312E+05 5.5 h 3.64

β+:88.20; IT:11.80

0

9.003E+05 9.275E+05 NUBASE

2039 60-Nd-140 0.0+ 3.37 d 0.59

β+:100.00

3

6.735E+03 2.773E+04 UKPADD67

2040 60-Nd-141 1.5+ 2.49 h 1.20

β+:100.00

4

1.416E+04 7.515E+04 ENSDF

2041 60-Nd-141M 5.5- 7.565E+05 1.033 m 1.29

IT:99.97; β+:0.03

0

2.751E+02 7.565E+05 NUBASE

2042 60-Nd-142 0.0+

NUBASE

2043 60-Nd-143 3.5-

NUBASE

2044 60-Nd-144 0.0+ 2.29E+15 y 6.99

α:100.00

1

1.905E+06 ENSDF

2045 60-Nd-145 3.5-

NUBASE

2046 60-Nd-146 0.0+

NUBASE

2047 60-Nd-147 2.5- 10.98 d 0.09

β-:100.00

4

2.690E+05 1.376E+05 LNHB

2048 60-Nd-148 0.0+ 2.7E+18 y 100

2β-:100.00

0

1.929E+06 ENSDF

2049 60-Nd-149 2.5- 1.728 h 0.06

β-:100.00

4

5.021E+05 3.700E+05 ENSDF

2050 60-Nd-150 0.0+ 2.1E+19 y 23.81

2β-:100.00

0

3.368E+06 ENSDF

2051 60-Nd-151 1.5+ 12.44 m 0.56

β-:100.00

4

6.074E+05 8.428E+05 ENSDF

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 101

MAIN DATA TABLES

Page 102: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2052 60-Nd-152 0.0+ 11.4 m 1.75

β-:100.00

0

3.680E+05 3.680E+05 NUBASE

2053 60-Nd-153 1.5- 31.6 s 3.16

β-:100.00

0

1.153E+06 5.086E+05 NUBASE

2054 60-Nd-154 0.0+ 25.9 s 0.77

β-:100.00

0

8.562E+05 5.506E+05 NUBASE

2055 60-Nd-155 1.5- 8.9 s 2.25

β-:100.00

0

1.085E+06 1.543E+06 NUBASE

2056 60-Nd-156 0.0+ 5.49 s 1.28

β-:100.00

0

1.230E+06 1.230E+06 NUBASE

2057 60-Nd-157 2.5- 2.5 s 20

β-:100.00

2

1.668E+06 1.140E+06 UKPADD67

2058 60-Nd-158 0.0+ 0.7 s 28.57

β-:100.00; β-,n:0.01

3

1.589E+06 9.239E+05 5.383E+00 UKPADD67

2059 60-Nd-159 3.5+ 0.5 s 20

β-:99.76; β-,n:0.24

3

2.063E+06 1.666E+06 5.109E+02 UKPADD67

2060 60-Nd-160 0.0+ 0.3 s 20

β-:99.05; β-,n:0.95

3

2.100E+06 1.206E+06 2.492E+03 UKPADD67

2061 60-Nd-161 0.5- 0.2 s 100

β-:100.00

0

2.490E+06 2.490E+06 NUBASE

2062 61-Pm-126 ? 0.5 s 100

β+:100.00

0

4.440E+06 4.440E+06 NUBASE

2063 61-Pm-127 2.5+ 1 s 100

β+:50.00; p:50.00

0

1.727E+06 1.727E+06 2.705E+05 NUBASE

2064 61-Pm-128 6.0+ 1 s 30

β+:100.00

0

4.043E+06 4.043E+06 NUBASE

2065 61-Pm-129 2.5+ 3 s 100

β+:100.00

0

3.097E+06 3.097E+06 NUBASE

2066 61-Pm-130 ? 2.6 s 7.69

β+:100.00

0

3.709E+06 3.709E+06 NUBASE

2067 61-Pm-131 2.5+ 6.3 s 12.70

β+:100.00

0

2.676E+06 2.676E+06 NUBASE

2068 61-Pm-132 3.0+ 6.3 s 11.11

β+:100.00

4

3.818E+06 1.506E+06 ENSDF

2069 61-Pm-133 1.5+ 15 s 20

β+:50.00; β+

m:50.00

0

2.285E+06 2.285E+06 NUBASE

2070 61-Pm-133M 5.5- 1.304E+05 10 s 100

β+:50.00; IT:50.00

0

1.175E+06 1.240E+06 NUBASE

2071 61-Pm-134 2.0+ 5 s 100

β+:100.00

4

3.225E+06 1.772E+06 ENSDF

2072 61-Pm-134M 2.0+ 5 s 100

β+:100.00

0

2.969E+06 2.969E+06 NUBASE

2073 61-Pm-135 ? 49 s 6.12

β+:50.00; β+

m:50.00

0

2.067E+06 2.067E+06 NUBASE

2074 61-Pm-135M 5.5- 5.000E+04 40 s 7.50

β+:100.00

0

2.095E+06 2.095E+06 NUBASE

2075 61-Pm-136 5.0- 1.783 m 5.61

β+:100.00

0

2.666E+06 2.666E+06 NUBASE

2076 61-Pm-136M 2.0+ 2.800E+05 47 s 4.26

β+:100.00

0

2.760E+06 2.760E+06 NUBASE

2077 61-Pm-137 2.5+ 2 m 100

β+:50.00; β+

m:50.00

0

1.749E+06 1.749E+06 NUBASE

2078 61-Pm-137M 5.5- 1.800E+05 2.4 m 4.17

β+:37.42; β+

m:62.58

0

1.787E+06 1.787E+06 NUBASE

2079 61-Pm-138 1.0+ 10 s 20

β+:100.00

0

2.359E+06 2.359E+06 NUBASE

2080 61-Pm-138M 5.0- 3.000E+04 3.24 m 1.54

β+:100.00

0

2.369E+06 2.369E+06 NUBASE

2081 61-Pm-139 2.5+ 4.15 m 1.20

β+:100.00

4

1.070E+06 9.400E+05 ENSDF

2082 61-Pm-139M 5.5- 1.887E+05 0.18 s 11.11

IT:99.94

3

1.007E+05 8.519E+04 ENSDF

2083 61-Pm-140 1.0+ 9.2 s 2.17

β+:100.00

4

2.034E+06 9.837E+05 ENSDF

2084 61-Pm-140M 7.0- 4.000E+05 5.95 m 0.84

β+:100.00

4

9.794E+05 2.963E+06 ENSDF

2085 61-Pm-141 2.5+ 20.9 m 0.24

β+:99.84; β+

m:0.16

4

6.314E+05 7.491E+05 ENSDF

2086 61-Pm-142 1.0+ 40.5 s 1.23

β+:100.00

4

1.368E+06 8.690E+05 ENSDF

2087 61-Pm-142M 8.0- 8.832E+05 2E-03 s 10

IT:100.00

0

8.832E+05 NUBASE

2088 61-Pm-143 2.5+ 266 d 3.01

β+:100.00

4

8.114E+03 3.158E+05 UKPADD67

2089 61-Pm-144 5.0- 363 d 3.86

β+:100.00

4

1.677E+04 1.556E+06 UKPADD67

2090 61-Pm-145 2.5+ 17.7 y 2.26

β+:100.00; α:~

5

1.220E+04 3.153E+04 6.502E-03 UKPADD67

2091 61-Pm-146 3.0- 5.531 y 0.89

β-:34.00; β+:66.00

5

9.441E+04 7.543E+05 UKPADD67

2092 61-Pm-147 3.5+ 2.623 y 0.01

β-:100.00

4

6.196E+04 4.375E+00 ENSDF

2093 61-Pm-148 1.0- 5.368 d 0.15

β-:100.00

4

7.263E+05 5.765E+05 UKPADD67

2094 61-Pm-148M 6.0- 1.379E+05 41.05 d 0.34

β-:95.00; IT:5.00

4

1.710E+05 1.984E+06 UKPADD67

102 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 103: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2095 61-Pm-149 3.5+ 2.212 d 0.09

β-:100.00

4

3.661E+05 1.186E+04 ENSDF

2096 61-Pm-150 1.0- 2.68 h 0.75

β-:100.00

4

7.342E+05 1.450E+06 ENSDF

2097 61-Pm-151 2.5+ 1.183 d 0.14

β-:100.00

4

3.035E+05 3.267E+05 ENSDF

2098 61-Pm-152 1.0+ 4.12 m 1.94

β-:100.00

4

1.304E+06 3.454E+05 ENSDF

2099 61-Pm-152M 4.0- 1.500E+05 7.52 m 1.06

β-:100.00

4

9.159E+05 1.476E+06 ENSDF

2100 61-Pm-152N 8.0- 3.200E+05 14.4 m 4.86

β-:100.00

4

7.284E+05 2.161E+06 UKPADD67

2101 61-Pm-153 2.5- 5.25 m 0.38

β-:100.00

4

6.626E+05 1.225E+05 ENSDF

2102 61-Pm-154 ? 1.73 m 5.78

β-:100.00

0

8.491E+05 1.876E+06 NUBASE

2103 61-Pm-154M ? 5.000E+04 2.68 m 2.61

β-:100.00

0

1.337E+06 1.337E+06 NUBASE

2104 61-Pm-155 2.5- 41.5 s 0.48

β-:100.00

4

1.061E+06 5.617E+05 UKPADD67

2105 61-Pm-156 4.0- 26.7 s 0.37

β-:100.00

0

1.206E+06 2.206E+06 NUBASE

2106 61-Pm-157 2.5- 10.56 s 0.95

β-:100.00

0

1.540E+06 8.490E+05 NUBASE

2107 61-Pm-158 ? 4.8 s 10.42

β-:100.00

0

2.040E+06 2.040E+06 NUBASE

2108 61-Pm-159 2.5- 3 s 20

β-:99.98; β-,n:0.02

3

1.782E+06 1.160E+06 2.156E+01 UKPADD67

2109 61-Pm-160 1.0- 2 s 20

β-:99.73; β-,n:0.27

3

1.969E+06 2.500E+06 5.530E+02 UKPADD67

2110 61-Pm-161 2.5- 0.7 s 100

β-:100.00

0

2.183E+06 2.183E+06 NUBASE

2111 61-Pm-162 ? 0.5 s 100

β-:100.00

0

2.813E+06 2.813E+06 NUBASE

2112 61-Pm-163 2.5- 0.2 s 100

β-:100.00

0

2.583E+06 2.583E+06 NUBASE

2113 62-Sm-128 0.0+ 0.5 s 100

β+:100.00

0

3.000E+06 3.000E+06 NUBASE

2114 62-Sm-129 2.5+ 0.55 s 18.18

β+:100.00

0

3.567E+06 3.567E+06 NUBASE

2115 62-Sm-130 0.0+ 1 s 100

β+:100.00

0

2.630E+06 2.630E+06 NUBASE

2116 62-Sm-131 2.5+ 1.2 s 16.67

β+:100.00

0

3.180E+06 3.180E+06 NUBASE

2117 62-Sm-132 0.0+ 4 s 7.50

β+:100.00

0

2.153E+06 2.153E+06 NUBASE

2118 62-Sm-133 2.5+ 2.9 s 5.86

β+:100.00

0

2.760E+06 2.760E+06 NUBASE

2119 62-Sm-134 0.0+ 10 s 10

β+:100.00

4

1.548E+06 1.056E+06 ENSDF

2120 62-Sm-135 3.5+ 10.3 s 4.85

β+:49.99; β+

m:49.99;

β+,p:0.02

0

2.365E+06 2.365E+06 2.749E+02 NUBASE

2121 62-Sm-135M ? 2.4 s 37.50

β+:100.00

0

2.373E+06 2.373E+06 NUBASE

2122 62-Sm-136 0.0+ 47 s 4.26

β+:100.00

4

1.012E+06 9.117E+05 ENSDF

2123 62-Sm-137 4.5- 45 s 2.22

β+m:100.00

0

1.954E+06 1.954E+06 NUBASE

2124 62-Sm-137M 0.5+ 1.800E+05 20 s 100

β+:100.00

0

2.074E+06 2.074E+06 NUBASE

2125 62-Sm-138 0.0+ 3.1 m 6.45

β+m:100.00

0

1.137E+06 1.137E+06 NUBASE

2126 62-Sm-139 0.5+ 2.57 m 3.89

β+:100.00

4

1.091E+06 1.459E+06 ENSDF

2127 62-Sm-139M 5.5- 4.574E+05 10.7 s 5.61

IT:93.70; β+

m:6.30

0

1.131E+05 5.417E+05 NUBASE

2128 62-Sm-140 0.0+ 14.82 m 0.81

β+:100.00

0

9.180E+05 9.180E+05 NUBASE

2129 62-Sm-141 0.5+ 10.2 m 1.96

β+:100.00

4

6.857E+05 1.385E+06 ENSDF

2130 62-Sm-141M 5.5- 1.760E+05 22.6 m 0.88

β+:99.69; IT:0.31

0

1.582E+06 1.582E+06 NUBASE

2131 62-Sm-142 0.0+ 1.208 h 0.07

β+:100.00

4

3.266E+04 8.928E+04 ENSDF

2132 62-Sm-143 1.5+ 8.75 m 0.91

β+:100.00

4

4.777E+05 5.127E+05 ENSDF

2133 62-Sm-143M 5.5- 7.540E+05 1.1 m 3.03

IT:99.76; β+:0.24

0

3.358E+03 7.555E+05 NUBASE

2134 62-Sm-143N 11.5- 2.794E+06 0.03 s 10

ITm:100.00

0

2.040E+06 NUBASE

2135 62-Sm-144 0.0+

NUBASE

2136 62-Sm-145 3.5- 340 d 0.88

β+:100.00

4

2.950E+04 6.299E+04 UKPADD67

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 103

MAIN DATA TABLES

Page 104: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2137 62-Sm-146 0.0+ 1E+08 y 8

α:100.00

1

2.571E+06 UKPADD67

2138 62-Sm-147 3.5- 1.06E+11 y 1.89

α:100.00

1

2.310E+06 ENSDF

2139 62-Sm-148 0.0+ 7E+15 y 28.57

α:100.00

1

1.986E+06 ENSDF

2140 62-Sm-149 3.5- 2E+15 y 100

α:100.00

1

1.870E+06 ENSDF

2141 62-Sm-150 0.0+

NUBASE

2142 62-Sm-151 2.5- 90.002 y 6.67

β-:100.00

4

1.987E+04 1.433E+01 UKPADD67

2143 62-Sm-152 0.0+

NUBASE

2144 62-Sm-153 1.5+ 1.928 d 0.01

β-:100.00

4

2.675E+05 6.233E+04 LNHB

2145 62-Sm-153M 5.5- 9.837E+04 0.011 s 2.83

IT:100.00

0

9.837E+04 NUBASE

2146 62-Sm-154 0.0+

NUBASE

2147 62-Sm-155 1.5- 22.3 m 0.90

β-:100.00

4

5.682E+05 1.026E+05 ENSDF

2148 62-Sm-156 0.0+ 9.4 h 2.13

β-:100.00

4

2.043E+05 1.142E+05 ENSDF

2149 62-Sm-157 1.5- 8.03 m 0.87

β-:100.00

0

8.389E+05 5.850E+05 NUBASE

2150 62-Sm-158 0.0+ 5.3 m 0.57

β-:100.00

0

5.121E+05 5.903E+05 NUBASE

2151 62-Sm-159 2.5- 11.37 s 1.32

β-:100.00

4

1.406E+06 4.306E+05 ENSDF

2152 62-Sm-160 0.0+ 9.6 s 3.12

β-:100.00

0

9.833E+05 9.833E+05 NUBASE

2153 62-Sm-161 3.5+ 4.8 s 16.67

β-:100.00

0

1.600E+06 1.600E+06 NUBASE

2154 62-Sm-162 0.0+ 2.4 s 20.83

β-:100.00

0

1.300E+06 1.300E+06 NUBASE

2155 62-Sm-163 0.5- 1 s 100

β-:100.00

0

1.910E+06 1.910E+06 NUBASE

2156 62-Sm-164 0.0+ 0.5 s 100

β-:100.00

0

1.640E+06 1.640E+06 NUBASE

2157 62-Sm-165 2.5- 0.2 s 100

β-:100.00

0

2.253E+06 2.253E+06 NUBASE

2158 63-Eu-130 2.0+ 1.1E-03 s 45.45

p:99.00; β+:1.00

0

4.547E+04 4.547E+04 1.011E+06 NUBASE

2159 63-Eu-131 1.5+ 0.018 s 10.67

p:88.00; β+:12.00

0

4.340E+05 4.340E+05 8.281E+05 NUBASE

2160 63-Eu-132 ? 0.1 s 100

β+:100.00

0

4.250E+06 4.250E+06 NUBASE

2161 63-Eu-133 5.5- 0.2 s 100

β+:100.00

0

3.283E+06 3.283E+06 NUBASE

2162 63-Eu-134 ? 0.5 s 40

β+:100.00

0

3.893E+06 3.893E+06 NUBASE

2163 63-Eu-135 5.5- 1.5 s 13.33

β+:100.00

0

2.890E+06 2.890E+06 NUBASE

2164 63-Eu-136 3.0+ 3.8 s 7.89

β+:100.00

4

2.514E+04 1.410E+06 ENSDF

2165 63-Eu-136M 3.0+ 3.8 s 7.89

β+:99.91; β+,p:0.05;

β+,pm:0.05

0

3.515E+06 3.515E+06 1.441E+03 NUBASE

2166 63-Eu-137 5.5- 8.4 s 5.95

β+:100.00

0

2.670E+06 2.670E+06 NUBASE

2167 63-Eu-138 6.0- 12.1 s 4.96

β+:100.00

0

3.249E+06 3.249E+06 NUBASE

2168 63-Eu-139 5.5- 17.9 s 3.35

β+:31.30; β+

m:68.70

0

2.223E+06 2.223E+06 NUBASE

2169 63-Eu-140 1.0+ 1.51 s 1.32

β+:100.00

4

3.156E+06 1.262E+06 ENSDF

2170 63-Eu-140M 5.0- 2.100E+05 0.125 s 1.60

IT:99.00; β+:1.00

0

2.892E+04 2.368E+05 NUBASE

2171 63-Eu-141 2.5+ 40.7 s 1.72

β+:98.23; β+

m:1.77

4

1.860E+06 1.059E+06 ENSDF

2172 63-Eu-141M 5.5- 9.645E+04 2.7 s 11.11

IT:86.00; β+:0.10;

β+m:13.90

0

2.769E+05 3.599E+05 NUBASE

2173 63-Eu-142 1.0+ 2.34 s 5.13

β+:100.00

4

2.754E+06 1.196E+06 ENSDF

2174 63-Eu-142M 8.0- 4.600E+05 1.223 m 0.65

β+:100.00

4

1.773E+06 3.416E+06 ENSDF

2175 63-Eu-143 2.5+ 2.59 m 0.77

β+:99.88; β+

m:0.12

4

1.295E+06 1.100E+06 ENSDF

2176 63-Eu-144 1.0+ 10.2 s 0.98

β+:100.00

4

2.057E+06 1.090E+06 ENSDF

2177 63-Eu-145 2.5+ 5.93 d 0.67

β+:100.00

4

2.280E+04 1.278E+06 ENSDF

104 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 105: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2178 63-Eu-146 4.0- 4.59 d 0.65

β+:100.00

4

4.228E+04 2.376E+06 ENSDF

2179 63-Eu-147 2.5+ 24 d 4.17

α:~; β+:100.00

5

3.448E+04 4.385E+05 6.398E+01 ENSDF

2180 63-Eu-148 5.0- 54.5 d 0.92

β+:100.00

4

1.911E+04 2.227E+06 ENSDF

2181 63-Eu-149 2.5+ 93.1 d 0.43

β+:100.00

4

2.414E+04 6.602E+04 UKPADD67

2182 63-Eu-150 5.0- 36.359 y 1.96

β+:100.00

4

2.721E+04 1.528E+06 UKPADD67

2183 63-Eu-150M 0.0- 4.210E+04 12.8 h 1.56

β-:88.00; β+:12.00

5

3.073E+05 5.022E+04 UKPADD67

2184 63-Eu-151 2.5+

NUBASE

2185 63-Eu-152 3.0- 13.525 y 0.10

β+:72.10; β-:27.90

5

1.248E+05 1.161E+06 LNHB

2186 63-Eu-152M 0.0- 4.560E+04 9.275 h 0.10

β-:72.00; β+:28.00

5

5.020E+05 3.111E+05 UKPADD67

2187 63-Eu-152N 8.0- 1.478E+05 1.6 h 3.12

IT:100.00

3

7.226E+04 7.551E+04 UKPADD67

2188 63-Eu-153 2.5+

NUBASE

2189 63-Eu-154 3.0- 8.593 y 0.04

β-:99.98; β+:0.02

5

2.745E+05 1.245E+06 UKPADD67

2190 63-Eu-154M 8.0- 1.570E+05 46.4 m 1.08

IT:100.00

3

8.250E+04 7.436E+04 UKPADD67

2191 63-Eu-155 2.5+ 4.753 y 0.29

β-:100.00

4

6.296E+04 6.129E+04 LNHB

2192 63-Eu-156 0.0+ 15.19 d 0.53

β-:100.00

4

4.536E+05 1.234E+06 ENSDF

2193 63-Eu-157 2.5+ 15.18 h 0.20

β-:100.00

4

3.928E+05 2.899E+05 ENSDF

2194 63-Eu-158 1.0- 45.9 m 0.44

β-:100.00

4

8.844E+05 1.271E+06 ENSDF

2195 63-Eu-159 2.5+ 18.1 m 0.55

β-:100.00

4

9.001E+05 2.875E+05 ENSDF

2196 63-Eu-160 1.0- 38 s 10.53

β-:100.00

0

1.526E+06 1.526E+06 NUBASE

2197 63-Eu-161 2.5+ 26 s 11.54

β-:100.00

0

1.244E+06 1.244E+06 NUBASE

2198 63-Eu-162 ? 10.6 s 9.43

β-:100.00

0

1.879E+06 1.879E+06 NUBASE

2199 63-Eu-163 2.5+ 6 s 100

β-:100.00

0

1.620E+06 1.620E+06 NUBASE

2200 63-Eu-164 ? 2 s 100

β-:100.00

0

2.217E+06 2.217E+06 NUBASE

2201 63-Eu-165 2.5+ 1 s 100

β-:100.00

0

1.970E+06 1.970E+06 NUBASE

2202 63-Eu-166 ? 0.4 s 100

β-:100.00

0

2.600E+06 2.600E+06 NUBASE

2203 63-Eu-167 2.5+ 0.2 s 100

β-:100.00

0

2.370E+06 2.370E+06 NUBASE

2204 64-Gd-134 0.0+ 0.4 s 100

β+:100.00

0

2.753E+06 2.753E+06 NUBASE

2205 64-Gd-135 1.5- 1.1 s 18.18

β+:98.00; β+,p:2.00

0

3.320E+06 3.320E+06 5.020E+04 NUBASE

2206 64-Gd-136 0.0+ 1 s 50

β+m:100.00

0

2.403E+06 2.403E+06 NUBASE

2207 64-Gd-137 3.5+ 2.2 s 9.09

β+:100.00

0

2.937E+06 2.937E+06 NUBASE

2208 64-Gd-138 0.0+ 4.7 s 19.15

β+:100.00

0

1.990E+06 1.990E+06 NUBASE

2209 64-Gd-139 4.5- 5.7 s 7.02

β+:100.00

0

2.623E+06 2.623E+06 NUBASE

2210 64-Gd-139M 0.5+ 2.500E+05 4.8 s 18.75

β+:100.00

0

2.706E+06 2.706E+06 NUBASE

2211 64-Gd-140 0.0+ 15.8 s 2.53

β+:100.00

0

1.736E+06 1.736E+06 NUBASE

2212 64-Gd-141 0.5+ 14 s 28.57

β+:100.00

4

2.365E+06 1.314E+06 ENSDF

2213 64-Gd-141M 5.5- 3.778E+05 24.5 s 2.04

β+m:89.00; IT:11.00

0

2.072E+06 2.114E+06 NUBASE

2214 64-Gd-142 0.0+ 1.17 m 0.85

β+:100.00

3

3.547E+03 4.850E+05 ENSDF

2215 64-Gd-143 0.5+ 39 s 5.13

β+:100.00

4

1.812E+06 1.221E+06 ENSDF

2216 64-Gd-143M 5.5- 1.526E+05 1.833 m 1.27

β+:100.00

4

1.251E+06 2.094E+06 ENSDF

2217 64-Gd-144 0.0+ 4.47 m 1.34

β+:100.00

0

1.287E+06 1.287E+06 NUBASE

2218 64-Gd-145 0.5+ 23 m 1.74

β+:100.00

4

3.441E+05 2.428E+06 ENSDF

2219 64-Gd-145M 5.5- 7.491E+05 1.417 m 3.53

IT:94.30; β+:5.70

0

1.106E+05 8.170E+05 NUBASE

2220 64-Gd-146 0.0+ 48.27 d 0.21

β+:100.00

4

1.217E+05 2.544E+05 ENSDF

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 105

MAIN DATA TABLES

Page 106: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2221 64-Gd-147 3.5- 1.586 d 0.32

β+:100.00

0

7.290E+05 7.290E+05 NUBASE

2222 64-Gd-148 0.0+ 74.602 y 4.02

α:100.00

0

3.271E+06 NUBASE

2223 64-Gd-149 3.5- 9.28 d 1.08

β+:100.00

4

6.485E+04 5.290E+05 ENSDF

2224 64-Gd-150 0.0+ 1.82E+06 y 9.34

α:100.00

1

2.797E+06 UKPADD67

2225 64-Gd-151 3.5- 124 d 0.81

β+:100.00; α:~

5

3.883E+04 7.040E+04 2.671E-02 UKPADD67

2226 64-Gd-152 0.0+ 1.08E+14 y 7.41

α:100.00

1

2.205E+06 ENSDF

2227 64-Gd-153 1.5- 240.4 d 0.42

β+:100.00

4

3.983E+04 1.055E+05 LNHB

2228 64-Gd-154 0.0+

NUBASE

2229 64-Gd-155 1.5-

NUBASE

2230 64-Gd-155M 5.5- 1.210E+05 0.032 s 0.94

IT:100.00

0

1.210E+05 NUBASE

2231 64-Gd-156 0.0+

NUBASE

2232 64-Gd-157 1.5-

NUBASE

2233 64-Gd-158 0.0+

NUBASE

2234 64-Gd-159 1.5- 18.479 h 0.02

β-:100.00

4

3.086E+05 5.669E+04 ENSDF

2235 64-Gd-160 0.0+ 1.3E+17 y 100

2β-:100.00

0

1.730E+06 NUBASE

2236 64-Gd-161 2.5- 3.66 m 1.37

β-:100.00

4

5.861E+05 3.927E+05 ENSDF

2237 64-Gd-162 0.0+ 8.4 m 2.38

β-:100.00

4

3.396E+05 4.168E+05 ENSDF

2238 64-Gd-163 2.5- 1.133 m 4.41

β-:100.00

4

1.064E+06 4.904E+05 UKPADD67

2239 64-Gd-164 0.0+ 45 s 6.67

β-:100.00

0

7.767E+05 7.767E+05 NUBASE

2240 64-Gd-165 0.5- 10.3 s 15.53

β-:100.00

0

1.397E+06 1.397E+06 NUBASE

2241 64-Gd-166 0.0+ 4.8 s 20.83

β-:100.00

0

1.120E+06 1.120E+06 NUBASE

2242 64-Gd-167 2.5- 3 s 100

β-:100.00

0

1.713E+06 1.713E+06 NUBASE

2243 64-Gd-168 0.0+ 0.3 s 100

β-:100.00

0

1.467E+06 1.467E+06 NUBASE

2244 64-Gd-169 3.5- 1 s 100

β-:100.00

0

2.067E+06 2.067E+06 NUBASE

2245 65-Tb-136 ? 0.2 s 100

β+:100.00

0

4.360E+06 4.360E+06 NUBASE

2246 65-Tb-137 5.5- 0.6 s 100

p:50.00; β+:50.00

0

1.702E+06 1.702E+06 3.805E+05 NUBASE

2247 65-Tb-138 ? 0.8 s 100

β+:100.00

0

4.050E+06 4.050E+06 NUBASE

2248 65-Tb-139 5.5- 1.6 s 12.50

β+:100.00

0

3.120E+06 3.120E+06 NUBASE

2249 65-Tb-140 ? 2.4 s 8.33

β+:99.74; β+,p:0.26

0

3.762E+06 3.762E+06 4.959E+03 NUBASE

2250 65-Tb-141 2.5- 3.5 s 5.71

β+:50.00; β+

m:50.00

0

2.832E+06 2.832E+06 NUBASE

2251 65-Tb-141M 5.5- 7.9 s 7.59

β+m:100.00

0

2.769E+06 2.769E+06 NUBASE

2252 65-Tb-142 1.0+ 0.597 s 2.85

β+:100.00

3

1.840E+03 2.684E+05 ENSDF

2253 65-Tb-142M 5.0- 2.802E+05 0.303 s 5.61

IT:99.50; β+:0.50

0

1.697E+04 2.958E+05 NUBASE

2254 65-Tb-143 5.5- 12 s 8.33

β+m:100.00

0

2.549E+06 2.549E+06 NUBASE

2255 65-Tb-143M 2.5+ 21 s 100

β+:50.00; β+

m:50.00

0

2.575E+06 2.575E+06 NUBASE

2256 65-Tb-144 1.0+ 1 s 100

β+:100.00

1

2.877E+05 ENSDF

2257 65-Tb-144M 6.0- 3.969E+05 4.25 s 3.53

IT:66.00; β+:34.00

0

1.109E+06 1.371E+06 NUBASE

2258 65-Tb-145 1.5+ 20 m 100

β+:100.00

0

2.349E+06 2.349E+06 NUBASE

2259 65-Tb-145M 5.5- 30.9 s 2.27

β+:50.34; β+

m:49.66

0

2.225E+06 2.225E+06 NUBASE

2260 65-Tb-146 1.0+ 8 s 50

β+:100.00

4

2.994E+06 1.366E+06 UKPADD67

2261 65-Tb-146M 5.0- 1.500E+05 24 s 2.08

β+:100.00

4

1.454E+06 4.097E+06 UKPADD67

2262 65-Tb-146N 10.0+ 9.300E+05 1.18E-03 s 1.69

ITm:100.00

0

7.800E+05 NUBASE

2263 65-Tb-147 0.5+ 1.7 h 5.88

β+:100.00

4

2.578E+05 1.917E+06 ENSDF

106 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 107: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2264 65-Tb-147M 5.5- 5.060E+04 1.83 m 3.28

β+:100.00

1

1.566E+06 ENSDF

2265 65-Tb-148 2.0- 1 h 1.67

β+:100.00

4

8.397E+05 2.186E+06 ENSDF

2266 65-Tb-148M 9.0+ 9.010E+04 2.2 m 2.27

β+:100.00

0

1.942E+06 1.942E+06 NUBASE

2267 65-Tb-149 0.5+ 4.118 h 0.61

α:16.70; β+:83.30

5

8.352E+04 1.359E+06 6.810E+05 ENSDF

2268 65-Tb-149M 5.5- 4.000E+04 4.16 m 0.96

β+:99.98; α:0.02

5

1.731E+05 1.069E+06 8.798E+02 ENSDF

2269 65-Tb-150 2.0- 3.48 h 4.60

β+:99.95; α:0.05

0

1.552E+06 1.552E+06 1.793E+03 NUBASE

2270 65-Tb-150M 9.0+ 4.500E+05 5.8 m 3.45

β+:100.00

0

1.703E+06 1.703E+06 NUBASE

2271 65-Tb-151 0.5+ 17.609 h 0.08

α:0.01; β+:100.00

5

7.595E+04 9.881E+05 3.242E+02 ENSDF

2272 65-Tb-151M 5.5- 9.954E+04 25 s 12

IT:93.80; β+:6.20

0

5.507E+04 1.484E+05 NUBASE

2273 65-Tb-152 2.0- 17.5 h 0.57

β+:100.00

4

2.107E+05 1.391E+06 ENSDF

2274 65-Tb-152M 8.0+ 5.017E+05 4.2 m 2.38

IT:78.80; β+:21.20

0

3.177E+05 7.131E+05 NUBASE

2275 65-Tb-153 2.5+ 2.34 d 0.43

β+:100.00

4

4.227E+04 3.216E+05 ENSDF

2276 65-Tb-154 0.0+ 21.5 h 1.86

β+:99.90; β-:0.10

0

1.183E+06 1.183E+06 NUBASE

2277 65-Tb-154M 3.0- 1.200E+04 9.4 h 4.26

β+:78.12; IT:21.78;

β-:0.10

0

9.285E+05 9.311E+05 NUBASE

2278 65-Tb-154N 7.0- 2.000E+05 22.7 h 2.20

β+:98.20; ITm:1.80

0

1.229E+06 1.232E+06 NUBASE

2279 65-Tb-155 1.5+ 5.32 d 1.13

β+:100.00

4

3.834E+04 1.766E+05 ENSDF

2280 65-Tb-156 3.0- 5.17 d 2.32

β+:100.00

4

8.460E+04 1.935E+06 UKPADD67

2281 65-Tb-156M 7.0- 6.000E+04 1.017 d 4.10

IT:100.00

3

2.206E+04 3.759E+04 UKPADD67

2282 65-Tb-156N 0.0+ 8.840E+04 5.1 h 5.88

β+:0.19; IT:99.81

4

8.406E+04 4.743E+03 UKPADD67

2283 65-Tb-157 1.5+ 99.002 y 10.10

β+:100.00

4

5.700E+03 1.039E+04 UKPADD67

2284 65-Tb-158 3.0- 180 y 6.11

β-:16.80; β+:83.20

5

1.117E+05 8.137E+05 UKPADD67

2285 65-Tb-158M 0.0+ 1.103E+05 10.8 s 1.85

IT:100.00

3

8.593E+04 2.420E+04 UKPADD67

2286 65-Tb-159 1.5+

NUBASE

2287 65-Tb-160 3.0- 72.3 d 0.28

β-:100.00

4

2.573E+05 1.130E+06 UKPADD67

2288 65-Tb-161 1.5+ 6.89 d 0.44

β-:100.00

4

2.007E+05 3.376E+04 UKPADD67

2289 65-Tb-162 1.0- 7.6 m 1.97

β-:100.00

4

5.396E+05 1.106E+06 ENSDF

2290 65-Tb-163 1.5+ 19.5 m 1.54

β-:100.00

4

3.622E+05 7.859E+05 ENSDF

2291 65-Tb-164 5.0+ 3 m 3.33

β-:100.00

0

1.298E+06 1.298E+06 NUBASE

2292 65-Tb-165 1.5+ 2.11 m 4.74

β-:100.00

2

9.116E+05 6.418E+05 ENSDF

2293 65-Tb-166 ? 25.6 s 8.59

β-:100.00

0

1.610E+06 1.610E+06 NUBASE

2294 65-Tb-167 1.5+ 19 s 15.79

β-:100.00

0

1.367E+06 1.367E+06 NUBASE

2295 65-Tb-168 4.0- 8.2 s 15.85

β-:100.00

0

2.020E+06 2.020E+06 NUBASE

2296 65-Tb-169 1.5+ 2 s 100

β-:100.00

0

1.833E+06 1.833E+06 NUBASE

2297 65-Tb-170 ? 3 s 100

β-:100.00

0

2.440E+06 2.440E+06 NUBASE

2298 65-Tb-171 1.5+ 0.5 s 100

β-:100.00

0

2.203E+06 2.203E+06 NUBASE

2299 66-Dy-138 0.0+ 0.2 s 100

β+:100.00

0

2.897E+06 2.897E+06 NUBASE

2300 66-Dy-139 3.5+ 0.6 s 33.33

β+:100.00

0

3.493E+06 3.493E+06 NUBASE

2301 66-Dy-140 0.0+ 0.7 s 57.14

β+:100.00

0

2.547E+06 2.547E+06 NUBASE

2302 66-Dy-141 4.5- 0.9 s 22.22

β+:50.00; β+

m:50.00

0

3.073E+06 3.073E+06 NUBASE

2303 66-Dy-142 0.0+ 2.3 s 13.04

β+:99.94; β+,p:0.03;

β+,pm:0.03

0

2.366E+06 2.366E+06 8.679E+02 NUBASE

2304 66-Dy-143 0.5+ 5.6 s 17.86

β+m:100.00

0

2.703E+06 2.703E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 107

MAIN DATA TABLES

Page 108: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2305 66-Dy-143M 5.5- 3.107E+05 3 s 10

β+:100.00

0

2.807E+06 2.807E+06 NUBASE

2306 66-Dy-144 0.0+ 9.1 s 4.40

β+:100.00

1

7.504E+04 ENSDF

2307 66-Dy-145 0.5+ 9.5 s 10.53

β+:100.00

0

2.530E+06 2.530E+06 NUBASE

2308 66-Dy-145M 5.5- 1.182E+05 14.1 s 4.96

β+:35.40; β+

m:64.60

0

2.569E+06 2.569E+06 NUBASE

2309 66-Dy-146 0.0+ 29 s 10.34

β+:100.00

3

1.333E+04 1.180E+06 ENSDF

2310 66-Dy-146M 10.0+ 2.936E+06 0.15 s 13.33

IT:100.00

0

2.936E+06 NUBASE

2311 66-Dy-147 0.5+ 40 s 25

β+:99.95; β+,p:0.05

0

2.187E+06 2.187E+06 5.770E+02 NUBASE

2312 66-Dy-147M 5.5- 7.505E+05 55 s 1.82

β+m:65.00; IT:35.00

0

1.574E+06 1.837E+06 NUBASE

2313 66-Dy-148 0.0+ 3.3 m 6.06

β+:100.00

4

2.571E+04 7.175E+05 ENSDF

2314 66-Dy-149 3.5- 4.2 m 3.33

β+:100.00

4

1.031E+05 1.613E+06 ENSDF

2315 66-Dy-149M 13.5- 2.661E+06 0.49 s 3.06

IT:99.30; β+

m:0.70

0

1.495E+04 2.657E+06 NUBASE

2316 66-Dy-150 0.0+ 7.17 m 0.70

β+:64.00; α:36.00

0

3.827E+05 3.827E+05 1.566E+06 NUBASE

2317 66-Dy-151 3.5- 17.9 m 1.68

β+:64.57; β+

m:29.83;

α:5.60

0

8.935E+05 8.935E+05 2.340E+05 NUBASE

2318 66-Dy-152 0.0+ 2.38 h 0.84

α:0.10; β+:99.90

5

1.030E+04 2.865E+05 3.628E+03 ENSDF

2319 66-Dy-153 3.5- 6.4 h 1.56

α:0.01; β+:100.00

5

8.094E+04 7.089E+05 3.256E+02 ENSDF

2320 66-Dy-154 0.0+ 3E+06 y 50

α:100.00

1

2.947E+06 ENSDF

2321 66-Dy-155 1.5- 9.9 h 2.02

β+:100.00

4

2.362E+04 6.054E+05 ENSDF

2322 66-Dy-156 0.0+ 1E+18 y 100

α:50.00; 2β+:50.00

0

1.006E+06 8.796E+05 NUBASE

2323 66-Dy-157 1.5- 8.14 h 0.61

β+:100.00

4

1.329E+04 3.504E+05 UKPADD67

2324 66-Dy-157M 5.5- 1.995E+05 0.022 s 7.41

IT:100.00

3

9.443E+04 1.012E+05 ENSDF

2325 66-Dy-158 0.0+

NUBASE

2326 66-Dy-159 1.5- 144.4 d 0.14

β+:100.00

4

1.282E+04 4.551E+04 UKPADD67

2327 66-Dy-160 0.0+

NUBASE

2328 66-Dy-161 2.5+

NUBASE

2329 66-Dy-162 0.0+

NUBASE

2330 66-Dy-163 2.5-

NUBASE

2331 66-Dy-164 0.0+

NUBASE

2332 66-Dy-165 3.5+ 2.334 h 0.26

β-:100.00

4

4.480E+05 2.628E+04 ENSDF

2333 66-Dy-165M 0.5- 1.082E+05 1.257 m 0.48

IT:97.76; β-:2.24

0

1.042E+04 1.162E+05 NUBASE

2334 66-Dy-166 0.0+ 3.401 d 0.21

β-:100.00

4

1.596E+05 4.198E+04 UKPADD67

2335 66-Dy-167 0.5- 6.2 m 1.29

β-:100.00

4

7.063E+05 5.237E+05 ENSDF

2336 66-Dy-168 0.0+ 8.7 m 3.45

β-:100.00

0

5.033E+05 5.033E+05 NUBASE

2337 66-Dy-169 2.5- 39 s 20.51

β-:100.00

0

1.068E+06 1.068E+06 NUBASE

2338 66-Dy-170 0.0+ 30 s 100

β-m:100.00

0

8.267E+05 8.267E+05 NUBASE

2339 66-Dy-171 3.5- 6 s 100

β-:100.00

0

1.470E+06 1.470E+06 NUBASE

2340 66-Dy-172 0.0+ 3 s 100

β-:100.00

0

1.223E+06 1.223E+06 NUBASE

2341 66-Dy-173 4.5+ 2 s 100

β-:100.00

0

1.773E+06 1.773E+06 NUBASE

2342 67-Ho-140 8.0+ 6E-03 s 50

p:99.00; β+:1.00

0

4.510E+04 4.510E+04 1.080E+06 NUBASE

2343 67-Ho-141 3.5- 4.1E-03 s 7.32

p:100.00

0

8.429E+03 ENSDF

2344 67-Ho-142 ? 0.4 s 25

β+:100.00

0

4.163E+06 4.163E+06 NUBASE

2345 67-Ho-143 5.5- 0.3 s 100

β+m:100.00

0

3.243E+06 3.243E+06 NUBASE

2346 67-Ho-144 ? 0.7 s 14.29

β+:100.00

0

3.793E+06 3.793E+06 NUBASE

108 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 109: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2347 67-Ho-145 5.5- 2.4 s 4.17

β+m:100.00

0

2.997E+06 2.997E+06 NUBASE

2348 67-Ho-145M 2.5+ 1.000E+05 0.1 s 100

β+:50.00; IT:50.00

0

1.535E+06 1.585E+06 NUBASE

2349 67-Ho-146 10.0+ 3.6 s 8.33

β+m:100.00

0

2.683E+06 2.683E+06 NUBASE

2350 67-Ho-147 5.5- 5.8 s 6.90

β+m:100.00

0

2.534E+06 2.534E+06 NUBASE

2351 67-Ho-148 1.0+ 2.2 s 50

β+:100.00

4

3.781E+06 1.104E+06 ENSDF

2352 67-Ho-148M 10.0+ 6.944E+05 2.35E-03 s 1.70

IT:100.00

3

4.226E+04 6.484E+05 ENSDF

2353 67-Ho-148N 10.0+ 6.900E+05 2.35E-03 s 1.70

ITm:100.00

0

2.900E+05 NUBASE

2354 67-Ho-149 5.5- 21.1 s 0.95

β+:100.00

0

2.009E+06 2.009E+06 NUBASE

2355 67-Ho-149M 0.5+ 4.880E+04 56 s 5.36

β+:100.00

0

2.025E+06 2.025E+06 NUBASE

2356 67-Ho-150 2.0- 1.28 m 2.34

β+:100.00

0

2.456E+06 2.456E+06 NUBASE

2357 67-Ho-150M 9.0+ 23.3 s 1.29

β+:100.00

0

2.456E+06 2.456E+06 NUBASE

2358 67-Ho-151 5.5- 35.2 s 0.28

β+:78.00; α m:22.00

0

1.333E+06 1.333E+06 1.022E+06 NUBASE

2359 67-Ho-151M 0.5+ 4.100E+04 47.2 s 2.12

α:77.00; β+:23.00

0

3.962E+05 3.962E+05 3.647E+06 NUBASE

2360 67-Ho-152 2.0- 2.697 m 0.19

β+:88.00; α:12.00

0

1.911E+06 1.911E+06 5.409E+05 NUBASE

2361 67-Ho-152M 9.0+ 1.600E+05 50 s 0.80

β+:89.20; α m:10.80

0

1.985E+06 1.985E+06 4.943E+05 NUBASE

2362 67-Ho-153 5.5- 2.01 m 1.49

α:0.05; β+:99.95

5

5.271E+05 9.147E+05 1.994E+03 ENSDF

2363 67-Ho-153M 0.5+ 6.870E+04 9.3 m 5.38

β+:99.82; α:0.18

0

1.397E+06 1.397E+06 7.417E+03 NUBASE

2364 67-Ho-154 2.0- 11.76 m 1.62

β+:99.98; α:0.02

0

1.918E+06 1.918E+06 7.680E+02 NUBASE

2365 67-Ho-154M 8.0+ 2.400E+05 3.1 m 4.52

β+:100.00; α m:~

0

1.998E+06 1.998E+06 3.832E+01 NUBASE

2366 67-Ho-155 2.5+ 48 m 4.17

β+:100.00

4

2.084E+05 4.455E+05 ENSDF

2367 67-Ho-156 4.0- 56 m 1.79

β+:100.00

0

1.727E+06 1.727E+06 NUBASE

2368 67-Ho-156M 1.0- 5.240E+04 9.5 s 15.79

IT:50.00; β+:50.00

0

8.721E+05 8.983E+05 NUBASE

2369 67-Ho-156N 9.0+ 1.000E+05 7.8 m 3.85

β+:75.00; IT:25.00

0

1.320E+06 1.345E+06 NUBASE

2370 67-Ho-157 3.5- 12.6 m 1.59

β+:50.00; β+

m:50.00

0

8.331E+05 8.331E+05 NUBASE

2371 67-Ho-158 5.0+ 11.3 m 3.54

β+:100.00

0

1.407E+06 1.407E+06 NUBASE

2372 67-Ho-158M 2.0- 6.720E+04 28 m 7.14

IT:81.00; β+:19.00

0

2.716E+05 3.260E+05 NUBASE

2373 67-Ho-158N 9.0+ 1.800E+05 21.3 m 10.80

β+:93.00; IT:7.00

0

1.364E+06 1.377E+06 NUBASE

2374 67-Ho-159 3.5- 33.05 m 0.33

β+:100.00

4

5.117E+04 3.806E+05 ENSDF

2375 67-Ho-159M 0.5+ 2.059E+05 8.3 s 0.96

IT:100.00

3

1.036E+05 1.000E+05 ENSDF

2376 67-Ho-160 5.0+ 25.3 m 2.77

β+:100.00

4

7.034E+04 1.713E+06 UKPADD67

2377 67-Ho-160M 2.0- 5.998E+04 5 h 2

IT:65.00; β+:35.00

4

8.167E+04 6.498E+05 UKPADD67

2378 67-Ho-160N 9.0+ 2.000E+05 2.9 s 6.90

IT:100.00

3

9.388E+04 1.057E+05 UKPADD67

2379 67-Ho-161 3.5- 2.48 h 4.84

β+:100.00

4

3.344E+04 5.817E+04 UKPADD67

2380 67-Ho-161M 0.5+ 2.111E+05 6.77 s 0.89

IT:100.00

3

1.072E+05 1.037E+05 UKPADD67

2381 67-Ho-162 1.0+ 15 m 6.67

β+:100.00

4

5.676E+04 1.641E+05 ENSDF

2382 67-Ho-162M 6.0- 1.060E+05 1.117 h 1.04

IT:62.00; β+:38.00

0

2.845E+05 3.502E+05 NUBASE

2383 67-Ho-163 3.5- 4570.09 y 0.46

β+:100.00

1

2.650E+03 1.053E-03 UKPADD67

2384 67-Ho-163M 0.5+ 2.979E+05 1.1 s 6.36

IT:100.00

3

6.124E+04 2.365E+05 UKPADD67

2385 67-Ho-164 1.0+ 28.6 m 2.10

β-:51.70; β+:48.30

5

1.843E+05 2.816E+04 UKPADD67

2386 67-Ho-164M 6.0- 1.400E+05 37.6 m 1.33

IT:100.00

3

9.190E+04 4.803E+04 UKPADD67

2387 67-Ho-165 3.5-

NUBASE

2388 67-Ho-166 0.0- 1.117 d 0.07

β-:100.00

4

6.947E+05 3.021E+04 ENSDF

2389 67-Ho-166M 7.0+ 5.980E+03 1200 y 16.67

β-:100.00

4

1.411E+05 1.627E+06 LNHB

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 109

MAIN DATA TABLES

Page 110: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2390 67-Ho-167 3.5- 3.1 h 3.23

β-:88.05; β-

m:11.95

4

2.269E+05 3.630E+05 ENSDF

2391 67-Ho-168 3.0+ 2.99 m 2.34

β-:100.00

4

8.009E+05 8.633E+05 ENSDF

2392 67-Ho-168M 6.0+ 5.900E+04 2.2 m 3.03

IT:99.50; β-:0.50

0

4.976E+03 6.368E+04 NUBASE

2393 67-Ho-169 3.5- 4.7 m 2.13

β-:100.00

0

7.086E+05 7.086E+05 NUBASE

2394 67-Ho-170 6.0+ 2.78 m 5.04

β-:100.00

4

8.361E+05 1.835E+06 UKPADD67

2395 67-Ho-170M 1.0+ 1.200E+05 43 s 4.65

β-:100.00

4

1.365E+06 6.794E+05 UKPADD67

2396 67-Ho-171 3.5- 53 s 3.77

β-:100.00

0

1.068E+06 1.068E+06 NUBASE

2397 67-Ho-172 ? 25 s 12

β-:100.00

0

1.696E+06 1.696E+06 NUBASE

2398 67-Ho-173 3.5- 10 s 100

β-:100.00

0

1.517E+06 1.517E+06 NUBASE

2399 67-Ho-174 ? 8 s 100

β-:100.00

0

2.150E+06 2.150E+06 NUBASE

2400 67-Ho-175 3.5- 5 s 100

β-:100.00

0

1.950E+06 1.950E+06 NUBASE

2401 68-Er-143 4.5- 0.2 s 100

β+:100.00

0

3.643E+06 3.643E+06 NUBASE

2402 68-Er-144 0.0+ 0.4 s 50

β+:100.00

0

2.763E+06 2.763E+06 NUBASE

2403 68-Er-145 0.5+ 0.9 s 33.33

β+m:100.00

0

3.130E+06 3.130E+06 NUBASE

2404 68-Er-146 0.0+ 1.7 s 35.29

β+:100.00

0

2.287E+06 2.287E+06 NUBASE

2405 68-Er-147 0.5+ 2.5 s 100

β+:100.00

0

2.929E+06 2.929E+06 NUBASE

2406 68-Er-147M 5.5- 1.000E+05 2.5 s 8

β+:100.00

0

2.962E+06 2.962E+06 NUBASE

2407 68-Er-148 0.0+ 4.6 s 4.35

β+:99.85; β+,p:0.07;

β+,pm:0.07

0

2.122E+06 2.122E+06 1.828E+03 NUBASE

2408 68-Er-149 0.5+ 4 s 50

β+m:93.00; β+,p:7.00

0

2.568E+06 2.568E+06 1.195E+05 NUBASE

2409 68-Er-149M 5.5- 7.418E+05 8.9 s 2.25

β+:96.32; IT:3.50;

β+,p:0.18

0

2.793E+06 2.819E+06 3.406E+03 NUBASE

2410 68-Er-150 0.0+ 18.5 s 3.78

β+:100.00

0

1.372E+06 1.372E+06 NUBASE

2411 68-Er-151 3.5- 23.5 s 5.53

β+:100.00

4

8.287E+05 1.660E+06 ENSDF

2412 68-Er-151M 13.5- 2.586E+06 0.58 s 3.45

IT:95.30; β+:4.70

0

1.246E+05 2.589E+06 NUBASE

2413 68-Er-152 0.0+ 10.3 s 0.97

α:91.00; β+:10.00

5

1.887E+04 4.111E+04 4.490E+06 ENSDF

2414 68-Er-153 3.5- 37.1 s 0.54

α:53.00; β+:47.00

4

1.329E+03 3.227E+05 2.544E+06 ENSDF

2415 68-Er-154 0.0+ 3.73 m 2.41

α:0.47; β+:99.53

5

3.183E+04 7.596E+04 1.959E+04 ENSDF

2416 68-Er-155 3.5- 5.3 m 5.66

β+:99.98; α:0.02

0

1.275E+06 1.275E+06 9.062E+02 NUBASE

2417 68-Er-156 0.0+ 19.5 m 5.13

β+:4.59; β+

m:95.41

4

6.980E+04 5.725E+04 ENSDF

2418 68-Er-157 1.5- 18.65 m 0.54

β+:100.00

0

1.136E+06 1.136E+06 NUBASE

2419 68-Er-157M 4.5+ 1.554E+05 0.076 s 7.89

IT:100.00

0

1.554E+05 NUBASE

2420 68-Er-158 0.0+ 2.29 h 2.62

β+m:100.00

0

4.099E+04 8.198E+04 NUBASE

2421 68-Er-159 1.5- 36 m 2.78

β+:76.43; β+

m:23.57

4

6.804E+04 7.412E+05 ENSDF

2422 68-Er-160 0.0+ 1.191 d 0.31

β+m:100.00

0

1.350E+04 2.700E+04 NUBASE

2423 68-Er-161 1.5- 3.21 h 0.93

β+:73.40; β+

m:26.60

0

6.459E+05 6.459E+05 NUBASE

2424 68-Er-162 0.0+ 1.4E+14 y 100

α:50.00; 2β+:50.00

0

9.219E+05 8.220E+05 NUBASE

2425 68-Er-163 2.5- 1.25 h 0.53

β+:99.98; β+

m:0.02

4

5.270E+03 4.018E+04 ENSDF

2426 68-Er-164 0.0+

NUBASE

2427 68-Er-165 2.5- 10.36 h 0.39

β+:100.00

3

5.178E+03 3.783E+04 ENSDF

2428 68-Er-166 0.0+

NUBASE

2429 68-Er-167 3.5+

NUBASE

2430 68-Er-167M 0.5- 2.078E+05 2.27 s 0.26

IT:100.00

3

1.101E+05 9.759E+04 UKPADD67

110 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 111: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2431 68-Er-168 0.0+

NUBASE

2432 68-Er-169 0.5- 9.4 d 0.21

β-:100.00

4

1.018E+05 1.981E+01 LNHB

2433 68-Er-170 0.0+

NUBASE

2434 68-Er-171 2.5- 7.516 h 0.03

β-:100.00

4

4.164E+05 3.726E+05 ENSDF

2435 68-Er-172 0.0+ 2.054 d 0.61

β-:100.00

4

1.287E+05 5.157E+05 UKPADD67

2436 68-Er-173 3.5- 1.4 m 7.14

β-:100.00

4

6.975E+05 8.303E+05 ENSDF

2437 68-Er-174 0.0+ 3.2 m 6.25

β-:100.00

0

6.400E+05 6.400E+05 NUBASE

2438 68-Er-175 4.5+ 1.2 m 25

β-:100.00

0

1.223E+06 1.223E+06 NUBASE

2439 68-Er-176 0.0+ 20 s 100

β-:100.00

0

9.567E+05 9.567E+05 NUBASE

2440 68-Er-177 0.5- 3 s 100

β-:100.00

0

1.557E+06 1.557E+06 NUBASE

2441 69-Tm-145 5.5- 3.1E-06 s 9.68

p:100.00

0

1.741E+06 NUBASE

2442 69-Tm-146 6.0- 0.24 s 12.50

p:100.00

0

1.121E+06 NUBASE

2443 69-Tm-146M 10.0+ 7.100E+04 0.072 s 31.94

p:84.00; β+:16.00

0

7.201E+05 7.201E+05 1.001E+06 NUBASE

2444 69-Tm-147 5.5- 0.58 s 5.17

β+m:85.00; p:15.00

0

2.998E+06 2.998E+06 1.576E+05 NUBASE

2445 69-Tm-148 10.0+ 0.7 s 28.57

β+:100.00

0

4.127E+06 4.127E+06 NUBASE

2446 69-Tm-149 5.5- 0.9 s 22.22

β+m:99.74; β+,p:0.09;

β+,pm:0.09; β+,pn:0.09

0

2.983E+06 2.983E+06 4.113E+03 NUBASE

2447 69-Tm-150 1.0+ 3 s 100

β+:100.00

0

3.741E+06 3.741E+06 NUBASE

2448 69-Tm-150M 6.0- 1.400E+05 2.2 s 2.73

β+:98.80; β+,p:0.60;

β+,pm:0.60

0

3.766E+06 3.766E+06 2.371E+04 NUBASE

2449 69-Tm-150N 10.0+ 8.100E+05 5.2E-03 s 5.77

ITm:100.00

0

6.700E+05 NUBASE

2450 69-Tm-151 5.5- 4.17 s 2.40

β+:100.00

4

1.557E+06 2.557E+06 ENSDF

2451 69-Tm-151M 0.5+ 5.000E+04 6.6 s 21.21

β+:100.00

4

1.425E+06 2.945E+06 ENSDF

2452 69-Tm-152 2.0- 8 s 12.50

β+:100.00

0

2.910E+06 2.910E+06 NUBASE

2453 69-Tm-152M 9.0+ 1.000E+05 5.2 s 11.54

β+:100.00

0

2.943E+06 2.943E+06 NUBASE

2454 69-Tm-153 5.5- 1.48 s 0.68

α:91.00; β+:9.00

5

1.583E+05 1.256E+05 4.769E+06 ENSDF

2455 69-Tm-153M 0.5+ 4.320E+04 2.5 s 8

α m:92.00; β+:8.00

0

1.738E+05 1.738E+05 4.823E+06 NUBASE

2456 69-Tm-154 2.0- 8.1 s 3.70

α:54.00; β+:46.00

0

1.255E+06 1.255E+06 2.751E+06 NUBASE

2457 69-Tm-154M 9.0+ 7.000E+04 3.3 s 2.12

α m:58.00; β+:42.00

0

1.155E+06 1.155E+06 2.995E+06 NUBASE

2458 69-Tm-155 5.5- 21.6 s 0.93

β+:99.10; α:0.90

0

1.843E+06 1.843E+06 4.115E+04 NUBASE

2459 69-Tm-155M 0.5+ 4.100E+04 45 s 6.67

β+:98.00; α m:2.00

0

1.836E+06 1.836E+06 9.144E+04 NUBASE

2460 69-Tm-156 2.0- 1.397 m 2.15

β+:99.94; α:0.06

0

2.456E+06 2.456E+06 2.780E+03 NUBASE

2461 69-Tm-157 0.5+ 3.63 m 2.48

β+:100.00

0

1.570E+06 1.570E+06 NUBASE

2462 69-Tm-158 2.0- 3.98 m 1.51

β+:100.00

4

1.557E+06 1.555E+06 ENSDF

2463 69-Tm-159 2.5+ 9.13 m 1.75

β+:100.00

0

1.332E+06 1.332E+06 NUBASE

2464 69-Tm-160 1.0- 9.4 m 3.19

β+:100.00

0

1.919E+06 1.919E+06 NUBASE

2465 69-Tm-160M 5.0+ 7.000E+04 1.242 m 2.01

IT:85.00; β+:15.00

0

2.914E+05 3.509E+05 NUBASE

2466 69-Tm-161 3.5+ 30.2 m 2.65

β+:100.00

0

1.103E+06 1.103E+06 NUBASE

2467 69-Tm-161M 0.5+ 7.400E+03 5 m 100

β+:50.00; IT:50.00

0

5.529E+05 5.566E+05 NUBASE

2468 69-Tm-162 1.0- 21.7 m 0.88

β+:100.00

0

1.620E+06 1.620E+06 NUBASE

2469 69-Tm-162M 5.0+ 1.300E+05 24.3 s 7

IT:82.00; β+:18.00

0

2.993E+05 4.059E+05 NUBASE

2470 69-Tm-163 0.5+ 1.81 h 0.28

β+:100.00

0

8.130E+05 8.130E+05 NUBASE

2471 69-Tm-164 1.0+ 2 m 5

β+:100.00

4

5.440E+05 7.176E+05 ENSDF

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 111

MAIN DATA TABLES

Page 112: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2472 69-Tm-164M 6.0- 1.000E+04 5.1 m 1.96

IT:80.00; β+:20.00

0

2.715E+05 2.795E+05 NUBASE

2473 69-Tm-165 0.5+ 1.252 d 0.10

β+:100.00

4

5.595E+04 5.464E+05 ENSDF

2474 69-Tm-166 2.0+ 7.7 h 0.39

β+:100.00

4

8.115E+04 1.956E+06 ENSDF

2475 69-Tm-166M 6.0- 1.220E+05 0.34 s 7.35

IT:100.00

0

1.220E+05 NUBASE

2476 69-Tm-167 0.5+ 9.246 d 0.15

β+:1.71; β+

m:98.29

4

2.156E+04 5.162E+04 UKPADD67

2477 69-Tm-168 3.0+ 90 d 4.44

β-:0.01; β+:99.99

5

8.308E+04 1.210E+06 UKPADD67

2478 69-Tm-169 0.5+

NUBASE

2479 69-Tm-170 1.0- 128.6 d 0.23

β+:0.13; β-:99.87

5

3.275E+05 4.185E+03 ENSDF

2480 69-Tm-171 0.5+ 1.917 y 0.71

β-:100.00

4

2.556E+04 6.821E+02 UKPADD67

2481 69-Tm-172 2.0- 2.65 d 0.31

β-:100.00

4

5.277E+05 4.805E+05 UKPADD67

2482 69-Tm-173 0.5+ 8.24 h 0.97

β-:100.00

4

3.097E+05 3.884E+05 ENSDF

2483 69-Tm-174 4.0- 5.4 m 1.85

β-:100.00

4

5.139E+05 1.779E+06 ENSDF

2484 69-Tm-175 0.5+ 15.2 m 3.29

β-:23.00; β-

m:77.00

0

6.614E+05 6.614E+05 NUBASE

2485 69-Tm-176 4.0+ 1.85 m 1.62

β-:50.00; β-

m:50.00

0

1.200E+06 1.200E+06 NUBASE

2486 69-Tm-177 3.5- 1.5 m 6.67

β-m:100.00

0

1.063E+06 1.063E+06 NUBASE

2487 69-Tm-178 ? 30 s 100

β-:100.00

0

1.859E+06 1.859E+06 NUBASE

2488 69-Tm-179 0.5+ 20 s 100

β-:100.00

0

1.607E+06 1.607E+06 NUBASE

2489 70-Yb-148 0.0+ 0.25 s 60

β+:100.00

0

2.973E+06 2.973E+06 NUBASE

2490 70-Yb-149 ? 0.7 s 28.57

β+:100.00

0

3.513E+06 3.513E+06 NUBASE

2491 70-Yb-150 0.0+ 0.7 s 42.86

β+:100.00

0

2.627E+06 2.627E+06 NUBASE

2492 70-Yb-151 0.5+ 1.6 s 31.25

β+m:100.00

0

3.050E+06 3.050E+06 NUBASE

2493 70-Yb-151M 5.5- 7.500E+05 1.6 s 6.25

β+:99.60; IT:0.40

0

3.317E+06 3.320E+06 NUBASE

2494 70-Yb-152 0.0+ 3.04 s 1.97

β+:100.00

4

1.206E+06 1.163E+06 ENSDF

2495 70-Yb-153 3.5- 4.2 s 4.76

β+:25.00; β+

m:25.00;

α:25.00; α m:25.00;

β+,p:0.01

0

1.156E+06 1.156E+06 1.943E+06 NUBASE

2496 70-Yb-154 0.0+ 0.409 s 0.49

α:92.60; β+:7.40

0

1.109E+05 1.109E+05 5.069E+06 NUBASE

2497 70-Yb-155 3.5- 1.793 s 1.06

α:89.00; β+:5.50;

β+m:5.50

0

2.241E+05 2.241E+05 4.751E+06 NUBASE

2498 70-Yb-156 0.0+ 26.1 s 2.68

β+:90.00; α:10.00

0

1.073E+06 1.073E+06 4.811E+05 NUBASE

2499 70-Yb-157 3.5- 38.6 s 2.59

β+:99.50; α:0.50

0

1.747E+06 1.747E+06 2.311E+04 NUBASE

2500 70-Yb-158 0.0+ 1.49 m 8.72

β+:100.00; α:~

0

8.960E+05 8.960E+05 8.761E+01 NUBASE

2501 70-Yb-159 2.5- 1.72 m 5.81

β+:100.00

0

1.576E+06 1.576E+06 NUBASE

2502 70-Yb-160 0.0+ 4.8 m 4.17

β+:100.00

4

5.767E+04 2.706E+05 ENSDF

2503 70-Yb-161 1.5- 4.2 m 4.76

β+m:100.00

0

1.349E+06 1.349E+06 NUBASE

2504 70-Yb-162 0.0+ 18.87 m 1.01

β+:100.00

4

3.152E+04 2.357E+05 ENSDF

2505 70-Yb-163 1.5- 11.05 m 2.26

β+:100.00

0

1.144E+06 1.144E+06 NUBASE

2506 70-Yb-164 0.0+ 1.263 h 2.24

β+:100.00

4

6.027E+03 5.212E+04 ENSDF

2507 70-Yb-165 2.5- 9.9 m 3.03

β+:100.00

0

8.830E+05 8.830E+05 NUBASE

2508 70-Yb-166 0.0+ 2.362 d 0.18

β+m:100.00

0

9.200E+03 1.840E+04 NUBASE

2509 70-Yb-167 2.5- 17.5 m 1.14

β+:100.00

0

6.514E+05 6.514E+05 NUBASE

2510 70-Yb-168 0.0+ 1.3E+14 y 100

α:50.00; 2β+:50.00

0

7.108E+05 9.750E+05 NUBASE

2511 70-Yb-169 3.5+ 32.018 d 0.02

β+:100.00

4

1.118E+05 3.133E+05 LNHB

112 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 113: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2512 70-Yb-169M 0.5- 2.420E+04 46 s 4.35

IT:100.00

0

2.420E+04 NUBASE

2513 70-Yb-170 0.0+

NUBASE

2514 70-Yb-171 0.5-

NUBASE

2515 70-Yb-171M 3.5+ 9.528E+04 5.25E-03 s 4.57

IT:100.00

0

9.528E+04 NUBASE

2516 70-Yb-172 0.0+

NUBASE

2517 70-Yb-173 2.5-

NUBASE

2518 70-Yb-174 0.0+

NUBASE

2519 70-Yb-175 3.5- 4.185 d 0.02

β-:100.00

4

1.216E+05 7.994E+04 UKPADD67

2520 70-Yb-175M 0.5- 5.149E+05 0.068 s 0.44

IT:100.00

0

5.149E+05 NUBASE

2521 70-Yb-176 0.0+

NUBASE

2522 70-Yb-176M 8.0- 1.050E+06 11.4 s 2.63

IT:90.00; β-:10.00

0

3.144E+04 9.764E+05 NUBASE

2523 70-Yb-177 4.5+ 1.911 h 0.16

β-:100.00

4

4.260E+05 1.991E+05 ENSDF

2524 70-Yb-177M 0.5- 3.315E+05 6.41 s 0.31

IT:100.00

3

1.782E+05 1.500E+05 ENSDF

2525 70-Yb-178 0.0+ 1.233 h 4.05

β-:100.00

0

2.150E+05 2.150E+05 NUBASE

2526 70-Yb-179 0.5- 8 m 5

β-m:100.00

0

6.839E+05 6.839E+05 NUBASE

2527 70-Yb-180 0.0+ 2.4 m 20.83

β-m:100.00

0

7.587E+05 7.587E+05 NUBASE

2528 70-Yb-181 1.5- 1 m 100

β-:100.00

0

1.297E+06 1.297E+06 NUBASE

2529 71-Lu-150 ? 0.046 s 13.04

p:70.00; β+:30.00

0

1.379E+06 1.379E+06 8.897E+05 NUBASE

2530 71-Lu-151 5.5- 0.081 s 2.36

p:63.00; β+

m:37.00

0

1.306E+06 1.306E+06 7.818E+05 NUBASE

2531 71-Lu-152 ? 0.65 s 10.77

β+:85.00; β+,p:7.50;

β+,pm:7.50

0

4.028E+06 4.028E+06 3.760E+05 NUBASE

2532 71-Lu-153 5.5- 0.9 s 22.22

α:70.00; β+:30.00

0

8.650E+05 8.650E+05 2.244E+06 NUBASE

2533 71-Lu-153M 0.5+ 8.000E+04 1 s 100

β+:50.00; α:50.00

0

1.455E+06 1.455E+06 1.643E+06 NUBASE

2534 71-Lu-154 2.0- 1 s 100

β+:100.00

0

3.455E+06 3.455E+06 NUBASE

2535 71-Lu-154M 9.0+ 5.800E+04 1.12 s 7.14

β+:100.00; α n:~

0

3.474E+06 3.474E+06 7.726E+01 NUBASE

2536 71-Lu-155 5.5- 0.069 s 2.33

α:90.00; β+:10.00

0

2.650E+05 2.650E+05 5.223E+06 NUBASE

2537 71-Lu-155M 0.5+ 2.000E+04 0.138 s 5.80

α m:76.00; β+:24.00

0

6.375E+05 6.375E+05 4.356E+06 NUBASE

2538 71-Lu-155N 12.5- 1.781E+06 2.7E-03 s 1.11

α:50.00; α m:50.00

0

7.538E+06 NUBASE

2539 71-Lu-156 2.0- 0.494 s 2.43

α:95.00; β+:5.00

0

1.586E+05 1.586E+05 5.315E+06 NUBASE

2540 71-Lu-156M 9.0+ 2.200E+05 0.198 s 1.01

α m:94.00; β+:6.00

0

1.947E+05 1.947E+05 5.372E+06 NUBASE

2541 71-Lu-157 ? 6.8 s 26.47

β+:50.00; α m:50.00

0

1.160E+06 1.160E+06 2.532E+06 NUBASE

2542 71-Lu-157M 5.5- 2.100E+04 4.79 s 2.51

β+:94.00; α:6.00

0

2.187E+06 2.187E+06 3.077E+05 NUBASE

2543 71-Lu-158 2.0- 10.6 s 2.83

β+:99.09; α:0.91

0

2.907E+06 2.907E+06 4.359E+04 NUBASE

2544 71-Lu-159 0.5+ 12.1 s 8.26

β+:99.90; α m:0.10

0

2.042E+06 2.042E+06 4.459E+03 NUBASE

2545 71-Lu-159M 5.5- 1.000E+05 10 s 100

β+:33.33; IT:33.33;

α:33.33

0

6.926E+05 7.259E+05 1.533E+06 NUBASE

2546 71-Lu-160 2.0- 36.1 s 0.83

β+:100.00; α:~

0

2.633E+06 2.633E+06 4.145E+00 NUBASE

2547 71-Lu-160M ? 40 s 2.50

β+:100.00

0

2.633E+06 2.633E+06 NUBASE

2548 71-Lu-161 0.5+ 1.283 m 2.60

β+:100.00

0

1.761E+06 1.761E+06 NUBASE

2549 71-Lu-161M 4.5- 1.660E+05 7.3E-03 s 5.48

IT:100.00

0

1.660E+05 NUBASE

2550 71-Lu-162 1.0- 1.37 m 1.46

β+:100.00

0

2.331E+06 2.331E+06 NUBASE

2551 71-Lu-162M 4.0- 1.200E+05 1.5 m 100

β+:100.00

0

2.371E+06 2.371E+06 NUBASE

2552 71-Lu-162N ? 3.000E+05 1.9 m 100

β+:100.00

0

2.431E+06 2.431E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 113

MAIN DATA TABLES

Page 114: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2553 71-Lu-163 0.5+ 3.97 m 3.27

β+:100.00

0

1.504E+06 1.504E+06 NUBASE

2554 71-Lu-164 1.0- 3.14 m 0.96

β+:100.00

0

2.127E+06 2.127E+06 NUBASE

2555 71-Lu-165 0.5+ 10.74 m 0.93

β+:100.00

0

1.282E+06 1.282E+06 NUBASE

2556 71-Lu-166 6.0- 2.65 m 3.77

β+:100.00

0

1.856E+06 1.856E+06 NUBASE

2557 71-Lu-166M 3.0- 3.437E+04 1.41 m 7.09

β+:58.00; IT:42.00

0

1.083E+06 1.097E+06 NUBASE

2558 71-Lu-166N 0.0- 4.290E+04 2.12 m 4.72

β+:80.00; ITm:20.00

0

1.496E+06 1.498E+06 NUBASE

2559 71-Lu-167 3.5+ 51.5 m 1.94

β+:100.00

0

1.031E+06 1.031E+06 NUBASE

2560 71-Lu-167M 0.5- 1 m 100

IT:50.00; β+:50.00

0

5.157E+05 5.157E+05 NUBASE

2561 71-Lu-168 6.0- 5.5 m 1.82

β+:100.00

0

1.505E+06 1.505E+06 NUBASE

2562 71-Lu-168M 3.0+ 2.200E+05 6.7 m 5.97

β+:95.00; IT:5.00

0

1.499E+06 1.510E+06 NUBASE

2563 71-Lu-169 3.5+ 1.419 d 0.15

β+:86.40; β+

m:13.60

0

7.632E+05 7.632E+05 NUBASE

2564 71-Lu-169M 0.5- 2.900E+04 2.667 m 6.25

IT:100.00

0

2.900E+04 NUBASE

2565 71-Lu-170 0.0+ 2.012 d 0.99

β+:100.00

0

1.153E+06 1.153E+06 NUBASE

2566 71-Lu-170M 4.0- 9.291E+04 0.67 s 14.93

IT:100.00

0

9.291E+04 NUBASE

2567 71-Lu-171 3.5+ 8.25 d 0.36

β+:100.00

4

8.833E+04 6.413E+05 UKPADD67

2568 71-Lu-171M 0.5- 7.120E+04 1.3 m 2.56

IT:100.00

3

6.944E+04 1.787E+03 UKPADD67

2569 71-Lu-172 4.0- 6.7 d 0.15

β+:100.00

4

1.114E+05 1.955E+06 UKPADD67

2570 71-Lu-172M 1.0- 4.186E+04 3.7 m 13.51

IT:100.00

3

4.020E+04 1.667E+03 UKPADD67

2571 71-Lu-173 3.5+ 1.336 y 2.66

β+:100.00

4

4.618E+04 1.702E+05 UKPADD67

2572 71-Lu-174 1.0- 3.559 y 11.54

β+:100.00

4

4.482E+04 1.167E+05 UKPADD67

2573 71-Lu-174M 6.0- 1.708E+05 142 d 2.11

β+:0.58; IT:99.42

4

1.169E+05 6.167E+04 UKPADD67

2574 71-Lu-175 3.5+

NUBASE

2575 71-Lu-176 7.0- 4E+10 y 5.50

β-:100.00

4

2.982E+05 4.799E+05 ENSDF

2576 71-Lu-176M 1.0- 1.270E+05 3.635 h 0.33

β+:0.10; β-:99.91

5

4.662E+05 1.423E+04 LNHB

2577 71-Lu-177 3.5+ 6.647 d 0.60

β-:100.00

4

1.473E+05 3.343E+04 LNHB

2578 71-Lu-177M 11.5- 9.702E+05 160.3 d 0.25

β-m:77.40; IT:22.60

4

8.208E+04 1.678E+05 UKPADD67

2579 71-Lu-177N 19.5- 3.900E+06 7 m 28.57

β-n:50.00; ITm:50.00

0

2.768E+05 1.742E+06 NUBASE

2580 71-Lu-178 1.0+ 28.4 m 0.70

β-:100.00

4

7.555E+05 1.232E+05 ENSDF

2581 71-Lu-178M 9.0- 1.237E+05 23.1 m 1.30

β-m:100.00

0

3.592E+05 3.592E+05 NUBASE

2582 71-Lu-179 3.5+ 4.59 h 1.31

β-:100.00

4

4.862E+05 2.942E+04 ENSDF

2583 71-Lu-179M 0.5+ 5.924E+05 3.1E-03 s 29.03

IT:100.00

0

5.924E+05 NUBASE

2584 71-Lu-180 3.0+ 5.7 m 1.75

β-:100.00

4

5.918E+05 1.453E+06 ENSDF

2585 71-Lu-180M 3.0- 1.390E+04 1 s 100

β-:50.00; IT:50.00

0

5.187E+05 5.257E+05 NUBASE

2586 71-Lu-180N 9.0- 6.240E+05 1E-03 s 100

β-m:50.00; IT:50.00

0

4.302E+05 7.422E+05 NUBASE

2587 71-Lu-181 3.5+ 3.5 m 8.57

β-:100.00

0

8.906E+05 8.906E+05 NUBASE

2588 71-Lu-182 ? 2 m 10

β-:100.00

0

1.393E+06 1.393E+06 NUBASE

2589 71-Lu-183 3.5+ 58 s 6.90

β-:100.00

4

1.123E+06 6.514E+05 ENSDF

2590 71-Lu-184 3.0+ 20 s 15

β-:50.00; β-

m:50.00

0

1.485E+06 1.485E+06 NUBASE

2591 72-Hf-153 0.5+ 0.4 s 100

β+m:100.00

0

3.677E+06 3.677E+06 NUBASE

2592 72-Hf-153M 5.5- 7.500E+05 0.5 s 100

β+:50.00; IT:50.00

0

1.977E+06 2.352E+06 NUBASE

2593 72-Hf-154 0.0+ 2 s 50

β+:100.00

0

2.280E+06 2.280E+06 NUBASE

2594 72-Hf-155 3.5- 0.89 s 13.48

β+:50.00; β+

m:50.00

0

2.815E+06 2.815E+06 NUBASE

2595 72-Hf-156 0.0+ 0.023 s 4.35

α:97.00; β+:3.00

0

5.900E+04 5.900E+04 5.854E+06 NUBASE

114 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 115: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2596 72-Hf-157 3.5- 0.115 s 0.87

α:86.00; β+:7.00;

β+m:7.00

0

3.604E+05 3.604E+05 5.061E+06 NUBASE

2597 72-Hf-158 0.0+ 2.85 s 2.46

β+:55.70; α:44.30

0

9.488E+05 9.488E+05 2.394E+06 NUBASE

2598 72-Hf-159 3.5- 5.2 s 1.92

β+:65.00; α:35.00

0

1.485E+06 1.485E+06 1.828E+06 NUBASE

2599 72-Hf-160 0.0+ 13.6 s 1.47

β+:99.30; α:0.70

0

1.434E+06 1.434E+06 3.431E+04 NUBASE

2600 72-Hf-161 1.5- 18.2 s 2.75

β+:99.87; α:0.13

0

2.078E+06 2.078E+06 6.108E+03 NUBASE

2601 72-Hf-162 0.0+ 39.4 s 2.28

β+:99.99; α:0.01

0

1.222E+06 1.222E+06 3.534E+02 NUBASE

2602 72-Hf-163 1.5- 40 s 1.50

β+:100.00; α:~

0

1.835E+06 1.835E+06 4.132E+00 NUBASE

2603 72-Hf-164 0.0+ 1.85 m 7.21

β+:100.00

0

9.400E+05 9.400E+05 NUBASE

2604 72-Hf-165 2.5- 1.267 m 5.26

β+:100.00

0

1.602E+06 1.602E+06 NUBASE

2605 72-Hf-166 0.0+ 6.77 m 4.43

β+m:64.56; β+

n:35.44

0

7.082E+05 7.082E+05 NUBASE

2606 72-Hf-167 2.5- 2.05 m 2.44

β+:50.00; β+

m:50.00

0

1.344E+06 1.344E+06 NUBASE

2607 72-Hf-168 0.0+ 25.95 m 0.77

β+m:100.00

0

4.930E+05 4.930E+05 NUBASE

2608 72-Hf-169 2.5- 3.24 m 1.23

β+:96.50; β+

m:3.50

0

1.120E+06 1.120E+06 NUBASE

2609 72-Hf-170 0.0+ 16.01 h 0.81

β+:99.93; β+

m:0.07

0

5.280E+04 1.056E+05 NUBASE

2610 72-Hf-171 3.5+ 12.1 h 3.31

β+:100.00

0

8.008E+05 8.008E+05 NUBASE

2611 72-Hf-171M 0.5- 2.193E+04 29.5 s 3.05

IT:100.00

0

2.193E+04 NUBASE

2612 72-Hf-172 0.0+ 1.87 y 1.60

β+m:100.00

4

6.865E+04 1.093E+05 ENSDF

2613 72-Hf-173 0.5- 23.9 h 1.26

β+:100.00

4

5.205E+04 3.966E+05 UKPADD67

2614 72-Hf-174 0.0+ 2E+15 y 20

α:100.00

1

2.504E+06 UKPADD67

2615 72-Hf-175 2.5- 70 d 1.43

β+:100.00

4

4.551E+04 3.630E+05 UKPADD67

2616 72-Hf-176 0.0+

NUBASE

2617 72-Hf-177 3.5-

NUBASE

2618 72-Hf-177M 11.5+ 1.315E+06 1.08 s 5.56

IT:100.00

3

2.407E+05 1.068E+06 UKPADD67

2619 72-Hf-177N 18.5- 2.740E+06 51.4 m 0.97

ITm:100.00

3

2.515E+05 1.177E+06 UKPADD67

2620 72-Hf-178 0.0+

NUBASE

2621 72-Hf-178M 8.0- 1.147E+06 4 s 7.50

IT:100.00

3

1.415E+05 1.006E+06 UKPADD67

2622 72-Hf-178N 16.0+ 2.446E+06 31.001 y 3.23

ITm:100.00

3

7.362E+04 1.223E+06 UKPADD67

2623 72-Hf-179 4.5+

NUBASE

2624 72-Hf-179M 0.5- 3.750E+05 18.67 s 0.16

IT:100.00

3

1.341E+05 2.407E+05 UKPADD67

2625 72-Hf-179N 12.5- 1.106E+06 25.1 d 0.80

IT:100.00

3

1.863E+05 9.190E+05 UKPADD67

2626 72-Hf-180 0.0+

NUBASE

2627 72-Hf-180M 8.0- 1.141E+06 5.5 h 1.82

β-m:0.31; IT:99.69

4

1.486E+05 9.924E+05 UKPADD67

2628 72-Hf-181 0.5- 42.38 d 0.14

β-:100.00

4

2.044E+05 5.305E+05 UKPADD67

2629 72-Hf-182 0.0+ 9E+06 y 22.22

β-:100.00

4

3.215E+04 2.394E+05 ENSDF

2630 72-Hf-182M 8.0- 1.173E+06 1.025 h 2.44

β-n:58.00; IT:42.00

0

1.987E+05 6.913E+05 NUBASE

2631 72-Hf-183 1.5- 1.067 h 1.59

β-:100.00

0

6.687E+05 6.687E+05 NUBASE

2632 72-Hf-184 0.0+ 4.12 h 1.21

β-:100.00

0

4.470E+05 4.470E+05 NUBASE

2633 72-Hf-184M 8.0- 1.272E+06 48 s 20.83

β-:100.00

0

8.711E+05 8.711E+05 NUBASE

2634 72-Hf-185 1.5- 3.5 m 17.14

β-:100.00

0

1.012E+06 1.012E+06 NUBASE

2635 72-Hf-186 0.0+ 2.6 m 46.15

β-:100.00

0

7.267E+05 7.267E+05 NUBASE

2636 72-Hf-187 1.5- 30 s 100

β-:100.00

0

1.263E+06 1.263E+06 NUBASE

2637 72-Hf-188 0.0+ 20 s 100

β-:100.00

0

9.767E+05 9.767E+05 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 115

MAIN DATA TABLES

Page 116: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2638 73-Ta-155 5.5- 1.3E-05 s 30.77

p:100.00

0

1.771E+06 NUBASE

2639 73-Ta-156 2.0- 0.144 s 16.67

p:100.00

0

1.011E+06 NUBASE

2640 73-Ta-156M 9.0+ 1.000E+05 0.36 s 11.11

β+:95.80; p:4.20

0

3.880E+06 3.880E+06 4.666E+04 NUBASE

2641 73-Ta-157 0.5+ 0.01 s 3.96

α:95.60; p:3.40;

β+:1.00

0

3.040E+04 3.040E+04 6.107E+06 NUBASE

2642 73-Ta-157M 5.5- 2.200E+04 4.3E-03 s 2.33

α m:99.00; β+:1.00

0

3.047E+04 3.047E+04 6.234E+06 NUBASE

2643 73-Ta-157N 12.5- 1.593E+06 1.7E-03 s 5.88

α m:100.00

0

7.868E+06 NUBASE

2644 73-Ta-158 2.0- 0.049 s 16.33

α:96.00; β+:4.00

0

1.478E+05 1.478E+05 5.880E+06 NUBASE

2645 73-Ta-158M 9.0+ 1.400E+05 0.036 s 2.22

α m:93.00; β+:3.50;

IT:3.50

0

1.309E+05 1.358E+05 5.773E+06 NUBASE

2646 73-Ta-159 0.5+ 1.04 s 8.65

β+:66.00; α:34.00

0

1.849E+06 1.849E+06 1.932E+06 NUBASE

2647 73-Ta-159M 5.5- 6.400E+04 0.514 s 3.89

α m:55.00; β+:45.00

0

1.270E+06 1.270E+06 3.149E+06 NUBASE

2648 73-Ta-160 2.0- 1.7 s 11.76

β+:50.00; α:50.00

0

1.676E+06 1.676E+06 2.723E+06 NUBASE

2649 73-Ta-160M 9.0+ 3.100E+05 1.55 s 2.58

β+:66.00; α m:34.00

0

2.281E+06 2.281E+06 1.882E+06 NUBASE

2650 73-Ta-161 0.5+ 3 s 100

β+:50.00; α:50.00

0

1.265E+06 1.265E+06 2.664E+06 NUBASE

2651 73-Ta-161M 5.5- 5.000E+04 2.89 s 4.15

β+:95.00; α m:5.00

0

2.419E+06 2.419E+06 2.679E+05 NUBASE

2652 73-Ta-162 3.0+ 3.57 s 3.36

β+:99.93; α:0.07

0

3.129E+06 3.129E+06 3.707E+03 NUBASE

2653 73-Ta-163 0.5+ 10.6 s 16.98

β+:99.80; α:0.10;

α m:0.10

0

2.244E+06 2.244E+06 9.390E+03 NUBASE

2654 73-Ta-164 3.0+ 14.2 s 2.11

β+:100.00

4

2.739E+06 1.617E+06 ENSDF

2655 73-Ta-165 2.5- 31 s 4.84

β+:100.00

0

1.927E+06 1.927E+06 NUBASE

2656 73-Ta-166 2.0+ 34.4 s 1.45

β+:100.00

0

2.587E+06 2.587E+06 NUBASE

2657 73-Ta-167 1.5+ 1.33 m 5.26

β+:100.00

0

1.706E+06 1.706E+06 NUBASE

2658 73-Ta-168 ? 2 m 5

β+:100.00

0

2.322E+06 2.322E+06 NUBASE

2659 73-Ta-169 2.5+ 4.9 m 8.16

β+:100.00

0

1.476E+06 1.476E+06 NUBASE

2660 73-Ta-170 3.0+ 6.76 m 0.89

β+:100.00

4

1.598E+06 1.056E+06 ENSDF

2661 73-Ta-171 2.5- 23.3 m 1.29

β+:50.00; β+

m:50.00

0

1.233E+06 1.233E+06 NUBASE

2662 73-Ta-172 3.0+ 36.8 m 0.82

β+:100.00

4

4.243E+05 1.732E+06 ENSDF

2663 73-Ta-173 2.5- 3.14 h 4.14

β+:100.00

4

1.247E+05 4.093E+05 ENSDF

2664 73-Ta-174 3.0+ 1.14 h 7.02

β+:100.00

4

3.615E+05 8.373E+05 ENSDF

2665 73-Ta-175 3.5+ 10.5 h 1.90

β+:100.00

0

6.916E+05 6.916E+05 NUBASE

2666 73-Ta-176 1.0- 8.09 h 0.62

β+:100.00

4

7.009E+04 2.099E+06 ENSDF

2667 73-Ta-176M 0.0+ 1.030E+05 1.1E-03 s 9.09

IT:100.00

0

1.030E+05 NUBASE

2668 73-Ta-176N 20.0- 2.820E+06 9.7E-04 s 7.22

ITm:100.00

0

2.717E+06 NUBASE

2669 73-Ta-177 3.5+ 2.35 d 0.89

β+:100.00

4

2.272E+04 6.775E+04 UKPADD67

2670 73-Ta-178 1.0+ 9.29 m 0.43

β+:100.00

4

2.748E+04 1.189E+05 LNHB

2671 73-Ta-178M 7.0- 2.36 h 3.39

β+m:100.00

0

2.633E+05 2.633E+05 NUBASE

2672 73-Ta-178N 15.0- 1.471E+06 0.059 s 5.08

ITm:100.00

0

1.471E+06 NUBASE

2673 73-Ta-179 3.5+ 1.61 y 1.70

β+:100.00

3

7.395E+03 2.925E+04 UKPADD67

2674 73-Ta-179M 12.5+ 1.317E+06 9E-03 s 2.22

IT:100.00

0

1.317E+06 NUBASE

2675 73-Ta-179N 18.5+ 2.639E+06 0.054 s 3.14

ITm:100.00

0

1.322E+06 NUBASE

2676 73-Ta-180 1.0+ 8.08 h 0.62

β-:18.10; β+:81.90

5

6.406E+04 4.593E+04 UKPADD67

2677 73-Ta-180M 9.0- 7.500E+04 1.8E+15 y 33.33

β-:20.00; β+:80.00

5

1.259E+05 5.625E+05 UKPADD67

116 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 117: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2678 73-Ta-181 3.5+

NUBASE

2679 73-Ta-182 3.0- 114.7 d 0.35

β-:100.00

4

2.163E+05 1.283E+06 UKPADD67

2680 73-Ta-182M 5.0+ 1.626E+04 0.283 s 1.06

IT:100.00

3

1.432E+04 1.917E+03 UKPADD67

2681 73-Ta-182N 10.0- 5.196E+05 15.84 m 0.63

ITm:100.00

3

2.444E+05 2.546E+05 UKPADD67

2682 73-Ta-183 3.5+ 5.09 d 1.38

β-:96.60; β-

m:3.40

4

3.494E+05 2.866E+05 UKPADD67

2683 73-Ta-184 5.0- 8.7 h 1.15

β-:100.00

0

9.554E+05 9.554E+05 NUBASE

2684 73-Ta-185 3.5+ 49 m 4.08

β-:100.00

4

7.341E+05 1.374E+05 ENSDF

2685 73-Ta-185M 10.5- 1.308E+06 1E-03 s 100

IT:100.00

0

1.308E+06 NUBASE

2686 73-Ta-186 ? 10.5 m 2.86

β-:100.00

0

1.300E+06 1.300E+06 NUBASE

2687 73-Ta-187 3.5+ 2 m 100

β-:100.00

0

1.045E+06 1.045E+06 NUBASE

2688 73-Ta-188 ? 20 s 100

β-:100.00

0

1.619E+06 1.619E+06 NUBASE

2689 73-Ta-189 3.5+ 3 s 100

β-:100.00

0

1.217E+06 1.217E+06 NUBASE

2690 73-Ta-190 ? 0.3 s 100

β-:100.00

0

1.880E+06 1.880E+06 NUBASE

2691 74-W -158 0.0+ 1.37E-03 s 12.41

α:100.00

0

6.605E+06 NUBASE

2692 74-W -159 3.5- 8.2E-03 s 8.54

α:82.00; β+:9.00;

β+m:9.00

0

5.512E+05 5.512E+05 5.285E+06 NUBASE

2693 74-W -160 0.0+ 0.09 s 5.56

α:87.00; β+:13.00

0

2.825E+05 2.825E+05 5.277E+06 NUBASE

2694 74-W -161 3.5- 0.409 s 3.91

α:73.00; β+:13.50;

β+m:13.50

0

7.466E+05 7.466E+05 4.318E+06 NUBASE

2695 74-W -162 0.0+ 1.36 s 5.15

β+:54.80; α:45.20

0

1.055E+06 1.055E+06 2.566E+06 NUBASE

2696 74-W -163 1.5- 2.8 s 7.14

β+:87.00; α:13.00

0

2.213E+06 2.213E+06 7.175E+05 NUBASE

2697 74-W -164 0.0+ 6.3 s 3.17

β+:96.20; α:3.80

0

1.619E+06 1.619E+06 2.006E+05 NUBASE

2698 74-W -165 1.5- 5.1 s 9.80

β+:99.80; α:0.20

0

2.326E+06 2.326E+06 1.006E+04 NUBASE

2699 74-W -166 0.0+ 19.2 s 3.12

β+:99.97; α:0.03

0

1.402E+06 1.402E+06 1.700E+03 NUBASE

2700 74-W -167 1.5- 19.9 s 2.51

β+:99.96; α:0.04

0

2.086E+06 2.086E+06 1.909E+03 NUBASE

2701 74-W -168 0.0+ 51 s 3.92

β+:100.00; α:~

0

1.168E+06 1.168E+06 1.442E+02 NUBASE

2702 74-W -169 2.5- 1.267 m 7.89

β+:100.00

0

1.791E+06 1.791E+06 NUBASE

2703 74-W -170 0.0+ 2.42 m 1.65

β+:99.00; α:1.00

0

9.388E+05 9.388E+05 4.141E+04 NUBASE

2704 74-W -171 2.5- 2.38 m 1.68

β+:100.00

0

1.545E+06 1.545E+06 NUBASE

2705 74-W -172 0.0+ 6.6 m 13.64

β+:100.00

0

7.443E+05 7.443E+05 NUBASE

2706 74-W -173 2.5- 7.6 m 2.63

β+:100.00

0

1.223E+06 1.223E+06 NUBASE

2707 74-W -174 0.0+ 33.2 m 6.33

β+:100.00

0

5.047E+05 5.047E+05 NUBASE

2708 74-W -175 0.5- 35.2 m 1.70

β+:100.00

0

9.253E+05 9.253E+05 NUBASE

2709 74-W -176 0.0+ 2.5 h 4

β+:100.00

4

5.730E+04 1.715E+05 UKPADD67

2710 74-W -177 0.5- 2.2 h 1.52

β+:100.00

4

8.187E+04 8.153E+05 ENSDF

2711 74-W -178 0.0+ 21.6 d 1.39

β+:100.00

3

6.995E+03 1.916E+04 UKPADD67

2712 74-W -179 3.5- 37.05 m 0.43

β+:100.00

4

1.288E+04 5.405E+04 ENSDF

2713 74-W -179M 0.5- 2.219E+05 6.4 m 1.09

IT:99.72; β+:0.28

0

1.199E+03 2.225E+05 NUBASE

2714 74-W -180 0.0+

NUBASE

2715 74-W -180M 8.0- 1.529E+06 5.47E-03 s 1.65

IT:100.00

0

1.529E+06 NUBASE

2716 74-W -181 4.5+ 120.98 d 0.10

β+:100.00

4

1.268E+04 4.121E+04 UKPADD67

2717 74-W -182 0.0+

NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 117

MAIN DATA TABLES

Page 118: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2718 74-W -183 0.5- 1.1E+17 y 100

α:33.40; α m:33.30;

α n:33.30

0

1.187E+06 NUBASE

2719 74-W -183M 5.5+ 3.095E+05 5.25 s 1.33

IT:100.00

3

1.840E+05 1.254E+05 UKPADD67

2720 74-W -184 0.0+ 4E+17 y 100

α:100.00

0

1.656E+06 NUBASE

2721 74-W -185 1.5- 75.1 d 0.40

β-:100.00

4

1.268E+05 5.016E+01 UKPADD67

2722 74-W -185M 5.5+ 1.974E+05 1.667 m 2

IT:100.00

3

1.720E+05 2.574E+04 UKPADD67

2723 74-W -186 0.0+ 5.9E+17 y 100

2β-:50.00; α:50.00

0

2.450E+05 5.623E+05 NUBASE

2724 74-W -186M 16.0+ 3.543E+06 3E-03 s 100

IT:100.00

0

3.543E+06 NUBASE

2725 74-W -187 1.5- 23.85 h 0.34

β-:100.00

4

3.013E+05 4.421E+05 UKPADD67

2726 74-W -188 0.0+ 69.78 d 0.07

β-:100.00

4

9.959E+04 1.913E+03 UKPADD67

2727 74-W -189 1.5- 10.7 m 4.67

β-:100.00

0

8.327E+05 8.327E+05 NUBASE

2728 74-W -190 0.0+ 30 m 5

β-:100.00

4

4.669E+05 1.498E+05 ENSDF

2729 74-W -190M 10.0- 2.381E+06 3.1E-03 s 100

IT:100.00

0

2.381E+06 NUBASE

2730 74-W -191 1.5- 20 s 100

β-:100.00

0

1.080E+06 1.080E+06 NUBASE

2731 74-W -192 0.0+ 10 s 100

β-:100.00

0

6.867E+05 6.867E+05 NUBASE

2732 75-Re-160 2.0- 8.6E-04 s 13.95

p:91.00; α:9.00

0

1.770E+06 NUBASE

2733 75-Re-161 0.5+ 0.015 s 26.67

α:100.00

1

6.439E+06 ENSDF

2734 75-Re-161M 5.5- 1.238E+05 0.016 s 5.77

α m:95.20; p:4.80

0

6.182E+06 NUBASE

2735 75-Re-162 2.0- 0.107 s 12.15

α:94.00; β+:6.00

0

2.330E+05 2.330E+05 5.870E+06 NUBASE

2736 75-Re-162M 9.0+ 1.730E+05 0.077 s 11.69

α m:91.00; β+:9.00

0

3.548E+05 3.548E+05 5.713E+06 NUBASE

2737 75-Re-163 0.5+ 0.39 s 17.95

β+:68.00; α:32.00

0

2.018E+06 2.018E+06 1.925E+06 NUBASE

2738 75-Re-163M 5.5- 1.150E+05 0.214 s 2.34

α m:66.00; β+:34.00

0

1.022E+06 1.022E+06 4.004E+06 NUBASE

2739 75-Re-164 ? 1E-09 s 100

α m:100.00

0

5.505E+06 NUBASE

2740 75-Re-164M 2.0- 2.200E+05 0.53 s 43.40

α:58.00; β+:42.00

0

1.514E+06 1.514E+06 3.500E+06 NUBASE

2741 75-Re-165 0.5+ 1 s 100

β+:50.00; α:50.00

0

1.368E+06 1.368E+06 2.824E+06 NUBASE

2742 75-Re-165M 5.5- 4.700E+04 2.1 s 14.29

β+:87.00; α m:13.00

0

2.393E+06 2.393E+06 7.339E+05 NUBASE

2743 75-Re-166 2.0- 2 s 100

β+:50.00; α:50.00

0

1.674E+06 1.674E+06 2.753E+06 NUBASE

2744 75-Re-166M 9.0+ 2.500E+05 2.5 s 8

β+:95.00; α:5.00

0

3.259E+06 3.259E+06 2.878E+05 NUBASE

2745 75-Re-167 4.5- 3.4 s 11.76

α:100.00

0

5.275E+06 NUBASE

2746 75-Re-167M 0.5+ 1.300E+05 5.9 s 5.08

β+:99.00; α:1.00

0

2.435E+06 2.435E+06 5.405E+04 NUBASE

2747 75-Re-168 ? 4.4 s 2.27

β+:100.00; α:0.01

0

3.033E+06 3.033E+06 2.534E+02 NUBASE

2748 75-Re-169 4.5- 8.1 s 6.17

β+:100.00; α:0.01

0

2.177E+06 2.177E+06 2.522E+02 NUBASE

2749 75-Re-169M 0.5+ 1.600E+05 15.1 s 10.60

β+:99.80; α:0.20

0

2.226E+06 2.226E+06 1.041E+04 NUBASE

2750 75-Re-170 5.0+ 9.2 s 2.17

β+:99.99; α:0.01

0

2.791E+06 2.791E+06 4.755E+02 NUBASE

2751 75-Re-171 4.5- 15.2 s 2.63

β+:100.00

0

1.945E+06 1.945E+06 NUBASE

2752 75-Re-172 ? 15 s 20

β+:100.00

0

2.526E+06 2.526E+06 NUBASE

2753 75-Re-172M ? 55 s 9.09

β+:100.00

0

2.526E+06 2.526E+06 NUBASE

2754 75-Re-173 2.5- 2 m 15

β+:100.00

0

1.724E+06 1.724E+06 NUBASE

2755 75-Re-174 ? 2.4 m 1.67

β+:100.00

0

2.185E+06 2.185E+06 NUBASE

2756 75-Re-175 2.5- 5.89 m 0.85

β+:100.00

0

1.448E+06 1.448E+06 NUBASE

2757 75-Re-176 3.0+ 5.3 m 5.66

β+:100.00

4

1.088E+06 1.051E+06 ENSDF

2758 75-Re-177 2.5- 14 m 7.14

β+:100.00

0

1.144E+06 1.144E+06 NUBASE

2759 75-Re-178 3.0+ 13.2 m 1.52

β+:100.00

0

1.588E+06 1.588E+06 NUBASE

118 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 119: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2760 75-Re-179 2.5+ 19.5 m 0.51

β+:76.00; β+

m:24.00

0

8.882E+05 8.882E+05 NUBASE

2761 75-Re-180 1.0- 2.44 m 2.46

β+:100.00

4

1.335E+05 1.147E+06 ENSDF

2762 75-Re-181 2.5+ 19.9 h 3.52

β+:100.00

4

1.271E+05 7.872E+05 ENSDF

2763 75-Re-182 7.0+ 2.667 d 0.78

β+:100.00

4

1.896E+05 1.795E+06 ENSDF

2764 75-Re-182M 2.0+ 6.000E+04 12.7 h 1.57

β+:100.00

4

8.211E+04 1.206E+06 ENSDF

2765 75-Re-183 2.5+ 70 d 2

β+:100.00

4

1.074E+05 1.592E+05 UKPADD67

2766 75-Re-183M 12.5+ 1.908E+06 1.03E-03 s 3.88

IT:100.00

3

3.170E+05 1.589E+06 UKPADD67

2767 75-Re-184 3.0- 37.9 d 1.32

β+:100.00

4

5.472E+04 9.056E+05 UKPADD67

2768 75-Re-184M 8.0+ 1.880E+05 168 d 4.76

β+:25.20; IT:74.80

4

1.405E+05 3.902E+05 UKPADD67

2769 75-Re-185 2.5+

NUBASE

2770 75-Re-186 1.0- 3.75 d 0.80

β-:93.13; β+:6.87

5

3.373E+05 2.089E+04 UKPADD67

2771 75-Re-186M 8.0+ 1.490E+05 1.9E+05 y 10.53

IT:100.00

3

1.298E+05 1.980E+04 UKPADD67

2772 75-Re-187 2.5+ 4.35E+10 y 2.99

β-:100.00

1

6.600E+02 ENSDF

2773 75-Re-188 1.0- 16.98 h 0.12

β-:100.00

4

7.802E+05 5.788E+04 LNHB

2774 75-Re-188M 6.0- 1.721E+05 18.59 m 0.22

IT:100.00

0

1.721E+05 NUBASE

2775 75-Re-189 2.5+ 1.012 d 1.65

β-:89.72; β-

m:10.28

4

3.310E+05 5.555E+04 ENSDF

2776 75-Re-190 2.0- 3.1 m 9.68

β-:100.00

4

6.979E+05 1.340E+06 ENSDF

2777 75-Re-190M 6.0- 2.100E+05 3.2 h 6.25

β-m:54.40; IT:45.60

0

2.976E+05 3.933E+05 NUBASE

2778 75-Re-191 1.5+ 9.7 m 4.12

β-:100.00

1

7.270E+05 2.229E+03 UKPADD67

2779 75-Re-192 1.0- 6.2 s 12.90

β-:100.00

4

1.638E+06 1.591E+05 UKPADD67

2780 75-Re-193 2.5+ 30 s 100

β-:100.00

0

1.031E+06 1.031E+06 NUBASE

2781 75-Re-194 ? 2 s 100

β-:100.00

0

1.628E+06 1.628E+06 NUBASE

2782 76-Os-162 0.0+ 1.9E-03 s 36.84

α:100.00

1

6.779E+06 ENSDF

2783 76-Os-163 3.5- 5.5E-03 s 10.91

α:100.00

0

6.685E+06 NUBASE

2784 76-Os-164 0.0+ 0.021 s 4.76

α:98.00; β+

m:2.00

0

4.640E+04 4.640E+04 6.346E+06 NUBASE

2785 76-Os-165 3.5- 0.071 s 4.23

α:60.00; β+:20.00;

β+m:20.00

0

1.198E+06 1.198E+06 3.801E+06 NUBASE

2786 76-Os-166 0.0+ 0.216 s 4.17

α:72.00; β+:28.00

0

5.985E+05 5.985E+05 4.420E+06 NUBASE

2787 76-Os-167 1.5- 0.81 s 7.41

α:57.00; β+

m:43.00

0

1.177E+06 1.177E+06 3.412E+06 NUBASE

2788 76-Os-168 0.0+ 2.06 s 3.40

β+:51.00; α:49.00

0

9.858E+05 9.858E+05 2.851E+06 NUBASE

2789 76-Os-169 1.5- 3.46 s 3.18

β+:44.50; β+

m:44.50;

α:11.00

0

2.250E+06 2.250E+06 6.288E+05 NUBASE

2790 76-Os-170 0.0+ 7.46 s 3.08

β+:91.40; α:8.60

0

1.520E+06 1.520E+06 4.764E+05 NUBASE

2791 76-Os-171 2.5- 8.3 s 2.41

α:1.80; β+:98.20

5

2.003E+06 1.038E+06 9.675E+04 ENSDF

2792 76-Os-172 0.0+ 19.2 s 4.69

β+m:98.90; α:1.10

0

1.412E+06 1.412E+06 5.750E+04 NUBASE

2793 76-Os-173 2.5- 22.4 s 4.02

β+:99.60; α:0.40

0

2.031E+06 2.031E+06 2.022E+04 NUBASE

2794 76-Os-174 0.0+ 44 s 9.09

β+:99.98; α:0.02

0

1.225E+06 1.225E+06 1.169E+03 NUBASE

2795 76-Os-175 2.5- 1.4 m 7.14

β+:100.00

0

1.728E+06 1.728E+06 NUBASE

2796 76-Os-176 0.0+ 3.6 m 13.89

β+:100.00

0

9.883E+05 9.883E+05 NUBASE

2797 76-Os-177 0.5- 3 m 6.67

β+:100.00

0

1.440E+06 1.440E+06 NUBASE

2798 76-Os-178 0.0+ 5 m 8

β+:100.00

0

7.023E+05 7.023E+05 NUBASE

2799 76-Os-179 0.5- 6.5 m 4.62

β+:100.00

0

1.189E+06 1.189E+06 NUBASE

2800 76-Os-180 0.0+ 21.5 m 1.86

β+:100.00

4

2.382E+04 1.368E+05 UKPADD67

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 119

MAIN DATA TABLES

Page 120: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2801 76-Os-181 0.5- 1.75 h 2.86

β+:100.00

0

9.870E+05 9.870E+05 NUBASE

2802 76-Os-181M 3.5- 4.890E+04 2.7 m 3.70

β+:100.00

0

1.003E+06 1.003E+06 NUBASE

2803 76-Os-182 0.0+ 22.1 h 1.13

β+:100.00

4

4.807E+04 4.311E+05 ENSDF

2804 76-Os-183 4.5+ 13 h 3.85

β+:100.00

0

7.170E+05 7.170E+05 NUBASE

2805 76-Os-183M 0.5- 1.707E+05 9.9 h 3.03

β+:85.00; IT:15.00

0

6.578E+05 6.834E+05 NUBASE

2806 76-Os-184 0.0+ 5.6E+13 y 100

α:50.00; 2β+:50.00

0

7.256E+05 1.482E+06 NUBASE

2807 76-Os-185 0.5- 93.8 d 0.96

β+:100.00

4

1.833E+04 7.190E+05 UKPADD67

2808 76-Os-186 0.0+ 2E+15 y 55

α:100.00

0

2.823E+06 NUBASE

2809 76-Os-187 0.5-

NUBASE

2810 76-Os-188 0.0+

NUBASE

2811 76-Os-189 1.5-

NUBASE

2812 76-Os-189M 4.5- 3.081E+04 5.81 h 1.03

IT:100.00

0

3.081E+04 NUBASE

2813 76-Os-190 0.0+

NUBASE

2814 76-Os-190M 10.0- 1.705E+06 9.9 m 4.04

IT:100.00

3

1.169E+05 1.589E+06 UKPADD67

2815 76-Os-191 4.5- 15.3 d 1.96

β-m:100.00

1

3.752E+04 UKPADD67

2816 76-Os-191M 1.5- 7.438E+04 13.1 h 0.38

IT:100.00

3

6.658E+04 7.807E+03 UKPADD67

2817 76-Os-192 0.0+

NUBASE

2818 76-Os-192M 10.0- 2.015E+06 5.9 s 1.69

IT:87.00; β-

n:13.00

0

3.466E+04 1.788E+06 NUBASE

2819 76-Os-193 1.5- 1.255 d 0.03

β-:99.65; β-

m:0.35

4

3.796E+05 6.706E+04 ENSDF

2820 76-Os-194 0.0+ 6 y 3.33

β-:100.00

4

4.429E+04 4.091E+03 UKPADD67

2821 76-Os-195 0.5- 6.5 m 9.23

β-:100.00

4

7.153E+05 1.422E+05 UKPADD67

2822 76-Os-196 0.0+ 34.9 m 0.57

β-:100.00

4

3.726E+05 7.703E+04 UKPADD67

2823 77-Ir-164 2.0- 1E-03 s 100

p:33.33; α:33.33;

β+:33.33

0

1.466E+06 1.466E+06 2.842E+06 NUBASE

2824 77-Ir-164M 9.0+ 2.700E+05 9.4E-05 s 28.72

p:33.33; α:33.33;

β+:33.33

0

1.496E+06 1.496E+06 3.022E+06 NUBASE

2825 77-Ir-165 0.5+ 1E-06 s 100

p:50.00; α:50.00

0

4.183E+06 NUBASE

2826 77-Ir-166 2.0- 0.011 s 20.95

α:93.10; p:6.90

1

6.261E+06 ENSDF

2827 77-Ir-166M 9.0+ 1.720E+05 0.015 s 5.96

α m:98.20; p:1.80

0

6.617E+06 NUBASE

2828 77-Ir-167 0.5+ 0.035 s 5.68

α:48.00; p:32.00;

β+:20.00

0

6.281E+05 6.281E+05 3.464E+06 NUBASE

2829 77-Ir-167M 5.5- 1.753E+05 0.03 s 2

α m:80.00; β+:19.60;

p:0.40

0

6.270E+05 6.270E+05 5.256E+06 NUBASE

2830 77-Ir-168 ? 0.161 s 13.04

α:100.00

0

6.475E+06 NUBASE

2831 77-Ir-168M ? 1.500E+05 0.125 s 32

α m:50.00; β+:50.00

0

1.900E+06 1.900E+06 3.203E+06 NUBASE

2832 77-Ir-169 0.5+ 0.4 s 25

α:100.00

1

6.275E+06 ENSDF

2833 77-Ir-169M 5.5- 1.540E+05 0.308 s 7.14

α m:72.00; β+:28.00

0

8.208E+05 8.208E+05 4.506E+06 NUBASE

2834 77-Ir-170 ? 0.91 s 16.48

β+:94.80; α:2.60;

α m:2.60

0

3.352E+06 3.352E+06 3.110E+05 NUBASE

2835 77-Ir-170M ? 3.707E+05 0.44 s 13.64

α:18.00; α m:18.00;

β+:32.00; IT:32.00

0

1.171E+06 1.290E+06 2.286E+06 NUBASE

2836 77-Ir-171 0.5+ 3.6 s 27.78

α m:100.00

0

5.855E+06 NUBASE

120 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 121: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2837 77-Ir-171M 5.5- 1.800E+05 1.4 s 7.14

α:58.00; β+:21.00;

p:21.00

0

5.630E+05 5.630E+05 3.657E+06 NUBASE

2838 77-Ir-172 3.0+ 4.4 s 6.82

β+:98.00; α:2.00

0

3.175E+06 3.175E+06 1.169E+05 NUBASE

2839 77-Ir-172M 7.0+ 1.390E+05 2 s 5

β+:77.00; α:23.00

0

2.530E+06 2.530E+06 1.376E+06 NUBASE

2840 77-Ir-173 ? 9 s 8.89

β+:93.00; α:3.50;

α m:3.50

0

2.221E+06 2.221E+06 3.926E+05 NUBASE

2841 77-Ir-173M 5.5- 2.500E+05 2.2 s 2.27

β+:88.00; α:12.00

0

2.175E+06 2.175E+06 7.127E+05 NUBASE

2842 77-Ir-174 3.0+ 7.9 s 7.59

β+:99.50; α:0.50

0

3.027E+06 3.027E+06 2.812E+04 NUBASE

2843 77-Ir-174M 7.0+ 1.930E+05 4.9 s 6.12

β+:97.50; α:2.50

0

3.029E+06 3.029E+06 1.454E+05 NUBASE

2844 77-Ir-175 2.5- 9 s 22.22

β+:99.15; α:0.85

0

2.206E+06 2.206E+06 4.587E+04 NUBASE

2845 77-Ir-176 ? 8.3 s 7.23

β+:96.90; α:1.55;

α m:1.55

0

2.661E+06 2.661E+06 1.623E+05 NUBASE

2846 77-Ir-177 2.5- 30 s 6.67

β+:99.94; α:0.06

0

1.966E+06 1.966E+06 3.049E+03 NUBASE

2847 77-Ir-178 ? 12 s 16.67

β+:100.00

0

2.431E+06 2.431E+06 NUBASE

2848 77-Ir-179 2.5- 1.317 m 1.27

β+:100.00

0

1.648E+06 1.648E+06 NUBASE

2849 77-Ir-180 ? 1.5 m 6.67

β+:100.00

0

2.127E+06 2.127E+06 NUBASE

2850 77-Ir-181 2.5- 4.9 m 3.06

β+:50.00; β+

m:50.00

0

1.351E+06 1.351E+06 NUBASE

2851 77-Ir-182 3.0+ 15 m 6.67

β+:100.00

0

1.852E+06 1.852E+06 NUBASE

2852 77-Ir-183 2.5- 58 m 8.62

β+:32.98; β+

m:66.97;

α:0.05

0

1.116E+06 1.116E+06 1.982E+03 NUBASE

2853 77-Ir-184 5.0- 3.09 h 0.97

β+:100.00

0

1.548E+06 1.548E+06 NUBASE

2854 77-Ir-185 2.5- 14.4 h 0.69

β+:100.00

0

8.245E+05 8.245E+05 NUBASE

2855 77-Ir-186 5.0+ 16.64 h 0.18

β+:100.00

0

1.276E+06 1.276E+06 NUBASE

2856 77-Ir-186M 2.0- 8.000E+02 1.92 h 2.60

β+:75.00; IT:25.00

0

9.568E+05 9.570E+05 NUBASE

2857 77-Ir-187 1.5+ 10.5 h 2.86

β+:100.00

4

6.379E+04 3.015E+05 UKPADD67

2858 77-Ir-187M 4.5- 1.862E+05 0.03 s 1.98

IT:100.00

0

1.862E+05 NUBASE

2859 77-Ir-188 1.0- 1.729 d 1.20

β+:100.00

0

9.361E+05 9.361E+05 NUBASE

2860 77-Ir-188M 7.0+ 9.700E+05 4.2E-03 s 4.76

IT:100.00

0

9.700E+05 NUBASE

2861 77-Ir-189 1.5+ 13.2 d 0.76

β+:92.51; β+

m:7.49

4

4.026E+04 7.892E+04 ENSDF

2862 77-Ir-189M 5.5- 3.722E+05 0.013 s 2.26

IT:100.00

0

3.722E+05 NUBASE

2863 77-Ir-189N 12.5+ 2.333E+06 3.7E-03 s 5.41

ITm:100.00

0

1.961E+06 NUBASE

2864 77-Ir-190 4.0- 12 d 1.67

β+:100.00

4

7.211E+04 1.478E+06 UKPADD67

2865 77-Ir-190M 1.0- 2.610E+04 1.12 h 0.27

IT:100.00

3

2.384E+04 2.283E+03 UKPADD67

2866 77-Ir-190N 11.0- 3.764E+05 3.087 h 0.39

IT:8.60; β+

m:91.40

4

2.888E+04 5.887E+04 UKPADD67

2867 77-Ir-191 1.5+

NUBASE

2868 77-Ir-191M 5.5- 1.712E+05 4.9 s 0.61

IT:100.00

3

9.572E+04 7.539E+04 UKPADD67

2869 77-Ir-191N 13.5- 2.085E+06 5.5 s 12.73

ITm:100.00

3

4.576E+04 1.868E+06 UKPADD67

2870 77-Ir-192 4.0+ 73.822 d 0.01

β-:95.20; β+:4.80

5

2.173E+05 8.165E+05 UKPADD67

2871 77-Ir-192M 1.0- 5.672E+04 1.44 m 4.86

β-:0.02; IT:99.98

4

5.443E+04 2.439E+03 UKPADD67

2872 77-Ir-192N 11.0- 1.681E+05 241 y 3.73

IT:100.00

3

1.650E+05 3.086E+03 UKPADD67

2873 77-Ir-193 1.5+

NUBASE

2874 77-Ir-193M 5.5- 8.024E+04 10.54 d 0.38

IT:100.00

3

7.770E+04 2.591E+03 UKPADD67

2875 77-Ir-194 1.0- 19.3 h 0.52

β-:100.00

4

8.103E+05 9.099E+04 LNHB

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 121

MAIN DATA TABLES

Page 122: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2876 77-Ir-194M 4.0+ 1.471E+05 0.032 s 0.75

IT:100.00

3

8.321E+04 5.330E+04 ENSDF

2877 77-Ir-194N ? 3.700E+05 171 d 6.43

β-:100.00

4

8.306E+04 2.334E+06 ENSDF

2878 77-Ir-195 1.5+ 2.5 h 8

β-:100.00

4

3.784E+05 5.839E+04 ENSDF

2879 77-Ir-195M 5.5- 1.230E+05 3.8 h 5.26

β-:64.60; β-

m:30.40;

IT:5.00

0

3.632E+05 3.694E+05 NUBASE

2880 77-Ir-196 0.0- 52 s 3.85

β-:100.00

2

1.168E+06 2.272E+05 ENSDF

2881 77-Ir-196M ? 2.100E+05 1.4 h 1.43

β-:99.70; IT:0.30

0

1.136E+06 1.136E+06 NUBASE

2882 77-Ir-197 1.5+ 5.8 m 8.62

β-:100.00

4

7.334E+05 2.238E+05 UKPADD67

2883 77-Ir-197M 5.5- 1.150E+05 8.9 m 3.37

β-m:99.75; IT:0.25

4

6.800E+05 2.042E+03 UKPADD67

2884 77-Ir-198 ? 8 s 12.50

β-:100.00

0

1.363E+06 1.363E+06 NUBASE

2885 77-Ir-199 1.5+ 20 s 100

β-:100.00

0

9.973E+05 9.973E+05 NUBASE

2886 78-Pt-166 0.0+ 3E-04 s 33.33

α:100.00

0

7.285E+06 NUBASE

2887 78-Pt-167 3.5- 7E-04 s 28.57

α:100.00

0

7.155E+06 NUBASE

2888 78-Pt-168 0.0+ 2E-03 s 20

α:99.30

1

6.950E+06 ENSDF

2889 78-Pt-169 1.5- 3.7E-03 s 40.54

α:99.00; β+:1.00

0

3.234E+04 3.234E+04 6.777E+06 NUBASE

2890 78-Pt-170 0.0+ 0.014 s 3.62

α:98.00; β+:1.00;

β+m:1.00

0

4.552E+04 4.552E+04 6.573E+06 NUBASE

2891 78-Pt-171 1.5- 0.044 s 15.91

α:98.00; β+:2.00

0

5.973E+04 5.973E+04 6.473E+06 NUBASE

2892 78-Pt-172 0.0+ 0.098 s 2.44

α:77.00; β+:23.00

0

4.921E+05 4.921E+05 4.978E+06 NUBASE

2893 78-Pt-173 2.5- 0.365 s 1.92

α:84.00; β+:16.00

0

4.444E+05 4.444E+05 5.339E+06 NUBASE

2894 78-Pt-174 0.0+ 0.889 s 1.91

α:76.00; β+:24.00

0

4.440E+05 4.440E+05 4.700E+06 NUBASE

2895 78-Pt-175 2.5- 2.53 s 2.37

α:64.00; β+:36.00

0

9.287E+05 9.287E+05 3.954E+06 NUBASE

2896 78-Pt-176 0.0+ 6.33 s 2.37

β+:62.00; α:38.00

0

1.019E+06 1.019E+06 2.236E+06 NUBASE

2897 78-Pt-177 2.5- 10.6 s 3.77

β+:94.30; α:5.70

0

2.099E+06 2.099E+06 3.217E+05 NUBASE

2898 78-Pt-178 0.0+ 21.1 s 2.84

β+:92.30; α:7.70

0

1.309E+06 1.309E+06 4.291E+05 NUBASE

2899 78-Pt-179 0.5- 21.2 s 1.89

β+:99.76; α:0.24

0

1.933E+06 1.933E+06 1.300E+04 NUBASE

2900 78-Pt-180 0.0+ 56 s 3.57

β+:99.70; α:0.30

0

1.177E+06 1.177E+06 1.571E+04 NUBASE

2901 78-Pt-181 0.5- 52 s 4.23

β+:99.93; α:0.07

0

1.698E+06 1.698E+06 3.811E+03 NUBASE

2902 78-Pt-182 0.0+ 2.2 m 4.55

β+:99.96; α:0.04

0

9.606E+05 9.606E+05 1.882E+03 NUBASE

2903 78-Pt-183 0.5- 6.5 m 15.38

β+:99.99; α:0.01

0

1.475E+06 1.475E+06 4.630E+02 NUBASE

2904 78-Pt-183M 3.5- 3.450E+04 43 s 11.63

β+:100.00; α:~

0

1.486E+06 1.486E+06 1.943E+01 NUBASE

2905 78-Pt-184 0.0+ 17.3 m 1.16

β+:100.00; α:~

0

7.597E+05 7.597E+05 7.824E+01 NUBASE

2906 78-Pt-184M 8.0- 1.839E+06 1.01E-03 s 4.95

IT:100.00

0

1.839E+06 NUBASE

2907 78-Pt-185 4.5+ 1.182 h 3.39

β+:100.00; α m:0.01

0

1.219E+06 1.219E+06 2.198E+02 NUBASE

2908 78-Pt-185M 0.5- 1.034E+05 33 m 2.42

β+:98.00; IT:2.00

0

1.228E+06 1.230E+06 NUBASE

2909 78-Pt-186 0.0+ 2.08 h 2.40

β+m:100.00; α:~

0

4.361E+05 4.361E+05 6.048E+00 NUBASE

2910 78-Pt-187 1.5- 2.35 h 1.28

β+:100.00

4

1.032E+05 4.483E+05 ENSDF

2911 78-Pt-188 0.0+ 10.2 d 2.94

β+:100.00

4

7.456E+04 2.054E+05 ENSDF

2912 78-Pt-189 1.5- 10.87 h 1.10

β+:100.00

4

8.756E+04 4.728E+05 ENSDF

2913 78-Pt-190 0.0+ 6.5E+11 y 4.62

α:100.00

1

3.243E+06 ENSDF

2914 78-Pt-191 1.5- 2.802 d 0.89

β+:98.98; β+

m:1.02

4

6.594E+04 2.943E+05 ENSDF

2915 78-Pt-192 0.0+

NUBASE

2916 78-Pt-193 0.5- 50.001 y 18

β+:100.00

3

7.856E+03 3.378E+04 UKPADD67

122 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 123: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2917 78-Pt-193M 6.5+ 1.498E+05 4.34 d 0.69

IT:100.00

3

1.380E+05 1.233E+04 UKPADD67

2918 78-Pt-194 0.0+

NUBASE

2919 78-Pt-195 0.5-

NUBASE

2920 78-Pt-195M 6.5+ 2.593E+05 4.1 d 2.44

IT:100.00

3

1.823E+05 7.647E+04 UKPADD67

2921 78-Pt-196 0.0+

NUBASE

2922 78-Pt-197 0.5- 19.891 h 0.01

β-:100.00

4

2.544E+05 2.438E+04 UKPADD67

2923 78-Pt-197M 6.5+ 3.996E+05 1.588 h 0.21

β-m:3.30; IT:96.70

4

3.169E+05 7.608E+04 UKPADD67

2924 78-Pt-198 0.0+

NUBASE

2925 78-Pt-199 2.5- 30.8 m 1.30

β-:100.00

4

5.495E+05 1.994E+05 ENSDF

2926 78-Pt-199M 6.5+ 4.240E+05 13.6 s 2.94

IT:100.00

3

7.728E+04 3.406E+05 ENSDF

2927 78-Pt-200 0.0+ 12.5 h 2.40

β-:100.00

4

2.266E+05 5.960E+04 ENSDF

2928 78-Pt-201 2.5- 2.5 m 4

β-:100.00

0

8.870E+05 8.870E+05 NUBASE

2929 78-Pt-202 0.0+ 1.833 d 34.09

β-:100.00

1

6.589E+05 1.927E+03 UKPADD67

2930 79-Au-169 0.5+ 1.5E-04 s 100

α:50.00; β+:50.00

0

1.765E+06 1.765E+06 3.708E+06 NUBASE

2931 79-Au-170 2.0- 3.1E-04 s 16.13

p:85.00; α:15.00

0

2.335E+06 NUBASE

2932 79-Au-170M 9.0+ 2.740E+05 6.3E-04 s 9.52

p:75.00; α m:12.50;

β+:12.50

0

5.404E+05 5.404E+05 2.226E+06 NUBASE

2933 79-Au-171 0.5+ 1.7E-05 s 52.94

p:100.00

0

8.575E+03 ENSDF

2934 79-Au-171M 5.5- 2.500E+05 1.014E-03 s 1.87

α m:54.00; p:46.00

0

4.651E+06 NUBASE

2935 79-Au-172 ? 4.7E-03 s 23.40

α:49.00; α m:49.00;

p:2.00

0

6.839E+06 NUBASE

2936 79-Au-173 0.5+ 0.059 s 76.27

α:100.00

1

6.879E+06 ENSDF

2937 79-Au-173M 5.5- 2.140E+05 0.014 s 6.34

α m:95.70; β+:4.30

0

1.338E+05 1.338E+05 6.599E+06 NUBASE

2938 79-Au-174 ? 0.139 s 2.16

α:45.00; α m:45.00;

β+:10.00

0

3.706E+05 3.706E+05 5.859E+06 NUBASE

2939 79-Au-174M ? 4.600E+05 0.171 s 16.96

α:25.00; α m:25.00;

β+:50.00

0

1.930E+06 1.930E+06 3.485E+06 NUBASE

2940 79-Au-175 0.5+ 0.1 s 100

α:50.00; β+:50.00

0

1.375E+06 1.375E+06 3.283E+06 NUBASE

2941 79-Au-175M 5.5- 2.000E+05 0.156 s 3.21

α m:82.00; β+:18.00

0

5.070E+05 5.070E+05 5.400E+06 NUBASE

2942 79-Au-176 5.0- 1.08 s 15.74

α:30.00; α m:30.00;

β+:40.00

0

1.385E+06 1.385E+06 3.891E+06 NUBASE

2943 79-Au-176M 7.0+ 1.500E+05 0.86 s 18.60

α m:60.00; β+:40.00

0

1.405E+06 1.405E+06 3.940E+06 NUBASE

2944 79-Au-177 ? 1.46 s 2.05

α:100.00

0

6.297E+06 NUBASE

2945 79-Au-177M 5.5- 2.100E+05 1.18 s 1.02

α m:100.00

0

6.257E+06 NUBASE

2946 79-Au-178 ? 2.6 s 19.23

β+:60.00; α:20.00;

α m:20.00

0

1.934E+06 1.934E+06 2.407E+06 NUBASE

2947 79-Au-179 2.5- 7.1 s 4.23

β+:78.00; α:22.00

0

1.901E+06 1.901E+06 1.331E+06 NUBASE

2948 79-Au-180 ? 8.1 s 3.70

β+:98.20; α:1.80

0

2.894E+06 2.894E+06 1.051E+05 NUBASE

2949 79-Au-181 1.5- 13.7 s 10.22

β+:97.30; α:2.70

0

2.109E+06 2.109E+06 1.553E+05 NUBASE

2950 79-Au-182 2.0+ 15.5 s 2.58

β+:99.87; α:0.13

0

2.619E+06 2.619E+06 7.184E+03 NUBASE

2951 79-Au-183 2.5- 42 s 2.86

α:0.55; β+:99.64

5

7.981E+05 1.330E+06 2.938E+04 ENSDF

2952 79-Au-184 5.0+ 20.6 s 4.37

β+:49.99; β+

m:49.99;

α:0.02

0

2.031E+06 2.031E+06 8.375E+02 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 123

MAIN DATA TABLES

Page 124: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2953 79-Au-184M 2.0+ 6.846E+04 47.6 s 2.94

β+:69.98; IT:30.00;

α:0.02

0

1.652E+06 1.672E+06 8.484E+02 NUBASE

2954 79-Au-185 2.5- 4.25 m 1.41

β+:25.33; β+

m:74.41;

α:0.26

0

1.575E+06 1.575E+06 1.347E+04 NUBASE

2955 79-Au-186 3.0- 10.7 m 4.67

β+:100.00

4

1.054E+06 1.430E+06 ENSDF

2956 79-Au-187 0.5+ 8.4 m 3.57

β+:100.00; α:~

0

1.236E+06 1.236E+06 1.430E+02 NUBASE

2957 79-Au-187M 4.5- 1.205E+05 2.3 s 4.35

IT:100.00

0

1.205E+05 NUBASE

2958 79-Au-188 1.0- 8.84 m 0.68

β+:100.00

0

1.841E+06 1.841E+06 NUBASE

2959 79-Au-189 0.5+ 28.7 m 1.05

β+:100.00; α:~

0

9.670E+05 9.670E+05 1.299E+00 NUBASE

2960 79-Au-189M 5.5- 2.472E+05 4.59 m 2.40

β+:100.00

0

1.049E+06 1.049E+06 NUBASE

2961 79-Au-190 1.0- 42.8 m 2.34

β+:100.00

4

1.299E+05 2.123E+06 ENSDF

2962 79-Au-190M 11.0- 2.000E+05 0.125 s 16

IT:100.00

0

2.000E+05 NUBASE

2963 79-Au-191 1.5+ 3.18 h 2.52

β+:100.00

4

7.186E+04 5.582E+05 ENSDF

2964 79-Au-191M 5.5- 2.662E+05 0.92 s 11.96

IT:100.00

0

2.662E+05 NUBASE

2965 79-Au-192 1.0- 4.94 h 1.82

β+:100.00

4

8.286E+04 1.702E+06 ENSDF

2966 79-Au-192M 5.0+ 1.354E+05 0.029 s 10.34

IT:100.00

3

1.261E+05 8.855E+03 UKPADD67

2967 79-Au-192N 11.0- 4.316E+05 0.16 s 12.50

ITm:100.00

3

1.615E+05 1.347E+05 UKPADD67

2968 79-Au-193 1.5+ 17.65 h 0.85

β+:100.00

4

4.902E+04 1.588E+05 ENSDF

2969 79-Au-193M 5.5- 2.902E+05 3.9 s 7.69

IT:99.97; β+:0.02;

β+m:0.02

0

1.298E+02 2.902E+05 NUBASE

2970 79-Au-194 1.0- 1.584 d 0.26

β+:100.00

4

3.677E+04 1.031E+06 ENSDF

2971 79-Au-194M 5.0+ 1.074E+05 0.6 s 1.33

IT:100.00

0

1.074E+05 NUBASE

2972 79-Au-194N 11.0- 4.758E+05 0.42 s 2.38

ITm:100.00

0

3.684E+05 NUBASE

2973 79-Au-195 1.5+ 186.094 d 0.02

β+:100.00

4

4.879E+04 8.633E+04 UKPADD67

2974 79-Au-195M 5.5- 3.186E+05 30.5 s 0.66

IT:100.00

3

1.155E+05 2.030E+05 UKPADD67

2975 79-Au-196 2.0- 6.183 d 0.16

β+:92.80; β-:7.20

5

2.786E+04 4.721E+05 ENSDF

2976 79-Au-196M 5.0+ 8.466E+04 8.1 s 2.47

IT:100.00

0

8.466E+04 NUBASE

2977 79-Au-196N 12.0- 5.957E+05 9.6 h 1.04

ITm:100.00

0

5.110E+05 NUBASE

2978 79-Au-197 1.5+

NUBASE

2979 79-Au-197M 5.5- 4.092E+05 7.74 s 0.90

IT:100.00

3

1.838E+05 2.254E+05 UKPADD67

2980 79-Au-198 2.0- 2.694 d 0.03

β-:100.00

4

3.262E+05 4.028E+05 LNHB

2981 79-Au-198M 12.0- 8.120E+05 2.3 d 1.74

IT:100.00

3

2.621E+05 5.278E+05 UKPADD67

2982 79-Au-199 1.5+ 3.139 d 0.22

β-:100.00

4

1.451E+05 9.607E+04 UKPADD67

2983 79-Au-200 1.0- 48.4 m 0.62

β-:100.00

4

7.427E+05 2.733E+05 ENSDF

2984 79-Au-200M 12.0- 9.600E+05 18.7 h 2.67

β-:82.00; IT:18.00

0

8.731E+05 1.046E+06 NUBASE

2985 79-Au-201 1.5+ 26 m 3.85

β-:100.00

4

4.241E+05 3.419E+04 ENSDF

2986 79-Au-202 1.0- 28.8 s 6.60

β-:100.00

2

1.180E+06 1.697E+05 ENSDF

2987 79-Au-203 1.5+ 53 s 3.77

β-:100.00

2

7.669E+05 6.900E+04 ENSDF

2988 79-Au-204 2.0- 39.8 s 2.26

β-:100.00

0

1.313E+06 1.313E+06 NUBASE

2989 79-Au-205 1.5+ 31 s 6.45

β-:100.00

0

1.179E+06 1.179E+06 NUBASE

2990 80-Hg-171 1.5- 8E-05 s 37.50

α:99.99; β+:0.01

0

3.688E+02 3.688E+02 7.614E+06 NUBASE

2991 80-Hg-172 0.0+ 4.2E-04 s 57.14

α:100.00

0

7.525E+06 NUBASE

2992 80-Hg-173 1.5- 1.1E-03 s 36.36

α:100.00

0

7.385E+06 NUBASE

124 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 125: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

2993 80-Hg-174 0.0+ 1.9E-03 s 21.05

α:99.70

1

7.212E+06 ENSDF

2994 80-Hg-175 2.5- 0.011 s 3.70

α:99.00

1

6.980E+06 ENSDF

2995 80-Hg-176 0.0+ 0.02 s 7.35

α:90.00; β+:10.00

0

2.254E+05 2.254E+05 6.207E+06 NUBASE

2996 80-Hg-177 6.5+ 0.127 s 1.41

α:85.00; β+:15.00

0

4.385E+05 4.385E+05 5.725E+06 NUBASE

2997 80-Hg-178 0.0+ 0.269 s 1.12

α:70.00; β+:30.00

0

6.013E+05 6.013E+05 4.604E+06 NUBASE

2998 80-Hg-179 2.5- 1.09 s 3.67

α:53.00; β+:46.85;

β+,p:0.15

0

1.257E+06 1.257E+06 3.365E+06 NUBASE

2999 80-Hg-180 0.0+ 2.58 s 0.39

β+:52.00; α:48.00

0

9.275E+05 9.275E+05 3.004E+06 NUBASE

3000 80-Hg-181 0.5- 3.6 s 2.78

β+:68.98; α:31.00;

β+,p:0.02; β+,n:~

0

1.658E+06 1.658E+06 1.948E+06 NUBASE

3001 80-Hg-182 0.0+ 10.83 s 0.55

β+:86.20; α:13.80;

β+,p:~

0

1.358E+06 1.358E+06 8.276E+05 NUBASE

3002 80-Hg-183 0.5- 9.4 s 7.45

β+:88.30; α:11.70;

β+,p:~

0

1.880E+06 1.880E+06 7.066E+05 NUBASE

3003 80-Hg-183M 6.5+ 2.400E+05 5 s 100

β+:100.00

0

2.209E+06 2.209E+06 NUBASE

3004 80-Hg-184 0.0+ 30.6 s 0.98

β+m:98.89; α:1.11

0

1.286E+06 1.286E+06 6.285E+04 NUBASE

3005 80-Hg-185 0.5- 49.1 s 2.04

β+:94.00; α:6.00

0

1.783E+06 1.783E+06 3.464E+05 NUBASE

3006 80-Hg-185M 6.5+ 1.038E+05 21.6 s 6.94

IT:53.98; β+:45.99;

α:0.03

0

8.883E+05 9.443E+05 1.763E+03 NUBASE

3007 80-Hg-186 0.0+ 1.38 m 4.35

α:0.02; β+:100.00

5

1.588E+05 4.236E+05 9.169E+02 ENSDF

3008 80-Hg-187 1.5- 1.9 m 15.79

β+:100.00; α:~

0

1.629E+06 1.629E+06 6.275E+00 NUBASE

3009 80-Hg-187M 6.5+ 3.000E+04 2.4 m 12.50

β+m:100.00; α m:~

0

1.599E+06 1.599E+06 1.306E+01 NUBASE

3010 80-Hg-188 0.0+ 3.25 m 4.62

β+:100.00

4

4.448E+04 1.717E+05 ENSDF

3011 80-Hg-189 1.5- 7.6 m 1.32

β+:100.00; α m:~

0

1.317E+06 1.317E+06 1.357E+00 NUBASE

3012 80-Hg-189M 6.5+ 1.000E+05 8.6 m 1.16

β+m:100.00; α:~

0

1.268E+06 1.268E+06 1.418E+00 NUBASE

3013 80-Hg-190 0.0+ 20 m 2

β+:100.00

4

6.807E+04 2.044E+05 UKPADD67

3014 80-Hg-191 1.5- 49 m 20.41

β+:100.00; α:~

0

1.072E+06 1.072E+06 1.848E-01 NUBASE

3015 80-Hg-191M 6.5+ 1.280E+05 50.8 m 2.95

β+:56.00; β+

m:44.00;

α:~

0

1.076E+06 1.076E+06 1.912E-01 NUBASE

3016 80-Hg-192 0.0+ 4.85 h 4.12

β+:100.00

4

5.289E+04 2.723E+05 ENSDF

3017 80-Hg-193 1.5- 3.8 h 3.95

β+:96.64; β+

m:3.36

0

7.778E+05 7.778E+05 NUBASE

3018 80-Hg-193M 6.5+ 1.408E+05 11.8 h 1.69

β+:40.83; β+

m:51.97;

IT:7.20

0

7.180E+05 7.282E+05 NUBASE

3019 80-Hg-194 0.0+ 444.001 y 18.02

β+:100.00

3

7.340E+03 1.468E+04 UKPADD67

3020 80-Hg-195 0.5- 9.9 h 5.05

β+:97.90; β+

m:2.10

4

5.556E+04 1.995E+05 ENSDF

3021 80-Hg-195M 6.5+ 1.761E+05 1.733 d 1.92

IT:54.20; β+:22.90;

β+m:22.90

0

2.422E+05 3.377E+05 NUBASE

3022 80-Hg-196 0.0+ 2.5E+18 y 100

2β+:100.00

0

8.207E+05 NUBASE

3023 80-Hg-197 0.5- 2.692 d 0.93

β+:100.00

4

6.915E+04 7.351E+04 UKPADD67

3024 80-Hg-197M 6.5+ 2.989E+05 23.9 h 2.09

β+m:8.60; IT:91.40

4

2.006E+05 7.798E+04 UKPADD67

3025 80-Hg-198 0.0+

NUBASE

3026 80-Hg-199 0.5-

NUBASE

3027 80-Hg-199M 6.5+ 5.325E+05 42.1 m 2.14

IT:100.00

3

3.477E+05 1.846E+05 UKPADD67

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 125

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Page 126: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3028 80-Hg-200 0.0+

NUBASE

3029 80-Hg-201 1.5-

NUBASE

3030 80-Hg-202 0.0+

NUBASE

3031 80-Hg-203 2.5- 46.603 d 0.05

β-:100.00

4

9.833E+04 2.377E+05 LNHB

3032 80-Hg-204 0.0+

NUBASE

3033 80-Hg-205 0.5- 5.2 m 1.92

β-:100.00

4

5.362E+05 6.886E+03 UKPADD67

3034 80-Hg-205M 6.5+ 1.556E+06 1.09E-03 s 3.67

IT:100.00

0

1.556E+06 NUBASE

3035 80-Hg-206 0.0+ 8.15 m 1.23

β-:100.00

4

4.307E+05 1.020E+05 LNHB

3036 80-Hg-207 4.5+ 2.9 m 6.90

β-:54.20; β-

m:45.80

0

1.399E+06 1.399E+06 NUBASE

3037 80-Hg-208 0.0+ 42 m 11.90

β-:100.00

0

1.216E+06 1.216E+06 NUBASE

3038 80-Hg-209 4.5+ 37 s 21.62

β-:100.00

0

1.763E+06 1.763E+06 NUBASE

3039 80-Hg-210 0.0+ 10 m 100

β-:100.00

0

1.379E+06 1.379E+06 NUBASE

3040 81-Tl-176 ? 0.01 s 100

α:100.00

0

7.405E+06 NUBASE

3041 81-Tl-177 0.5+ 0.018 s 27.78

α:73.00; p:27.00

0

5.473E+06 NUBASE

3042 81-Tl-178 ? 0.255 s 3.92

α:26.50; α m:26.50;

β+:47.00

0

1.812E+06 1.812E+06 3.601E+06 NUBASE

3043 81-Tl-179 0.5+ 0.27 s 11.11

α m:70.00; β+:30.00

0

8.622E+05 8.622E+05 4.561E+06 NUBASE

3044 81-Tl-179M 4.5- 8.600E+05 1.6E-03 s 10

α:100.00

0

7.575E+06 NUBASE

3045 81-Tl-180 ? 1.5 s 13.33

β+:93.00; α:3.50;

α m:3.50; β+,SF:~

0

3.362E+06 3.362E+06 4.648E+05 NUBASE

3046 81-Tl-181 0.5+ 3.2 s 9.37

α:50.00; β+:50.00

0

1.310E+06 1.310E+06 3.162E+06 NUBASE

3047 81-Tl-181M 4.5- 8.500E+05 1.7E-03 s 23.53

β+:33.33; α m:33.33;

IT:33.33

0

9.678E+05 1.251E+06 2.321E+06 NUBASE

3048 81-Tl-182 2.0- 2 s 15

β+:96.00; α:4.00

0

3.272E+06 3.272E+06 2.622E+05 NUBASE

3049 81-Tl-182M 7.0+ 1.000E+05 2.9 s 17.24

α:100.00

0

6.655E+06 NUBASE

3050 81-Tl-183 0.5+ 6.9 s 10.14

β+:98.00; α:2.00

0

2.356E+06 2.356E+06 1.188E+05 NUBASE

3051 81-Tl-183M 4.5- 6.420E+05 0.06 s 25

α:1.50; β+

m:49.25;

IT:49.25

0

1.250E+06 1.566E+06 9.873E+04 NUBASE

3052 81-Tl-184 2.0- 9.7 s 6.19

β+:97.90; α:2.10

0

3.087E+06 3.087E+06 1.319E+05 NUBASE

3053 81-Tl-184M 7.0+ 1.000E+05 10 s 100

β+:50.00; IT:50.00

0

1.593E+06 1.643E+06 NUBASE

3054 81-Tl-185 0.5+ 19.5 s 2.56

β+:50.00; α:50.00

0

1.069E+06 1.069E+06 2.843E+06 NUBASE

3055 81-Tl-185M 4.5- 4.528E+05 1.83 s 6.56

IT:99.90; α:0.10

0

4.523E+05 6.133E+03 NUBASE

3056 81-Tl-186 2.0- 40 s 100

β+:100.00

0

2.783E+06 2.783E+06 NUBASE

3057 81-Tl-186M 10.0- 3.740E+05 2.9 s 6.90

IT:100.00

3

6.802E+04 3.050E+05 ENSDF

3058 81-Tl-186N 10.0- 5.200E+05 2.9 s 6.90

ITm:100.00

0

3.700E+05 NUBASE

3059 81-Tl-187 0.5+ 51 s 100

β+:100.00

0

1.891E+06 1.891E+06 NUBASE

3060 81-Tl-187M 4.5- 3.330E+05 15.6 s 0.77

IT:49.93; β+

m:49.93;

α:0.15

0

9.947E+05 1.161E+06 8.477E+03 NUBASE

3061 81-Tl-188 7.0+ 1.183 m 1.41

β+:100.00

4

1.658E+06 2.361E+06 ENSDF

3062 81-Tl-188M 7.0+ 1.000E+05 1.183 m 1.41

β+:100.00

0

2.651E+06 2.651E+06 NUBASE

3063 81-Tl-188N 9.0- 1.800E+05 0.041 s 9.76

ITm:100.00

0

8.000E+04 NUBASE

3064 81-Tl-189 0.5+ 2.3 m 8.70

β+:100.00

0

1.676E+06 1.676E+06 NUBASE

3065 81-Tl-189M 4.5- 2.576E+05 1.4 m 7.14

β+m:96.00; IT:4.00

0

1.659E+06 1.670E+06 NUBASE

126 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 127: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3066 81-Tl-190 2.0- 2.6 m 11.54

β+:100.00

0

2.347E+06 2.347E+06 NUBASE

3067 81-Tl-190M 7.0+ 1.300E+05 3.7 m 8.11

β+:100.00

0

2.390E+06 2.390E+06 NUBASE

3068 81-Tl-191 0.5+ 20 m 100

β+:100.00

0

1.437E+06 1.437E+06 NUBASE

3069 81-Tl-191M 4.5- 2.970E+05 5.22 m 3.07

β+m:100.00

0

1.494E+06 1.494E+06 NUBASE

3070 81-Tl-192 2.0- 9.6 m 4.17

β+:100.00

0

2.047E+06 2.047E+06 NUBASE

3071 81-Tl-192M 7.0+ 1.600E+05 10.8 m 1.85

β+:100.00

0

2.100E+06 2.100E+06 NUBASE

3072 81-Tl-193 0.5+ 21.8 m 3.21

β+:100.00

4

9.434E+04 5.559E+05 UKPADD67

3073 81-Tl-193M 4.5- 3.690E+05 2.11 m 7.11

β+:25.00; IT:75.00

4

1.092E+05 3.635E+05 UKPADD67

3074 81-Tl-194 2.0- 33 m 1.52

β+:100.00; α:~

0

1.788E+06 1.788E+06 3.626E-03 NUBASE

3075 81-Tl-194M 7.0+ 3.000E+05 32.8 m 0.61

β+:100.00

0

1.888E+06 1.888E+06 NUBASE

3076 81-Tl-195 0.5+ 1.16 h 4.31

β+:100.00

0

9.483E+05 9.483E+05 NUBASE

3077 81-Tl-195M 4.5- 4.826E+05 3.6 s 11.11

IT:100.00

0

4.826E+05 NUBASE

3078 81-Tl-196 2.0- 1.84 h 1.63

β+:100.00

4

1.710E+05 1.496E+06 ENSDF

3079 81-Tl-196M 7.0+ 3.942E+05 1.41 h 1.42

β+:95.50; IT:4.50

0

1.504E+06 1.522E+06 NUBASE

3080 81-Tl-197 0.5+ 2.84 h 1.41

β+:100.00

4

4.627E+04 4.566E+05 ENSDF

3081 81-Tl-197M 4.5- 6.083E+05 0.54 s 1.85

IT:100.00

3

1.689E+05 4.354E+05 ENSDF

3082 81-Tl-198 2.0- 5.3 h 9.43

β+:100.00

4

3.195E+04 1.984E+06 ENSDF

3083 81-Tl-198M 7.0+ 5.435E+05 1.87 h 1.60

β+:54.00; IT:46.00

4

1.847E+05 1.171E+06 ENSDF

3084 81-Tl-198N 10.0- 7.423E+05 0.032 s 3.12

ITm:100.00

0

1.988E+05 NUBASE

3085 81-Tl-199 0.5+ 7.42 h 1.08

β+:100.00

4

5.230E+04 2.510E+05 ENSDF

3086 81-Tl-199M 4.5- 7.495E+05 0.028 s 0.70

IT:100.00

3

9.447E+04 6.572E+05 ENSDF

3087 81-Tl-200 2.0- 1.087 d 0.38

β+:100.00

4

3.392E+04 1.310E+06 ENSDF

3088 81-Tl-200M 7.0+ 7.536E+05 0.034 s 2.92

IT:100.00

0

7.536E+05 NUBASE

3089 81-Tl-201 0.5+ 3.041 d 0.10

β+:100.00

4

3.739E+04 9.491E+04 LNHB

3090 81-Tl-201M 4.5- 9.195E+05 2.035E-03 s 0.34

IT:100.00

0

9.195E+05 NUBASE

3091 81-Tl-202 2.0- 12.24 d 0.25

β+:100.00

4

2.251E+04 4.665E+05 UKPADD67

3092 81-Tl-203 0.5+

NUBASE

3093 81-Tl-204 2.0- 3.788 y 0.40

β+:2.92; β-:97.08

4

2.369E+05 1.278E+03 LNHB

3094 81-Tl-205 0.5+

NUBASE

3095 81-Tl-206 0.0- 4.202 m 0.40

β-:100.00

4

5.361E+05 2.571E+03 UKHEDD25

3096 81-Tl-206M 12.0- 2.643E+06 3.76 m 1.06

IT:100.00

3

1.533E+05 2.489E+06 UKHEDD25

3097 81-Tl-207 0.5+ 4.77 m 0.63

β-:100.00

4

4.914E+05 3.341E+03 UKHEDD25

3098 81-Tl-207M 5.5- 1.341E+06 1.33 s 8.27

IT:100.00

3

1.837E+05 1.157E+06 UKHEDD25

3099 81-Tl-208 5.0+ 3.053 m 0.13

β-:100.00

4

5.847E+05 3.384E+06 LNHB

3100 81-Tl-209 0.5+ 2.2 m 3.18

β-:100.00

4

6.849E+05 2.122E+06 UKHEDD25

3101 81-Tl-210 5.0+ 1.3 m 2.31

β-:99.99; β-,n:0.01

5

1.092E+06 2.727E+06 5.791E+02 UKHEDD25

3102 81-Tl-211 0.5+ 1 m 100

β-:100.00

0

1.470E+06 1.470E+06 NUBASE

3103 81-Tl-212 5.0+ 30 s 100

β-:100.00

0

1.966E+06 1.966E+06 NUBASE

3104 82-Pb-178 0.0+ 2.3E-04 s 65.22

α:100.00

0

7.790E+06 NUBASE

3105 82-Pb-179 2.5- 3E-03 s 100

α:100.00

0

7.565E+06 NUBASE

3106 82-Pb-180 0.0+ 5E-03 s 60

α:100.00

0

7.415E+06 NUBASE

3107 82-Pb-181 2.5- 0.045 s 44.44

α:98.00; β+:1.00;

β+m:1.00

0

6.157E+04 6.157E+04 7.071E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 127

MAIN DATA TABLES

Page 128: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3108 82-Pb-182 0.0+ 0.06 s 66.67

α:98.00; β+:2.00

0

4.349E+04 4.349E+04 6.925E+06 NUBASE

3109 82-Pb-183 1.5- 0.535 s 5.61

α:90.00; β+:10.00

0

3.006E+05 3.006E+05 6.235E+06 NUBASE

3110 82-Pb-183M 6.5+ 9.400E+04 0.415 s 4.82

α:100.00

0

7.022E+06 NUBASE

3111 82-Pb-184 0.0+ 0.49 s 5.10

α:80.00; β+:20.00

0

3.897E+05 3.897E+05 5.420E+06 NUBASE

3112 82-Pb-185 1.5- 6.3 s 6.35

α:50.00; β+:50.00

0

1.370E+06 1.370E+06 3.348E+06 NUBASE

3113 82-Pb-185M 6.5+ 6.000E+04 4.07 s 3.69

α:50.00; β+

m:50.00

0

1.304E+06 1.304E+06 3.378E+06 NUBASE

3114 82-Pb-186 0.0+ 4.82 s 0.62

β+:60.00; α:40.00

0

1.102E+06 1.102E+06 2.588E+06 NUBASE

3115 82-Pb-187 1.5- 15.2 s 1.97

β+:93.00; α:7.00

0

2.314E+06 2.314E+06 4.477E+05 NUBASE

3116 82-Pb-187M 6.5+ 1.100E+04 18.3 s 1.64

β+m:88.00; α m:12.00

0

2.095E+06 2.095E+06 7.399E+05 NUBASE

3117 82-Pb-188 0.0+ 25.5 s 0.39

β+:90.70; α:9.30

0

1.371E+06 1.371E+06 5.681E+05 NUBASE

3118 82-Pb-189 1.5- 51 s 5.88

β+:99.60; α:0.40

0

2.232E+06 2.232E+06 2.363E+04 NUBASE

3119 82-Pb-189M 6.5+ 4.000E+04 1 m 100

β+m:50.00; IT:50.00

0

1.084E+06 1.104E+06 NUBASE

3120 82-Pb-190 0.0+ 1.183 m 1.41

β+:99.60; α:0.40

0

1.299E+06 1.299E+06 2.279E+04 NUBASE

3121 82-Pb-191 1.5- 1.33 m 6.02

β+:98.97; β+

m:1.02;

α:0.01

0

2.009E+06 2.009E+06 7.076E+02 NUBASE

3122 82-Pb-191M 6.5+ 2.18 m 3.67

β+m:99.98; α m:0.02

0

1.911E+06 1.911E+06 1.083E+03 NUBASE

3123 82-Pb-192 0.0+ 3.5 m 2.86

β+:99.99; α:0.01

0

1.105E+06 1.105E+06 3.080E+02 NUBASE

3124 82-Pb-193 1.5- 5 m 100

β+:100.00

0

1.710E+06 1.710E+06 NUBASE

3125 82-Pb-193M 6.5+ 1.300E+05 5.8 m 3.45

β+:95.30; β+

m:4.70

0

1.748E+06 1.748E+06 NUBASE

3126 82-Pb-194 0.0+ 12 m 4.17

α:~; β+:100.00

5

7.288E+04 1.035E+06 3.387E-01 ENSDF

3127 82-Pb-195 1.5- 15 m 100

β+:100.00

0

1.480E+06 1.480E+06 NUBASE

3128 82-Pb-195M 6.5+ 2.029E+05 15 m 8

β+:56.00; β+

m:44.00

0

1.477E+06 1.477E+06 NUBASE

3129 82-Pb-196 0.0+ 37 m 8.11

β+:100.00; α:~

0

7.120E+05 7.120E+05 1.268E+00 NUBASE

3130 82-Pb-197 1.5- 8 m 25

β+:100.00

4

7.505E+04 1.414E+06 ENSDF

3131 82-Pb-197M 6.5+ 3.193E+05 43 m 2.33

β+:40.50; β+

m:40.50;

IT:19.00; α m:~

0

9.739E+05 1.035E+06 1.217E+01 NUBASE

3132 82-Pb-198 0.0+ 2.4 h 4.17

β+:100.00

4

7.052E+04 4.372E+05 ENSDF

3133 82-Pb-199 1.5- 1.5 h 11.11

β+:100.00

4

5.081E+04 9.599E+05 ENSDF

3134 82-Pb-199M 6.5+ 4.295E+05 12.2 m 2.46

IT:93.00; β+

m:7.00

0

5.859E+04 4.580E+05 NUBASE

3135 82-Pb-200 0.0+ 21.5 h 1.86

β+:100.00

4

9.079E+04 2.080E+05 ENSDF

3136 82-Pb-201 2.5- 9.4 h 1.06

β+:100.00

4

5.828E+04 7.680E+05 UKPADD67

3137 82-Pb-201M 6.5+ 6.291E+05 1.017 m 4.92

IT:100.00

3

2.622E+05 3.661E+05 UKPADD67

3138 82-Pb-202 0.0+ 5.3E+04 y 3.77

β+:100.00

3

9.283E+03 6.997E+04 UKPADD67

3139 82-Pb-202M 9.0- 2.170E+06 3.57 h 0.84

β+:9.10; IT:90.90

4

1.385E+05 1.976E+06 UKPADD67

3140 82-Pb-203 2.5- 2.162 d 0.04

β+:100.00

4

4.754E+04 3.145E+05 LNHB

3141 82-Pb-203M 6.5+ 8.252E+05 6.29 s 1.91

IT:100.00

3

1.712E+05 6.541E+05 UKPADD67

3142 82-Pb-203N 14.5- 2.950E+06 0.48 s 4.17

ITm:100.00

3

2.164E+05 1.907E+06 UKPADD67

3143 82-Pb-204 0.0+ 1.4E+17 y 42.86

α:100.00

1

1.972E+06 UKPADD67

3144 82-Pb-204M 9.0- 2.186E+06 1.125 h 0.74

IT:100.00

3

1.033E+05 2.081E+06 UKPADD67

3145 82-Pb-205 2.5- 1.53E+07 y 4.58

β+:100.00

3

8.953E+03 5.929E+04 UKHEDD25

3146 82-Pb-205M 6.5+ 1.014E+06 5.55E-03 s 0.36

IT:100.00

0

1.014E+06 NUBASE

3147 82-Pb-206 0.0+

NUBASE

3148 82-Pb-207 0.5-

NUBASE

128 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 129: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3149 82-Pb-207M 6.5+ 1.633E+06 0.806 s 0.74

IT:100.00

0

1.633E+06 NUBASE

3150 82-Pb-208 0.0+

NUBASE

3151 82-Pb-209 4.5+ 3.253 h 0.43

β-:100.00

1

1.973E+05 UKHEDD25

3152 82-Pb-210 0.0+ 22.16 y 0.54

β-:100.00; α:~

5

4.072E+04 4.822E+03 7.205E-02 UKHEDD25

3153 82-Pb-211 4.5+ 36.1 m 0.55

β-:100.00

4

4.491E+05 6.845E+04 UKHEDD25

3154 82-Pb-212 0.0+ 10.64 h 0.09

β-:100.00

4

1.687E+05 1.447E+05 LNHB

3155 82-Pb-213 4.5+ 10.2 m 2.94

β-:100.00

0

6.823E+05 6.823E+05 NUBASE

3156 82-Pb-214 0.0+ 26.8 m 3.36

β-:100.00

4

2.925E+05 2.372E+05 LNHB

3157 82-Pb-215 2.5+ 36 s 2.78

β-:100.00

0

9.437E+05 9.437E+05 NUBASE

3158 83-Bi-184 3.0+ 6.6E-03 s 22.73

α:100.00

0

8.025E+06 NUBASE

3159 83-Bi-184M 10.0- 1.500E+05 0.013 s 15.38

α:100.00

0

8.175E+06 NUBASE

3160 83-Bi-185 4.5- 2E-03 s 100

p:85.00; α m:15.00

0

2.412E+06 NUBASE

3161 83-Bi-186 3.0+ 0.015 s 4.73

α:100.00

0

7.755E+06 NUBASE

3162 83-Bi-186M 10.0- 2.500E+05 9.8E-03 s 13.27

α m:100.00

0

7.905E+06 NUBASE

3163 83-Bi-187 4.5- 0.032 s 9.38

α m:50.00; β+

m:50.00

0

1.433E+06 1.433E+06 3.574E+06 NUBASE

3164 83-Bi-187M 0.5+ 1.020E+05 3.2E-04 s 21.88

α:50.00; β+:50.00

0

1.452E+06 1.452E+06 3.946E+06 NUBASE

3165 83-Bi-188 3.0+ 0.044 s 6.82

α:50.00; β+:50.00

0

1.769E+06 1.769E+06 3.633E+06 NUBASE

3166 83-Bi-188M 10.0- 2.100E+05 0.22 s 18.18

α m:50.00; β+:50.00

0

1.804E+06 1.804E+06 3.688E+06 NUBASE

3167 83-Bi-189 4.5- 0.674 s 1.63

α:2.50; α m:47.50;

β+m:50.00

0

1.297E+06 1.297E+06 3.422E+06 NUBASE

3168 83-Bi-189M 0.5+ 1.850E+05 5E-03 s 2

α:50.00; β+:50.00

0

1.334E+06 1.334E+06 3.730E+06 NUBASE

3169 83-Bi-190 3.0+ 6.3 s 1.59

α:77.00; β+:23.00

0

7.296E+05 7.296E+05 5.286E+06 NUBASE

3170 83-Bi-190M 10.0- 2.500E+05 6.2 s 1.61

α n:70.00; β+:30.00

0

9.767E+05 9.767E+05 4.617E+06 NUBASE

3171 83-Bi-191 4.5- 12.3 s 4.07

α m:60.00; β+

m:40.00

0

9.347E+05 9.347E+05 3.868E+06 NUBASE

3172 83-Bi-191M 0.5+ 2.440E+05 0.124 s 4.03

α:75.00; β+:25.00

0

6.045E+05 6.045E+05 5.267E+06 NUBASE

3173 83-Bi-192 3.0+ 34.6 s 2.60

β+:88.00; α:12.00

0

2.642E+06 2.642E+06 7.650E+05 NUBASE

3174 83-Bi-192M 10.0- 2.000E+04 39.6 s 1.01

β+:90.00; α m:9.71;

α n:0.29

0

2.708E+06 2.708E+06 6.293E+05 NUBASE

3175 83-Bi-193 4.5- 1.117 m 4.48

β+m:96.50; α:0.15;

α m:3.35

0

1.990E+06 1.990E+06 2.120E+05 NUBASE

3176 83-Bi-193M 0.5+ 3.080E+05 3.2 s 18.75

α:90.00; β+:10.00

0

2.208E+05 2.208E+05 5.951E+06 NUBASE

3177 83-Bi-194 3.0+ 1.583 m 3.16

β+:99.54; α:0.46

0

2.727E+06 2.727E+06 2.721E+04 NUBASE

3178 83-Bi-194M ? 1.100E+05 2.083 m 1.60

β+:100.00

0

2.776E+06 2.776E+06 NUBASE

3179 83-Bi-194N 10.0- 2.300E+05 1.917 m 3.48

β+:99.80; α m:0.20

0

2.810E+06 2.810E+06 1.203E+04 NUBASE

3180 83-Bi-195 4.5- 3.05 m 2.19

β+m:99.97; α m:0.03

0

1.828E+06 1.828E+06 1.661E+03 NUBASE

3181 83-Bi-195M 0.5+ 3.990E+05 1.45 m 1.15

β+:67.00; α:33.00

0

1.360E+06 1.360E+06 2.056E+06 NUBASE

3182 83-Bi-196 3.0+ 5.1 m 3.92

β+:100.00; α:~

0

2.451E+06 2.451E+06 6.252E+01 NUBASE

3183 83-Bi-196M 7.0+ 1.670E+05 0.6 s 83.33

IT:50.00; β+:50.00

0

1.253E+06 1.337E+06 NUBASE

3184 83-Bi-196N 10.0- 2.700E+05 4 m 1.25

β+:74.20; ITm:25.80;

α m:~

0

1.885E+06 1.912E+06 2.108E+01 NUBASE

3185 83-Bi-197 4.5- 9.3 m 5.38

β+m:100.00; α m:~

0

1.581E+06 1.581E+06 4.838E+00 NUBASE

3186 83-Bi-197M 0.5+ 3.600E+05 5.04 m 3.17

α:54.84; β+:44.87;

IT:0.30

0

8.107E+05 8.118E+05 3.053E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 129

MAIN DATA TABLES

Page 130: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3187 83-Bi-198 ? 10.3 m 2.91

β+:100.00

0

2.227E+06 2.227E+06 NUBASE

3188 83-Bi-198M 7.0+ 2.800E+05 11.6 m 2.59

β+:100.00

0

2.320E+06 2.320E+06 NUBASE

3189 83-Bi-198N 10.0- 5.300E+05 7.7 s 6.49

ITm:100.00

0

2.500E+05 NUBASE

3190 83-Bi-199 4.5- 27 m 3.70

β+:53.90; β+

m:46.10

0

1.411E+06 1.411E+06 NUBASE

3191 83-Bi-199M 0.5+ 6.670E+05 24.7 m 0.61

β+:97.99; IT:2.00;

α:0.01

0

1.665E+06 1.678E+06 5.599E+02 NUBASE

3192 83-Bi-200 7.0+ 36.4 m 1.37

β+:100.00

0

1.958E+06 1.958E+06 NUBASE

3193 83-Bi-200M 2.0+ 1.000E+05 31 m 6.45

β+:90.00; IT:10.00

0

1.792E+06 1.802E+06 NUBASE

3194 83-Bi-200N 10.0- 4.282E+05 0.4 s 12.50

IT:100.00

0

4.282E+05 NUBASE

3195 83-Bi-201 4.5- 1.8 h 2.78

β+:55.30; β+

m:44.70;

α m:~

0

1.187E+06 1.187E+06 3.892E+00 NUBASE

3196 83-Bi-201M 0.5+ 8.463E+05 59.1 m 1.02

β+:46.45; β+

m:46.45;

IT:6.80; α:0.30

0

1.354E+06 1.412E+06 1.604E+04 NUBASE

3197 83-Bi-202 5.0+ 1.72 h 2.91

β+:100.00

4

1.365E+05 2.460E+06 ENSDF

3198 83-Bi-203 4.5- 11.76 h 0.43

β+:80.00; β+

m:20.00;

α m:~

0

1.027E+06 1.027E+06 3.344E-01 NUBASE

3199 83-Bi-203M 0.5+ 1.098E+06 0.303 s 1.65

IT:100.00

0

1.098E+06 NUBASE

3200 83-Bi-204 6.0+ 11.22 h 0.89

β+:91.10; β+

m:8.90

0

1.416E+06 1.416E+06 NUBASE

3201 83-Bi-204M 10.0- 8.055E+05 0.013 s 0.77

IT:100.00

0

8.055E+05 NUBASE

3202 83-Bi-204N 17.0+ 2.833E+06 1.07E-03 s 2.80

ITm:100.00

0

2.028E+06 NUBASE

3203 83-Bi-205 4.5- 15.31 d 0.26

β+:85.80; β+

m:14.20

0

8.547E+05 8.547E+05 NUBASE

3204 83-Bi-206 6.0+ 6.243 d 0.05

β+:100.00

4

1.238E+05 3.274E+06 ENSDF

3205 83-Bi-207 4.5- 31.76 y 6.03

β+:100.00

4

1.185E+05 1.540E+06 UKPADD67

3206 83-Bi-208 5.0+ 3.68E+05 y 1.09

β+:100.00

4

8.518E+03 2.657E+06 UKPADD67

3207 83-Bi-208M 10.0- 1.571E+06 2.58E-03 s 1.55

IT:100.00

3

7.229E+04 1.501E+06 ENSDF

3208 83-Bi-209 4.5- 1.9E+19 y 10.53

α:100.00

0

3.137E+06 NUBASE

3209 83-Bi-210 1.0- 5.012 d 0.10

β-:100.00; α:~

5

3.877E+05 6.767E+02 6.266E+00 UKHEDD25

3210 83-Bi-210M 9.0- 2.650E+05 3E+06 y 3.33

α:100.00

4

4.694E+04 2.611E+05 5.009E+06 UKHEDD25

3211 83-Bi-211 4.5- 2.17 m 1.84

β-:0.27; α:99.73

5

1.006E+04 4.758E+04 6.675E+06 UKHEDD25

3212 83-Bi-212 1.0- 1.009 h 0.10

β-:64.06; β-,α:0.01;

α:35.93

5

5.026E+05 1.073E+05 2.217E+06 UKHEDD25

3213 83-Bi-212M 9.0- 2.500E+05 25 m 4

β-:3.20; β-,α:30.00;

α:66.80

5

1.337E+05 6.048E+04 7.423E+06 UKHEDD25

3214 83-Bi-212N 17.0- 3.930E+06 9 m 11.11

β-m:100.00

1

1.257E+06 5.061E+03 UKHEDD25

3215 83-Bi-213 4.5- 45.59 m 0.13

β-:97.84; α:2.16

5

4.444E+05 1.292E+05 1.287E+05 UKHEDD25

3216 83-Bi-214 1.0- 19.9 m 2.01

β-:99.98; α:0.02

5

6.286E+05 1.540E+06 1.168E+03 UKHEDD25

3217 83-Bi-215 4.5- 7.4 m 8.11

β-:100.00

0

7.507E+05 7.507E+05 UKHEDD25

3218 83-Bi-215M 12.5- 1.348E+06 36.9 s 1.63

IT:50.00; β-:50.00

0

5.895E+05 1.263E+06 NUBASE

3219 83-Bi-216 1.0- 2.17 m 2.30

β-:100.00

0

1.363E+06 1.363E+06 NUBASE

3220 83-Bi-217 4.5- 1.642 m 0.81

β-:100.00

0

9.730E+05 9.730E+05 NUBASE

3221 83-Bi-218 1.0- 33 s 3.03

β-:100.00

0

1.661E+06 1.661E+06 NUBASE

3222 84-Po-188 0.0+ 4.3E-04 s 41.86

α:50.00; β+:50.00

0

1.110E+06 1.110E+06 4.041E+06 NUBASE

130 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 131: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3223 84-Po-189 1.5- 5E-03 s 20

α:25.00; α m:25.00;

β+m:50.00

0

1.410E+06 1.410E+06 3.836E+06 NUBASE

3224 84-Po-190 0.0+ 2.45E-03 s 2.04

α:100.00

2

7.680E+06 ENSDF

3225 84-Po-191 1.5- 0.022 s 4.55

α:100.00

0

7.501E+06 NUBASE

3226 84-Po-191M 6.5+ 3.400E+04 0.098 s 8.16

α m:100.00

0

7.524E+06 NUBASE

3227 84-Po-192 0.0+ 0.033 s 4.22

α:99.50

2

7.267E+06 ENSDF

3228 84-Po-193 1.5- 0.42 s 9.52

α:100.00

2

7.092E+06 ENSDF

3229 84-Po-193M 6.5+ 1.000E+05 0.24 s 4.17

α:100.00

2

7.145E+06 ENSDF

3230 84-Po-194 0.0+ 0.392 s 1.02

α:100.00

0

6.987E+06 NUBASE

3231 84-Po-195 1.5- 4.64 s 1.94

α:75.00; β+

m:25.00

0

5.462E+05 5.462E+05 5.066E+06 NUBASE

3232 84-Po-195M 6.5+ 8.000E+04 1.92 s 1.04

α m:89.99; β+:10.00;

IT:0.01

0

2.344E+05 2.345E+05 6.151E+06 NUBASE

3233 84-Po-196 0.0+ 5.56 s 2.16

α:94.00; β+:6.00

0

9.070E+04 9.070E+04 6.258E+06 NUBASE

3234 84-Po-197 1.5- 53.6 s 1.87

β+m:56.00; α:44.00

0

1.114E+06 1.114E+06 2.818E+06 NUBASE

3235 84-Po-197M 6.5+ 2.300E+05 25.8 s 0.39

α m:84.00; β+:15.99;

IT:0.01

0

3.495E+05 3.496E+05 5.464E+06 NUBASE

3236 84-Po-198 0.0+ 1.77 m 1.69

α:57.00; β+:43.00

0

5.584E+05 5.584E+05 3.597E+06 NUBASE

3237 84-Po-199 1.5- 5.48 m 2.92

β+m:92.50; α:7.50

0

1.516E+06 1.516E+06 4.556E+05 NUBASE

3238 84-Po-199M 6.5+ 3.120E+05 4.17 m 0.96

β+:73.50; α m:24.00;

IT:2.50

0

1.444E+06 1.452E+06 1.484E+06 NUBASE

3239 84-Po-200 0.0+ 11.5 m 0.87

β+m:88.90; α:11.10

0

9.826E+05 9.826E+05 6.640E+05 NUBASE

3240 84-Po-201 1.5- 15.3 m 1.31

β+m:98.40; α:1.60

0

1.327E+06 1.327E+06 9.279E+04 NUBASE

3241 84-Po-201M 6.5+ 4.241E+05 8.9 m 2.25

IT:56.06; β+:41.04;

α m:2.90

0

7.271E+05 9.649E+05 1.714E+05 NUBASE

3242 84-Po-202 0.0+ 44.7 m 1.12

β+:98.08; α:1.92

0

9.184E+05 9.184E+05 1.095E+05 NUBASE

3243 84-Po-203 2.5- 36.7 m 1.36

α:0.11; β+:99.89

5

1.363E+05 1.381E+06 5.981E+03 ENSDF

3244 84-Po-203M 6.5+ 6.415E+05 45 s 4.44

IT:99.96; α m:0.04

0

6.412E+05 2.283E+03 NUBASE

3245 84-Po-204 0.0+ 3.53 h 0.57

β+:49.67; β+

m:49.67;

α:0.66

0

6.392E+05 6.392E+05 3.620E+04 NUBASE

3246 84-Po-205 2.5- 1.66 h 1.20

α:0.04; β+:99.90

5

5.259E+04 1.459E+06 2.090E+03 ENSDF

3247 84-Po-205M 9.5- 1.461E+06 0.057 s 1.57

IT:100.00

0

1.461E+06 NUBASE

3248 84-Po-206 0.0+ 8.8 d 1.14

β+:94.55; α:5.45

0

5.818E+05 5.818E+05 2.903E+05 NUBASE

3249 84-Po-207 2.5- 5.8 h 0.34

α:0.02; β+:99.98

5

4.202E+04 1.274E+06 1.073E+03 ENSDF

3250 84-Po-207M 9.5- 1.383E+06 2.79 s 2.87

IT:100.00

3

2.848E+05 1.075E+06 ENSDF

3251 84-Po-208 0.0+ 2.93 y 1.37

β+:~; α:100.00

5

2.860E+00 1.721E+01 5.215E+06 UKPADD67

3252 84-Po-209 0.5- 102.002 y 4.90

β+:0.26; α:99.74

5

4.443E+02 5.150E+03 4.964E+06 UKHEDD25

3253 84-Po-210 0.0+ 138.388 d ~

α:100.00

4

9.327E-02 9.725E+00 5.408E+06 UKHEDD25

3254 84-Po-211 4.5+ 0.516 s 0.58

α:100.00

4

1.573E+02 7.747E+03 7.586E+06 UKHEDD25

3255 84-Po-211M 12.5+ 1.463E+06 25.5 s 1.18

α:100.00

4

1.007E+04 1.490E+06 7.550E+06 UKHEDD25

3256 84-Po-212 0.0+ 2.98E-07 s 1.01

α:100.00

1

8.955E+06 LNHB

3257 84-Po-212M 18.0+ 2.922E+06 45.1 s 1.33

α:100.00

4

3.770E+02 9.123E+04 1.178E+07 UKHEDD25

3258 84-Po-213 4.5+ 4.2E-06 s 19.05

α:100.00

4

7.491E-01 2.344E+01 8.536E+06 UKHEDD25

3259 84-Po-214 0.0+ 1.637E-04 s 0.12

α:100.00

4

8.284E-01 8.419E+01 7.833E+06 UKHEDD25

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 131

MAIN DATA TABLES

Page 132: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3260 84-Po-215 4.5+ 1.78E-03 s 0.56

β-:~; α:100.00

5

3.148E+01 2.157E+02 7.526E+06 UKHEDD25

3261 84-Po-216 0.0+ 0.15 s 3.33

α:100.00

4

1.468E-01 1.531E+01 6.907E+06 UKHEDD25

3262 84-Po-217 2.5+ 1.47 s 3.40

α:95.00; β-:5.00

0

2.508E+04 2.508E+04 6.327E+06 NUBASE

3263 84-Po-218 0.0+ 3.098 m 0.26

β-:0.02; α:99.98

5

1.369E+01 9.213E+00 6.114E+06 UKHEDD25

3264 84-Po-219 3.5+ 2 m 100

β-:50.00; α:50.00

0

4.005E+05 4.005E+05 2.948E+06 NUBASE

3265 84-Po-220 0.0+ 40 s 100

β-:100.00

0

3.733E+05 3.733E+05 NUBASE

3266 85-At-193 4.5- 0.04 s 100

α:100.00

0

7.485E+06 NUBASE

3267 85-At-194 3.0+ 0.04 s 100

α:100.00

0

7.285E+06 NUBASE

3268 85-At-194M 10.0- 2.500E+05 0.25 s 100

α m:100.00

0

7.285E+06 NUBASE

3269 85-At-195 4.5- 0.328 s 6.10

α:100.00

0

7.339E+06 NUBASE

3270 85-At-195M 0.5+ 0.147 s 3.40

α m:75.00; β+:25.00

0

6.328E+05 6.328E+05 5.321E+06 NUBASE

3271 85-At-196 3.0+ 0.253 s 3.56

α:96.00; β+:4.00

0

1.274E+05 1.274E+05 6.917E+06 NUBASE

3272 85-At-196M 10.0- 2.000E+05 0.02 s 100

IT:100.00

0

2.000E+05 NUBASE

3273 85-At-197 4.5- 0.35 s 11.43

α:96.00; β+

m:4.00

0

9.053E+04 9.053E+04 6.824E+06 NUBASE

3274 85-At-197M 0.5+ 5.000E+04 3.7 s 67.57

α m:100.00; IT:~

0

2.000E+00 6.850E+06 NUBASE

3275 85-At-198 3.0+ 4.2 s 7.14

α:94.00; β+:6.00

0

1.761E+05 1.761E+05 6.481E+06 NUBASE

3276 85-At-198M 10.0- 3.300E+05 1 s 20

α n:86.00; β+:14.00

0

4.262E+05 4.262E+05 6.016E+06 NUBASE

3277 85-At-199 4.5- 7.2 s 6.94

α:89.00; β+

m:11.00

0

2.230E+05 2.230E+05 6.033E+06 NUBASE

3278 85-At-200 3.0+ 43.2 s 2.08

α:57.00; β+:43.00

0

1.142E+06 1.142E+06 3.760E+06 NUBASE

3279 85-At-200M 7.0+ 1.130E+05 47 s 2.13

α m:43.00; β+:28.50;

IT:28.50

0

7.675E+05 7.997E+05 2.813E+06 NUBASE

3280 85-At-200N 10.0- 3.440E+05 3.5 s 5.71

ITm:84.85; α n:10.61;

β+:4.55

0

1.259E+05 3.219E+05 7.074E+05 NUBASE

3281 85-At-201 4.5- 1.417 m 3.53

α:71.00; β+

m:29.00

0

5.135E+05 5.135E+05 4.597E+06 NUBASE

3282 85-At-202 ? 3.067 m 0.54

β+:82.00; α:18.00

0

2.004E+06 2.004E+06 1.144E+06 NUBASE

3283 85-At-202M 7.0+ 1.900E+05 3.033 m 1.10

IT:45.65; β+:45.65;

α m:8.70

0

1.145E+06 1.231E+06 5.449E+05 NUBASE

3284 85-At-202N 10.0- 5.800E+05 0.46 s 10.87

ITm:99.65; β+:0.25;

α n:0.10

0

6.594E+03 3.952E+05 6.147E+03 NUBASE

3285 85-At-203 4.5- 7.4 m 2.70

β+:34.50; β+

m:34.50;

α:31.00

0

1.109E+06 1.109E+06 1.925E+06 NUBASE

3286 85-At-204 7.0+ 9.2 m 2.17

β+:96.20; α:3.80

0

2.071E+06 2.071E+06 2.307E+05 NUBASE

3287 85-At-204M 10.0- 5.873E+05 0.108 s 9.26

IT:100.00

0

5.873E+05 NUBASE

3288 85-At-205 4.5- 26.9 m 0.30

β+:45.00; β+

m:45.00;

α:10.00

0

1.142E+06 1.142E+06 6.019E+05 NUBASE

3289 85-At-206 5.0+ 30 m 2

α:0.89; β+:99.11

5

3.030E+05 2.303E+06 5.180E+04 ENSDF

3290 85-At-207 4.5- 1.8 h 2.22

β+:91.40; α:8.60

0

1.189E+06 1.189E+06 5.050E+05 NUBASE

3291 85-At-208 6.0+ 1.63 h 1.84

β+:99.45; α:0.55

0

1.650E+06 1.650E+06 3.163E+04 NUBASE

3292 85-At-209 4.5- 5.41 h 0.92

β+:95.90; α:4.10

0

1.114E+06 1.114E+06 2.360E+05 NUBASE

3293 85-At-210 5.0+ 8.1 h 4.94

α:0.18; β+:99.83

5

6.930E+04 2.964E+06 9.558E+03 ENSDF

3294 85-At-211 4.5- 7.214 h 0.10

α:41.80; β+:58.20

5

3.065E+03 3.915E+04 2.501E+06 ENSDF

3295 85-At-212 1.0- 0.314 s 0.64

α:100.00

1

7.786E+06 ENSDF

3296 85-At-212M 9.0- 2.220E+05 0.119 s 2.52

α:100.00

3

3.142E+04 4.805E+03 7.990E+06 ENSDF

132 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 133: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3297 85-At-213 4.5- 1.25E-07 s 4.80

α:100.00

1

9.254E+06 ENSDF

3298 85-At-214 1.0- 5.58E-07 s 1.79

α:100.00

1

8.983E+06 ENSDF

3299 85-At-215 4.5- 1E-04 s 20

α:100.00

4

1.651E+01 1.853E+02 8.178E+06 UKHEDD25

3300 85-At-216 1.0- 3E-04 s 10

α:100.00

1

7.957E+06 ENSDF

3301 85-At-217 4.5- 0.032 s 1.24

β-:0.01; α:99.99

5

8.290E+01 2.999E+02 7.199E+06 UKHEDD25

3302 85-At-218 1.0- 1.5 s 20

β-:0.10; α:99.90

5

5.247E+04 1.186E+04 6.804E+06 UKHEDD25

3303 85-At-219 2.5- 54 s 11.11

β-:3.00; α:97.00

2

1.786E+04 5.023E+01 6.195E+06 UKHEDD25

3304 85-At-220 3.0+ 3.71 m 1.08

α:8.00; β-:92.00

5

1.183E+06 3.724E+05 4.843E+05 ENSDF

3305 85-At-221 1.5- 2.3 m 8.70

β-:100.00

0

7.793E+05 7.793E+05 NUBASE

3306 85-At-222 ? 54 s 18.52

β-:100.00

0

1.475E+06 1.475E+06 NUBASE

3307 85-At-223 1.5- 50 s 14

β-:100.00

0

1.053E+06 1.053E+06 NUBASE

3308 86-Rn-195 1.5- 6E-03 s 50

α:100.00

0

7.699E+06 NUBASE

3309 86-Rn-195M 6.5+ 5.000E+04 6E-03 s 50

α m:100.00

0

7.715E+06 NUBASE

3310 86-Rn-196 0.0+ 3E-03 s 233.33

α:99.80

1

7.606E+06 ENSDF

3311 86-Rn-197 1.5- 0.065 s 38.46

α:100.00

1

7.412E+06 ENSDF

3312 86-Rn-197M 6.5+ 2.000E+05 0.019 s 42.11

α m:100.00

1

7.523E+06 ENSDF

3313 86-Rn-198 0.0+ 0.057 s 15.79

α:99.40

1

7.310E+06 ENSDF

3314 86-Rn-199 1.5- 0.62 s 4.84

α:94.00; β+:6.00

0

1.460E+05 1.460E+05 6.698E+06 NUBASE

3315 86-Rn-199M 6.5+ 1.500E+05 0.32 s 6.25

α m:97.00; β+:3.00

0

7.450E+04 7.450E+04 6.979E+06 NUBASE

3316 86-Rn-200 0.0+ 1.03 s 4.85

α:98.00; β+:2.00

0

3.321E+04 3.321E+04 6.902E+06 NUBASE

3317 86-Rn-201 1.5- 7 s 5.71

α:80.00; β+:20.00

0

4.479E+05 4.479E+05 5.492E+06 NUBASE

3318 86-Rn-201M 6.5+ 2.800E+05 3.8 s 2.63

α m:89.99; β+:10.00;

IT:0.01

0

2.333E+05 2.333E+05 6.223E+06 NUBASE

3319 86-Rn-202 0.0+ 9.94 s 1.81

α:86.00; β+:14.00

0

2.014E+05 2.014E+05 5.825E+06 NUBASE

3320 86-Rn-203 ? 43.5 s 4.83

α:66.00; β+:34.00

0

6.803E+05 6.803E+05 4.376E+06 NUBASE

3321 86-Rn-203M 6.5+ 3.630E+05 26.7 s 1.87

α m:80.00; β+:20.00

0

4.244E+05 4.244E+05 5.345E+06 NUBASE

3322 86-Rn-204 0.0+ 1.24 m 2.42

α:73.00; β+:13.50;

β+m:13.50

0

3.238E+05 3.238E+05 4.778E+06 NUBASE

3323 86-Rn-205 2.5- 2.8 m 3.57

β+:75.40; α:24.60

0

1.323E+06 1.323E+06 1.572E+06 NUBASE

3324 86-Rn-206 0.0+ 5.67 m 3

α:62.00; β+:38.00

0

4.185E+05 4.185E+05 3.958E+06 NUBASE

3325 86-Rn-207 2.5- 9.25 m 1.84

β+:79.00; α:21.00

0

1.214E+06 1.214E+06 1.313E+06 NUBASE

3326 86-Rn-208 0.0+ 24.35 m 0.57

α:62.00; β+:38.00

0

3.601E+05 3.601E+05 3.882E+06 NUBASE

3327 86-Rn-209 2.5- 28.5 m 3.51

α:17.00; β+:83.00

5

1.118E+05 9.774E+05 1.047E+06 ENSDF

3328 86-Rn-210 0.0+ 2.4 h 4.17

α:96.00; β+:4.00

5

8.138E+03 5.881E+04 5.912E+06 ENSDF

3329 86-Rn-211 0.5- 14.6 h 1.37

β+:72.60; α:27.40

0

6.996E+05 6.996E+05 1.634E+06 NUBASE

3330 86-Rn-212 0.0+ 23.9 m 5.02

α:100.00

1

6.384E+06 ENSDF

3331 86-Rn-213 4.5+ 0.025 s 0.80

α:100.00

1

8.238E+06 ENSDF

3332 86-Rn-214 0.0+ 2.7E-07 s 7.41

α:100.00

0

9.208E+06 NUBASE

3333 86-Rn-215 4.5+ 2.3E-06 s 4.35

α:100.00

1

8.839E+06 ENSDF

3334 86-Rn-216 0.0+ 4.5E-05 s 11.11

α:100.00

0

8.200E+06 NUBASE

3335 86-Rn-217 4.5+ 5.4E-04 s 9.26

α:100.00

4

8.395E+01 1.534E+02 7.884E+06 UKHEDD25

3336 86-Rn-218 0.0+ 0.035 s 25.71

α:100.00

4

1.399E+01 7.571E+02 7.262E+06 UKHEDD25

3337 86-Rn-219 2.5+ 3.96 s 1.26

α:100.00

4

6.673E+03 5.529E+04 6.885E+06 UKHEDD25

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 133

MAIN DATA TABLES

Page 134: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3338 86-Rn-220 0.0+ 55.8 s 0.54

α:100.00

4

1.452E+01 6.285E+02 6.404E+06 UKHEDD25

3339 86-Rn-221 3.5+ 25 m 8

α:20.00; β-:78.00

5

2.775E+05 1.171E+05 1.220E+06 ENSDF

3340 86-Rn-222 0.0+ 3.823 d 0.01

α:100.00

4

1.097E+01 3.894E+02 5.590E+06 UKHEDD25

3341 86-Rn-223 3.5- 24.2 m 2.89

β-:100.00

4

6.249E+05 3.301E+05 UKPADD67

3342 86-Rn-224 0.0+ 1.783 h 2.80

β-:100.00

0

2.600E+05 2.600E+05 NUBASE

3343 86-Rn-225 3.5- 4.66 m 0.86

β-:100.00

0

8.933E+05 8.933E+05 NUBASE

3344 86-Rn-226 0.0+ 7.4 m 1.35

β-:100.00

0

4.667E+05 4.667E+05 NUBASE

3345 86-Rn-227 2.5+ 20.8 s 3.37

β-:100.00

0

1.110E+06 1.110E+06 NUBASE

3346 86-Rn-228 0.0+ 1.083 m 3.08

β-:100.00

0

7.000E+05 7.000E+05 NUBASE

3347 87-Fr-199 1.5- 0.016 s 43.75

α:100.00

0

7.811E+06 NUBASE

3348 87-Fr-200 3.0+ 0.024 s 41.67

α:100.00

0

7.615E+06 NUBASE

3349 87-Fr-200M 10.0- 2.000E+05 0.65 s 32.31

α m:100.00

0

7.615E+06 NUBASE

3350 87-Fr-201 4.5- 0.048 s 31.25

α:100.00

1

7.538E+06 ENSDF

3351 87-Fr-202 3.0+ 0.29 s 10.34

α:97.00; β+:3.00

0

9.415E+04 9.415E+04 7.164E+06 NUBASE

3352 87-Fr-202M 10.0- 3.300E+05 0.34 s 11.76

α m:97.00; β+:3.00

0

9.745E+04 9.745E+04 7.164E+06 NUBASE

3353 87-Fr-203 4.5- 0.55 s 3.64

α:95.00; β+:2.50;

β+m:2.50

0

1.140E+05 1.140E+05 6.893E+06 NUBASE

3354 87-Fr-204 3.0+ 1.7 s 17.65

α:96.00; β+:4.00

0

1.146E+05 1.146E+05 6.884E+06 NUBASE

3355 87-Fr-204M 7.0+ 5.400E+04 2.6 s 11.54

α m:90.00; β+:10.00

0

2.882E+05 2.882E+05 6.401E+06 NUBASE

3356 87-Fr-204N 10.0- 3.300E+05 1.7 s 35.29

α n:74.00; ITm:26.00

0

7.176E+04 5.296E+06 NUBASE

3357 87-Fr-205 4.5- 3.92 s 1.02

α:99.00; β+:1.00

0

2.133E+04 2.133E+04 6.984E+06 NUBASE

3358 87-Fr-206 ? 16 s 100

β+:58.00; α:42.00

0

1.522E+06 1.522E+06 2.908E+06 NUBASE

3359 87-Fr-206M 7.0+ 1.900E+05 15.9 s 0.63

α m:42.00; β+:29.00;

IT:29.00

0

7.794E+05 8.345E+05 2.908E+06 NUBASE

3360 87-Fr-206N 10.0- 7.200E+05 0.7 s 14.29

ITm:88.00; α n:12.00

0

4.664E+05 8.476E+05 NUBASE

3361 87-Fr-207 4.5- 14.8 s 0.68

α:95.00; β+:5.00

0

9.652E+04 9.652E+04 6.553E+06 NUBASE

3362 87-Fr-208 7.0+ 59.1 s 0.51

α:90.00; β+:10.00

0

2.326E+05 2.326E+05 6.102E+06 NUBASE

3363 87-Fr-209 4.5- 50 s 0.60

α:89.00; β+:11.00

0

1.892E+05 1.892E+05 6.033E+06 NUBASE

3364 87-Fr-210 6.0+ 3.18 m 1.89

α:60.00; β+:40.00

0

8.336E+05 8.336E+05 3.989E+06 NUBASE

3365 87-Fr-211 4.5- 3.1 m 0.65

α:80.00; β+:20.00

0

3.065E+05 3.065E+05 5.328E+06 NUBASE

3366 87-Fr-212 5.0+ 20 m 3

β+:57.00; α:43.00

0

9.732E+05 9.732E+05 2.807E+06 NUBASE

3367 87-Fr-213 4.5- 34.6 s 0.87

α:99.45; β+:0.55

0

3.938E+03 3.938E+03 6.867E+06 NUBASE

3368 87-Fr-214 1.0- 5E-03 s 4

α:100.00

1

8.581E+06 ENSDF

3369 87-Fr-214M 9.0- 1.220E+05 3.35E-03 s 1.49

α:100.00

1

8.664E+06 ENSDF

3370 87-Fr-215 4.5- 8.6E-08 s 5.81

α:100.00

1

9.538E+06 ENSDF

3371 87-Fr-216 1.0- 7E-07 s 2.86

α:100.00

1

9.175E+06 ENSDF

3372 87-Fr-217 4.5- 2.2E-05 s 22.73

α:100.00

1

8.472E+06 ENSDF

3373 87-Fr-218 1.0- 1E-03 s 60

α:100.00

1

7.955E+06 ENSDF

3374 87-Fr-218M ? 8.600E+04 0.022 s 2.27

α:100.00

0

8.100E+06 NUBASE

3375 87-Fr-219 4.5- 0.02 s 10

α:100.00

4

4.125E+02 3.550E+03 7.443E+06 ENSDF

3376 87-Fr-220 1.0+ 27.4 s 1.09

α:99.65; β-:0.35

5

1.372E+04 9.658E+03 6.673E+06 ENSDF

3377 87-Fr-221 2.5- 4.9 m 4.08

α:100.00

4

8.822E+03 2.982E+04 6.471E+06 UKHEDD25

3378 87-Fr-222 2.0- 14.2 m 2.11

β-:100.00

4

7.152E+05 1.772E+05 ENSDF

134 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 135: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3379 87-Fr-223 1.5- 21.8 m 1.83

β-:99.99; α:0.01

5

3.791E+05 5.899E+04 3.263E+02 UKHEDD25

3380 87-Fr-224 1.0- 3.33 m 3

β-:100.00

4

8.769E+05 5.353E+05 ENSDF

3381 87-Fr-225 1.5- 4 m 5

β-:100.00

0

6.053E+05 6.053E+05 NUBASE

3382 87-Fr-226 1.0- 49 s 2.04

β-:100.00

4

1.221E+06 4.361E+05 ENSDF

3383 87-Fr-227 0.5+ 2.47 m 1.21

β-:100.00

4

7.668E+05 4.349E+05 ENSDF

3384 87-Fr-228 2.0- 38 s 2.63

β-:100.00

4

1.437E+06 6.664E+05 ENSDF

3385 87-Fr-229 0.5+ 50.2 s 0.80

β-:100.00

0

1.086E+06 1.086E+06 NUBASE

3386 87-Fr-230 ? 19.1 s 2.62

β-:100.00

0

1.694E+06 1.694E+06 NUBASE

3387 87-Fr-231 0.5+ 17.6 s 3.41

β-:100.00

4

1.373E+06 4.421E+05 ENSDF

3388 87-Fr-232 ? 5 s 20

β-:100.00

0

1.903E+06 1.903E+06 NUBASE

3389 88-Ra-202 0.0+ 2.6E-03 s 80.77

α:100.00

0

8.016E+06 NUBASE

3390 88-Ra-203 1.5- 1E-03 s 500

α:100.00

1

7.730E+06 ENSDF

3391 88-Ra-203M 1.5- 1.900E+05 0.033 s 66.67

α:100.00

1

7.768E+06 ENSDF

3392 88-Ra-204 0.0+ 0.06 s 18.33

α:99.70; β+:0.30

0

5.446E+03 5.446E+03 7.612E+06 NUBASE

3393 88-Ra-205 1.5- 0.22 s 22.73

α:50.00; β+:50.00

0

1.192E+06 1.192E+06 3.743E+06 NUBASE

3394 88-Ra-205M 6.5+ 2.900E+05 0.18 s 27.78

α m:50.00; IT:50.00

0

1.450E+05 3.748E+06 NUBASE

3395 88-Ra-206 0.0+ 0.24 s 8.33

α:100.00

0

7.415E+06 NUBASE

3396 88-Ra-207 ? 1.3 s 15.38

α:90.00; β+:10.00

0

2.127E+05 2.127E+05 6.548E+06 NUBASE

3397 88-Ra-207M 6.5+ 5.600E+05 0.057 s 14.04

IT:85.00; α m:14.45;

β+:0.55

0

1.272E+04 4.887E+05 1.080E+06 NUBASE

3398 88-Ra-208 0.0+ 1.3 s 15.38

α:95.00; β+:5.00

0

7.307E+04 7.307E+04 6.909E+06 NUBASE

3399 88-Ra-209 2.5- 4.6 s 4.35

α:90.00; β+:10.00

0

1.873E+05 1.873E+05 6.422E+06 NUBASE

3400 88-Ra-210 0.0+ 3.7 s 5.41

α:96.00; β+:4.00

0

5.076E+04 5.076E+04 6.866E+06 NUBASE

3401 88-Ra-211 2.5- 13 s 15.38

α:93.00; β+:7.00

0

1.165E+05 1.165E+05 6.549E+06 NUBASE

3402 88-Ra-212 0.0+ 13 s 1.54

α:85.00; β+:15.00

0

1.674E+05 1.674E+05 5.977E+06 NUBASE

3403 88-Ra-213 0.5- 2.74 m 2.19

α:80.00; β+:20.00

0

2.605E+05 2.605E+05 5.490E+06 NUBASE

3404 88-Ra-213M 6.5+ 1.770E+06 2.1E-03 s 4.76

α:1.00; IT:99.00

4

9.988E+04 1.635E+06 8.591E+04 ENSDF

3405 88-Ra-214 0.0+ 2.46 s 1.22

α:99.94; β+

m:0.06

0

1.841E+02 1.841E+02 7.270E+06 NUBASE

3406 88-Ra-215 4.5+ 1.59E-03 s 5.66

α:100.00

1

8.834E+06 ENSDF

3407 88-Ra-216 0.0+ 1.82E-07 s 5.49

α:100.00; β+:~

0

1.560E-06 3.120E-06 9.526E+06 NUBASE

3408 88-Ra-217 4.5+ 1.6E-06 s 12.50

α:100.00

1

9.161E+06 ENSDF

3409 88-Ra-218 0.0+ 2.56E-05 s 4.30

α:100.00

0

8.546E+06 NUBASE

3410 88-Ra-219 3.5+ 0.01 s 30

α:100.00

4

5.652E+04 1.710E+05 7.946E+06 ENSDF

3411 88-Ra-220 0.0+ 0.018 s 11.11

α:100.00

2

4.650E+03 7.589E+06 ENSDF

3412 88-Ra-221 2.5+ 28 s 7.14

α:100.00

0

6.880E+06 NUBASE

3413 88-Ra-222 0.0+ 38 s 1.32

α:100.00

4

8.336E+02 9.191E+03 6.667E+06 ENSDF

3414 88-Ra-223 0.5+ 11.43 d 0.17

α:100.00

4

7.474E+04 1.343E+05 5.782E+06 UKHEDD25

3415 88-Ra-224 0.0+ 3.64 d 0.82

α:100.00

4

2.352E+03 1.043E+04 5.776E+06 UKHEDD25

3416 88-Ra-225 1.5+ 14.8 d 1.35

β-:100.00

4

1.078E+05 1.383E+04 UKHEDD25

3417 88-Ra-226 0.0+ 1600.001 y 0.44

α:100.00

4

3.499E+03 7.256E+03 4.859E+06 LNHB

3418 88-Ra-227 1.5+ 42.2 m 1.18

β-:100.00

0

4.427E+05 4.427E+05 NUBASE

3419 88-Ra-228 0.0+ 5.75 y 0.52

β-:100.00

4

2.147E+04 2.005E+03 UKHEDD25

3420 88-Ra-229 2.5+ 4 m 5

β-:100.00

1

6.134E+05 ENSDF

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 135

MAIN DATA TABLES

Page 136: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3421 88-Ra-230 0.0+ 1.55 h 2.15

β-:100.00

0

2.360E+05 2.360E+05 NUBASE

3422 88-Ra-231 2.5+ 1.717 m 2.91

β-:100.00

0

8.267E+05 8.267E+05 NUBASE

3423 88-Ra-232 0.0+ 4.167 m 20

β-:100.00

0

5.000E+05 5.000E+05 NUBASE

3424 88-Ra-233 0.5+ 30 s 16.67

β-:100.00

0

1.090E+06 1.090E+06 NUBASE

3425 88-Ra-234 0.0+ 30 s 33.33

β-:100.00

0

7.100E+05 7.100E+05 NUBASE

3426 89-Ac-206 3.0+ 0.025 s 28

α:99.80; β+:0.20

0

6.630E+03 6.630E+03 7.929E+06 NUBASE

3427 89-Ac-206M ? 8.000E+04 0.015 s 40

α:100.00

0

8.025E+06 NUBASE

3428 89-Ac-206N 10.0- 2.800E+05 0.041 s 39.02

α m:100.00

0

7.895E+06 NUBASE

3429 89-Ac-207 4.5- 0.022 s 181.82

α:100.00

1

7.864E+06 ENSDF

3430 89-Ac-208 3.0+ 0.095 s 25.26

α:99.00

1

7.644E+06 ENSDF

3431 89-Ac-208M 10.0- 5.100E+05 0.028 s 25

α n:89.00; IT:10.00;

β+:1.00

0

3.185E+04 8.285E+04 7.037E+06 NUBASE

3432 89-Ac-209 4.5- 0.1 s 50

α:99.00

1

7.656E+06 ENSDF

3433 89-Ac-210 7.0+ 0.35 s 14.29

α m:91.00; β+:9.00

0

2.499E+05 2.499E+05 6.750E+06 NUBASE

3434 89-Ac-211 4.5- 0.25 s 20

α:100.00

1

7.625E+06 ENSDF

3435 89-Ac-212 6.0+ 0.92 s 5.43

α:97.00; β+:3.00

0

7.471E+04 7.471E+04 7.299E+06 NUBASE

3436 89-Ac-213 4.5- 0.8 s 6.25

α:100.00

1

7.505E+06 ENSDF

3437 89-Ac-214 5.0+ 8.2 s 2.44

α:89.00; β+:11.00

0

2.320E+05 2.320E+05 6.542E+06 NUBASE

3438 89-Ac-215 4.5- 0.17 s 5.88

α:99.91

1

7.742E+06 ENSDF

3439 89-Ac-216 1.0- 3.3E-04 s 100

α:100.00

1

9.236E+06 ENSDF

3440 89-Ac-216M 9.0- 3.700E+04 3.3E-04 s 6.06

α:100.00

1

9.204E+06 ENSDF

3441 89-Ac-217 4.5- 6.9E-08 s 5.80

α:100.00

1

9.832E+06 ENSDF

3442 89-Ac-218 1.0- 1.08E-06 s 8.33

α:100.00

1

9.378E+06 ENSDF

3443 89-Ac-219 4.5- 1.18E-05 s 12.71

α:100.00

1

8.826E+06 ENSDF

3444 89-Ac-220 3.0- 0.026 s 0.76

α:100.00

4

1.140E+05 1.295E+05 7.960E+06 ENSDF

3445 89-Ac-221 4.5- 0.052 s 3.85

α:100.00

1

7.737E+06 ENSDF

3446 89-Ac-222 1.0- 5 s 10

α:99.00; β+:1.00

0

7.667E+03 7.667E+03 7.066E+06 NUBASE

3447 89-Ac-222M ? 2.000E+05 1.05 m 6.67

α:44.30; α m:44.30;

IT:10.00; β+:1.40

0

1.167E+04 3.167E+04 6.463E+06 NUBASE

3448 89-Ac-223 2.5- 2.1 m 2.38

α:99.00; β+:1.00

0

2.957E+02 5.913E+02 6.715E+06 NUBASE

3449 89-Ac-224 0.0- 2.78 h 6.12

α:9.10; β+:90.90

5

3.994E+04 2.310E+05 5.628E+05 ENSDF

3450 89-Ac-225 1.5- 10 d 1

α:100.00

4

2.761E+04 1.715E+04 5.868E+06 UKHEDD25

3451 89-Ac-226 1.0- 1.224 d 0.41

β-:83.00; β+:17.00;

α:0.01

0

3.134E+05 3.188E+05 3.321E+02 NUBASE

3452 89-Ac-227 1.5- 21.773 y 0.01

β-:98.62; α:1.38

5

1.481E+04 5.624E+02 6.933E+04 UKHEDD25

3453 89-Ac-228 3.0+ 6.15 h 0.33

β-:100.00

4

4.402E+05 9.632E+05 UKHEDD25

3454 89-Ac-229 1.5+ 1.045 h 0.80

β-:50.00; β-

m:50.00

0

3.878E+05 3.878E+05 NUBASE

3455 89-Ac-230 1.0+ 2.033 m 2.46

β-:100.00

4

9.098E+05 5.011E+05 ENSDF

3456 89-Ac-231 0.5+ 7.5 m 1.33

β-:100.00

4

6.289E+05 4.168E+05 ENSDF

3457 89-Ac-232 1.0+ 1.983 m 4.20

β-:100.00

4

9.840E+05 1.148E+06 ENSDF

3458 89-Ac-233 0.5+ 2.417 m 6.90

β-:100.00

4

9.207E+05 4.986E+05 ENSDF

3459 89-Ac-234 ? 44 s 15.91

β-:100.00

0

1.495E+06 1.495E+06 NUBASE

3460 89-Ac-235 0.5+ 40 s 100

β-:100.00

0

1.153E+06 1.153E+06 NUBASE

136 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 137: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3461 89-Ac-236 ? 2 m 100

β-:100.00

0

1.687E+06 1.687E+06 NUBASE

3462 90-Th-209 2.5- 7E-03 s 71.43

α:50.00; β+:50.00

0

1.277E+06 1.277E+06 4.118E+06 NUBASE

3463 90-Th-210 0.0+ 9E-03 s 188.89

α:100.00

1

8.053E+06 ENSDF

3464 90-Th-211 2.5- 0.048 s 41.67

α:99.50; β+:0.50

0

1.118E+04 1.118E+04 7.905E+06 NUBASE

3465 90-Th-212 0.0+ 0.036 s 41.67

α:99.70; β+:0.30

0

4.811E+03 4.811E+03 7.928E+06 NUBASE

3466 90-Th-213 2.5- 0.14 s 17.86

α:100.00

1

7.840E+06 ENSDF

3467 90-Th-214 0.0+ 0.1 s 25

α:99.90; β+:0.10

0

1.428E+03 1.428E+03 7.818E+06 NUBASE

3468 90-Th-215 0.5- 1.2 s 16.67

α:100.00

0

7.666E+06 NUBASE

3469 90-Th-216 0.0+ 0.027 s 1.12

α:99.99; β+:0.01

0

4.362E+01 4.362E+01 8.070E+06 NUBASE

3470 90-Th-217 4.5+ 2.52E-04 s 2.78

α:100.00

1

9.424E+06 ENSDF

3471 90-Th-218 0.0+ 1.09E-07 s 11.93

α:100.00

1

9.847E+06 ENSDF

3472 90-Th-219 4.5+ 1.05E-06 s 2.86

α:100.00

1

9.514E+06 ENSDF

3473 90-Th-220 0.0+ 9.7E-06 s 6.19

α:100.00; β+:~

0

9.170E-05 1.834E-04 8.953E+06 NUBASE

3474 90-Th-221 3.5+ 1.68E-03 s 3.57

α:100.00

0

8.626E+06 NUBASE

3475 90-Th-222 0.0+ 2.8E-03 s 10.71

α:100.00

1

8.117E+06 ENSDF

3476 90-Th-223 2.5+ 0.6 s 3.33

α:100.00

4

4.989E+04 7.368E+04 7.451E+06 ENSDF

3477 90-Th-224 0.0+ 1.05 s 1.90

α:100.00

4

1.214E+04 2.306E+04 7.225E+06 ENSDF

3478 90-Th-225 1.5+ 8.72 m 0.46

α:90.00; β+:10.00

0

3.360E+03 6.720E+03 6.229E+06 NUBASE

3479 90-Th-226 0.0+ 30.57 m 0.33

α:100.00

4

1.986E+04 8.630E+03 6.420E+06 ENSDF

3480 90-Th-227 0.5+ 18.718 d 0.03

α:100.00

4

4.451E+04 1.197E+05 6.007E+06 LNHB

3481 90-Th-228 0.0+ 1.913 y 0.03

α:100.00

4

2.048E+04 3.077E+03 5.498E+06 UKHEDD25

3482 90-Th-229 2.5+ 7340.164 y 2.18

α:100.00

4

1.159E+05 9.031E+04 4.947E+06 UKHEDD25

3483 90-Th-229M 1.5+ 3.500E+00 2.917 d 71.43

IT:100.00

0

3.500E+00 NUBASE

3484 90-Th-230 0.0+ 7.54E+04 y 0.40

α:100.00; SF:~

6

1.240E+04 1.277E+03 4.747E+06 UKHEDD25

3485 90-Th-231 2.5+ 1.063 d 0.04

β-:100.00

4

1.649E+05 2.582E+04 UKHEDD25

3486 90-Th-232 0.0+ 1.405E+10 y 0.43

α:100.00; SF:~

6

1.303E+04 1.243E+03 4.077E+06 UKHEDD25

3487 90-Th-233 1.5+ 22.3 m 0.45

β-:100.00

4

4.122E+05 3.749E+04 UKHEDD25

3488 90-Th-234 0.0+ 24.09 d 0.12

β-m:100.00

4

6.056E+04 8.801E+03 UKHEDD25

3489 90-Th-235 2.5+ 6.9 m 2.90

β-:100.00

0

6.400E+05 6.400E+05 UKHEDD25

3490 90-Th-236 0.0+ 37.5 m 0.53

β-:100.00

0

3.667E+05 3.667E+05 NUBASE

3491 90-Th-237 2.5+ 4.8 m 10.42

β-:100.00

0

8.533E+05 8.533E+05 NUBASE

3492 90-Th-238 0.0+ 9.4 m 21.28

β-:100.00

0

6.200E+05 6.200E+05 NUBASE

3493 91-Pa-212 7.0+ 8E-03 s 62.50

α:50.00; α m:50.00

0

8.170E+06 NUBASE

3494 91-Pa-213 4.5- 7E-03 s 42.86

α:100.00

0

8.395E+06 NUBASE

3495 91-Pa-214 ? 0.017 s 17.65

α:100.00

0

8.275E+06 NUBASE

3496 91-Pa-215 4.5- 0.014 s 14.29

α:100.00

0

8.245E+06 NUBASE

3497 91-Pa-216 ? 0.105 s 11.43

α:98.00; β+:2.00

0

4.997E+04 4.997E+04 7.933E+06 NUBASE

3498 91-Pa-217 4.5- 4.9E-03 s 12.24

α:100.00

1

8.497E+06 ENSDF

3499 91-Pa-217M 14.5+ 1.854E+06 1.6E-03 s 62.50

α:100.00

1

1.035E+07 ENSDF

3500 91-Pa-218 ? 1.2E-04 s 33.33

α:100.00

1

9.766E+06 ENSDF

3501 91-Pa-219 4.5- 5.3E-08 s 18.87

α:100.00

1

1.008E+07 ENSDF

3502 91-Pa-220 1.0- 7.8E-07 s 20.51

α:100.00; β+:~

0

5.711E-03 5.711E-03 9.832E+06 NUBASE

3503 91-Pa-221 4.5- 5.9E-06 s 28.81

α:100.00

0

9.248E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 137

MAIN DATA TABLES

Page 138: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3504 91-Pa-222 ? 3.2E-03 s 9.37

α:100.00

0

8.855E+06 NUBASE

3505 91-Pa-223 4.5- 5.1E-03 s 11.76

α:100.00

1

8.251E+06 ENSDF

3506 91-Pa-224 5.0- 0.844 s 2.25

α:99.90; β+:0.10

0

1.291E+03 1.291E+03 7.685E+06 NUBASE

3507 91-Pa-225 2.5- 1.7 s 5.88

α:100.00

1

7.361E+06 ENSDF

3508 91-Pa-226 ? 1.8 m 11.11

α:37.00; α m:37.00;

β+:26.00

0

2.458E+05 2.458E+05 5.096E+06 NUBASE

3509 91-Pa-227 2.5- 38.3 m 0.78

α:85.00; β+:15.00

0

7.694E+03 1.539E+04 5.594E+06 NUBASE

3510 91-Pa-228 3.0+ 22 h 4.55

α:2.00; β+:98.15

5

9.409E+04 1.332E+06 1.217E+05 ENSDF

3511 91-Pa-229 2.5+ 1.5 d 3.33

α:0.48; β+:99.52

5

6.586E+03 6.487E+04 2.644E+04 ENSDF

3512 91-Pa-230 2.0- 17.4 d 2.87

β+:91.60; β-:8.40;

α:~

0

4.160E+05 4.160E+05 1.741E+02 NUBASE

3513 91-Pa-231 1.5- 3.276E+04 y 0.34

α:100.00; SF:~

6

5.230E+04 3.873E+04 5.061E+06 UKHEDD25

3514 91-Pa-232 2.0- 1.31 d 1.53

β-:100.00; β+:~

5

1.682E+05 9.364E+05 UKHEDD25

3515 91-Pa-233 1.5- 27 d 0.37

β-:100.00

4

1.922E+05 2.205E+05 LNHB

3516 91-Pa-234 4.0+ 6.78 h 0.44

β-:100.00

4

3.859E+05 1.435E+06 UKHEDD25

3517 91-Pa-234M 0.0- 7.900E+04 1.17 m 2.56

β-:99.85; IT:0.15

4

8.165E+05 1.974E+04 UKHEDD25

3518 91-Pa-235 1.5- 24.2 m 1.24

β-m:100.00

4

4.641E+05 9.868E+03 UKHEDD25

3519 91-Pa-236 1.0- 9.1 m 1.10

β-:100.00

4

8.643E+05 8.057E+05 ENSDF

3520 91-Pa-237 0.5+ 8.7 m 2.30

β-:100.00

4

5.714E+05 6.079E+05 ENSDF

3521 91-Pa-238 3.0- 2.27 m 3.96

β-:100.00; β-,SF:~

0

1.154E+06 1.154E+06 NUBASE

3522 91-Pa-239 ? 1.8 h 27.78

β-:100.00

0

9.220E+05 9.220E+05 NUBASE

3523 91-Pa-240 ? 2 m 100

β-:100.00

0

1.362E+06 1.362E+06 NUBASE

3524 92-U -217 0.5- 0.026 s 53.85

α:100.00

0

8.155E+06 NUBASE

3525 92-U -218 0.0+ 6E-03 s 83.33

α:100.00

0

8.783E+06 NUBASE

3526 92-U -219 4.5+ 4.2E-05 s 80.95

α:100.00

1

9.861E+06 ENSDF

3527 92-U -220 0.0+ 6E-08 s 100

α:50.00; β+:50.00

0

4.417E+05 4.417E+05 5.151E+06 NUBASE

3528 92-U -221 4.5+ 7E-07 s 100

α:50.00; β+:50.00

0

7.017E+05 7.017E+05 4.975E+06 NUBASE

3529 92-U -222 0.0+ 1.4E-06 s 50

α:100.00; β+:~

0

7.267E-03 7.267E-03 9.501E+06 NUBASE

3530 92-U -223 3.5+ 1.8E-05 s 55.56

α:100.00

1

8.941E+06 ENSDF

3531 92-U -224 0.0+ 9.4E-04 s 28.72

α:100.00; β+:~

0

7.376E-01 7.376E-01 8.620E+06 NUBASE

3532 92-U -225 2.5+ 0.061 s 6.56

α:100.00

0

8.014E+06 NUBASE

3533 92-U -226 0.0+ 0.35 s 42.86

α:100.00

1

7.684E+06 ENSDF

3534 92-U -227 1.5+ 1.1 m 9.09

α:100.00

4

7.539E+04 1.155E+05 7.011E+06 ENSDF

3535 92-U -228 0.0+ 9.1 m 2.20

α:95.00; β+:5.00

0

7.525E+02 1.505E+03 6.464E+06 NUBASE

3536 92-U -229 1.5+ 58 m 5.17

β+:80.00; α:20.00

0

3.501E+05 3.501E+05 1.295E+06 NUBASE

3537 92-U -230 0.0+ 20.8 d 10.10

α:100.00

4

1.942E+04 2.681E+03 5.971E+06 ENSDF

3538 92-U -231 2.5+ 4.2 d 2.38

β+:100.00; α:~

0

1.906E+04 3.813E+04 2.230E+02 NUBASE

3539 92-U -232 0.0+ 69.801 y 0.72

α:100.00; SF:~

6

1.684E+04 1.685E+03 5.397E+06 UKHEDD25

3540 92-U -233 2.5+ 1.593E+05 y 0.13

α:100.00

4

7.597E+03 1.225E+03 4.904E+06 UKHEDD25

3541 92-U -234 0.0+ 2.457E+05 y 0.12

α:100.00; SF:~

6

1.414E+04 1.450E+03 4.842E+06 UKHEDD25

3542 92-U -235 3.5- 7.038E+08 y 0.07

α:100.00; SF:~

6

5.067E+04 1.636E+05 4.465E+06 UKHEDD25

3543 92-U -235M 0.5+ 7.680E+01 26 m 7.69

IT:100.00

2

7.680E+01 1.920E-10 UKHEDD25

3544 92-U -236 0.0+ 2.37E+07 y 0.84

α:100.00; SF:~

6

1.106E+04 1.202E+03 4.572E+06 UKHEDD25

138 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 139: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3545 92-U -237 0.5+ 6.75 d 0.15

β-:100.00

4

1.997E+05 1.434E+05 UKHEDD25

3546 92-U -238 0.0+ 4.468E+09 y 0.07

α:100.00; SF:~

6

1.021E+04 1.100E+03 4.259E+06 UKHEDD25

3547 92-U -239 2.5+ 23.47 m 0.21

β-:100.00

4

4.099E+05 5.157E+04 UKHEDD25

3548 92-U -240 0.0+ 14.1 h 1.42

β-:100.00

4

1.454E+05 9.258E+03 UKHEDD25

3549 92-U -241 3.5+ 5 m 100

β-:100.00

0

6.467E+05 6.467E+05 NUBASE

3550 92-U -242 0.0+ 16.8 m 2.98

β-:100.00

3

3.883E+05 3.641E+04 ENSDF

3551 93-Np-225 4.5- 3E-03 s 100

α:100.00

0

8.785E+06 NUBASE

3552 93-Np-226 ? 0.035 s 28.57

α:100.00

1

8.175E+06 ENSDF

3553 93-Np-227 2.5- 0.51 s 11.76

α:99.95; β+:0.05

0

5.897E+02 5.897E+02 7.811E+06 NUBASE

3554 93-Np-228 ? 1.023 m 2.28

β+:59.99; α:40.00;

β+,SF:0.01

0

8.948E+05 8.948E+05 2.962E+06 NUBASE

3555 93-Np-229 2.5+ 4 m 5

α:50.00; β+:50.00

0

4.282E+05 4.282E+05 3.508E+06 NUBASE

3556 93-Np-230 ? 4.6 m 6.52

β+:97.00; α:3.00

0

1.172E+06 1.172E+06 2.035E+05 NUBASE

3557 93-Np-231 2.5+ 48.8 m 0.41

β+:98.00; α:2.00

0

5.955E+05 5.955E+05 1.275E+05 NUBASE

3558 93-Np-232 4.0+ 14.7 m 2.04

β+:100.00

4

8.314E+04 1.178E+06 ENSDF

3559 93-Np-233 2.5+ 36.2 m 0.28

α:~; β+:100.00

5

4.596E+03 8.856E+04 5.602E+01 ENSDF

3560 93-Np-234 0.0+ 4.4 d 2.27

β+:100.00

4

4.033E+04 1.107E+06 ENSDF

3561 93-Np-235 2.5+ 1.084 y 0.28

β+:100.00; α:~

5

3.300E+03 7.999E+03 6.985E+01 LNHB

3562 93-Np-236 6.0- 1.52E+05 y 1.97

β-:11.80; β+:88.04;

α:0.16

6

2.396E+05 1.530E+05 8.109E+03 UKHEDD25

3563 93-Np-236M 1.0- 5.000E+00 22.5 h 1.33

β-:50.00; β+:50.00

5

9.141E+04 4.913E+04 UKHEDD25

3564 93-Np-237 2.5+ 2.14E+06 y 0.47

α:100.00

4

3.831E+04 3.240E+04 4.860E+06 LNHB

3565 93-Np-238 2.0+ 2.117 d 0.09

β-:100.00

4

2.325E+05 6.443E+05 UKHEDD25

3566 93-Np-239 2.5+ 2.355 d 0.17

β-:100.00

4

2.628E+05 1.822E+05 UKHEDD25

3567 93-Np-240 5.0+ 1.083 h 4.62

β-:100.00

4

4.668E+05 1.247E+06 UKHEDD25

3568 93-Np-240M 1.0- 2.000E+04 7.4 m 2.70

β-:99.89; IT:0.11

4

6.830E+05 3.368E+05 UKHEDD25

3569 93-Np-241 2.5+ 13.9 m 1.44

β-:100.00

4

4.372E+05 3.609E+04 UKHEDD25

3570 93-Np-242 1.0+ 2.2 m 9.09

β-:100.00

2

8.887E+05 2.432E+05 ENSDF

3571 93-Np-242M 6.0+ 5.5 m 1.82

β-:100.00

0

9.005E+05 9.005E+05 NUBASE

3572 93-Np-243 2.5- 1.85 m 8.11

β-:100.00

0

7.080E+05 7.080E+05 NUBASE

3573 93-Np-244 7.0- 2.29 m 6.99

β-:100.00

0

1.131E+06 1.131E+06 NUBASE

3574 94-Pu-228 0.0+ 0.01 s 100

α:99.90; β+:0.10

0

7.967E+02 7.967E+02 7.943E+06 NUBASE

3575 94-Pu-229 1.5+ 2 m 41.67

α:100.00

0

7.598E+06 NUBASE

3576 94-Pu-230 0.0+ 1.7 m 10

α:50.00; β+:50.00

0

2.823E+05 2.823E+05 3.590E+06 NUBASE

3577 94-Pu-231 1.5+ 8.6 m 5.81

β+:87.00; α:13.00

0

7.700E+05 7.700E+05 8.890E+05 NUBASE

3578 94-Pu-232 0.0+ 33.7 m 1.48

β+:89.00; α:11.00

0

4.477E+04 8.953E+04 7.388E+05 NUBASE

3579 94-Pu-233 2.5+ 20.9 m 1.91

β+:99.88; α:0.12

0

6.992E+05 6.992E+05 7.697E+03 NUBASE

3580 94-Pu-234 0.0+ 8.8 h 1.14

β+:94.00; α:6.00

0

1.852E+04 3.704E+04 3.786E+05 NUBASE

3581 94-Pu-235 2.5+ 25.3 m 1.98

β+:100.00; α:~

0

3.798E+05 3.798E+05 1.667E+02 NUBASE

3582 94-Pu-236 0.0+ 2.858 y 0.21

α:100.00; SF:~

6

1.339E+04 1.583E+03 5.852E+06 UKHEDD25

3583 94-Pu-237 3.5- 45.3 d 0.44

β+:100.00; α:~

5

1.750E+04 5.516E+04 2.341E+02 UKHEDD25

3584 94-Pu-237M 0.5+ 1.455E+05 0.18 s 11.11

IT:100.00

0

1.455E+05 NUBASE

3585 94-Pu-238 0.0+ 87.7 y 0.34

α:100.00; SF:~

6

1.119E+04 1.548E+03 5.580E+06 UKHEDD25

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 139

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Page 140: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3586 94-Pu-239 0.5+ 2.411E+04 y 0.05

α:0.06; α m:99.94;

SF:~

6

7.935E+03 7.277E+02 5.238E+06 UKHEDD25

3587 94-Pu-240 0.0+ 6562.997 y 0.08

α:100.00; SF:~

6

1.112E+04 1.363E+03 5.243E+06 UKHEDD25

3588 94-Pu-241 2.5+ 14.33 y 0.28

β-:100.00; α:~

5

5.235E+03 1.711E+00 1.226E+02 UKHEDD25

3589 94-Pu-242 0.0+ 3.735E+05 y 0.29

α:100.00; SF:~

6

9.381E+03 1.291E+03 4.973E+06 UKHEDD25

3590 94-Pu-243 3.5+ 4.956 h 0.06

β-:100.00

4

1.736E+05 2.508E+04 UKHEDD25

3591 94-Pu-244 0.0+ 8E+07 y 1.12

α:99.88; SF:0.12

6

7.715E+03 9.756E+03 4.873E+06 UKHEDD25

3592 94-Pu-245 4.5- 10.5 h 0.95

β-:100.00

4

3.314E+05 3.986E+05 UKHEDD25

3593 94-Pu-246 0.0+ 10.85 d 0.18

β-m:100.00

4

1.149E+05 1.238E+05 UKHEDD25

3594 94-Pu-247 0.5+ 2.27 d 10.13

β-:100.00

0

6.167E+05 6.167E+05 NUBASE

3595 95-Am-231 ? 30 s 100

β+:50.00; α:50.00

0

6.925E+05 6.925E+05 3.728E+06 NUBASE

3596 95-Am-232 ? 1.31 m 3.05

β+:97.93; α:2.00;

β+,SF:0.07

0

1.643E+06 1.643E+06 1.455E+05 NUBASE

3597 95-Am-233 ? 3.2 m 25

β+:97.00; α:3.00

0

1.009E+06 1.009E+06 2.090E+05 NUBASE

3598 95-Am-234 ? 2.32 m 3.45

β+:99.95; α:0.04;

β+,SF:0.01

0

1.393E+06 1.393E+06 2.677E+03 NUBASE

3599 95-Am-235 2.5- 9.9 m 5.05

β+:99.60; α:0.40

0

8.220E+05 8.220E+05 2.642E+04 NUBASE

3600 95-Am-236 ? 30 m 100

β+:50.00; α:50.00

0

5.462E+05 5.462E+05 3.198E+06 NUBASE

3601 95-Am-237 2.5- 1.217 h 1.37

β+:49.99; β+

m:49.99;

α:0.03

0

4.679E+05 4.679E+05 1.549E+03 NUBASE

3602 95-Am-238 1.0+ 1.633 h 2.04

β+:100.00

4

1.545E+04 8.877E+05 ENSDF

3603 95-Am-239 2.5- 11.9 h 0.84

β+:99.99; α:0.01

0

4.010E+04 8.020E+04 5.922E+02 NUBASE

3604 95-Am-240 3.0- 2.117 d 0.59

β+:100.00; α:~

5

8.295E+04 1.031E+06 1.038E+01 UKHEDD25

3605 95-Am-241 2.5- 432.808 y 0.16

α:100.00; SF:~

6

3.908E+04 2.751E+04 5.557E+06 UKHEDD25

3606 95-Am-242 1.0- 16.04 h 0.19

β-:83.20; β+:16.80

5

1.827E+05 1.670E+04 UKHEDD25

3607 95-Am-242M 5.0- 4.863E+04 141.003 y 1.42

IT:99.54; α:0.46;

SF:~

6

4.595E+04 4.183E+03 2.478E+04 UKHEDD25

3608 95-Am-242N ? 2.200E+06 0.014 s 7.14

SF:100.00

0

NUBASE

3609 95-Am-243 2.5- 7364.976 y 0.30

α:100.00; SF:~

6

2.393E+04 5.696E+04 5.359E+06 UKHEDD25

3610 95-Am-244 6.0- 10.1 h 0.99

β-:100.00

4

3.081E+05 8.434E+05 UKHEDD25

3611 95-Am-244M 1.0- 6.900E+04 26 m 7.69

β-:99.96; β+:0.04

5

5.039E+05 1.244E+04 UKHEDD25

3612 95-Am-245 2.5+ 2.05 h 0.49

β-:100.00

4

2.847E+05 2.774E+04 UKHEDD25

3613 95-Am-246 7.0+ 39 m 7.69

β-:100.00

4

7.153E+05 7.752E+05 UKHEDD25

3614 95-Am-246M 2.0+ 5.000E+03 25 m 0.80

β-:100.00

4

4.846E+05 1.016E+06 UKHEDD25

3615 95-Am-247 2.5+ 23 m 5.65

β-:100.00

4

5.873E+05 1.345E+05 ENSDF

3616 95-Am-248 ? 3 m 100

β-:100.00

0

1.056E+06 1.056E+06 NUBASE

3617 95-Am-249 ? 1 m 100

β-:100.00

0

7.833E+05 7.833E+05 NUBASE

3618 96-Cm-233 1.5+ 1 m 100

α:50.00; β+:50.00

0

6.867E+05 6.867E+05 3.733E+06 NUBASE

3619 96-Cm-234 0.0+ 51 s 23.53

α:50.00; β+:47.00;

SF:3.00

0

3.437E+05 3.437E+05 3.683E+06 NUBASE

3620 96-Cm-235 2.5+ 5 m 100

β+:50.00; α:50.00

0

5.417E+05 5.417E+05 3.600E+06 NUBASE

3621 96-Cm-236 0.0+ 10 m 100

β+:50.00; α:50.00

0

2.850E+05 2.850E+05 3.550E+06 NUBASE

3622 96-Cm-237 2.5+ 20 m 100

β+:50.00; α:50.00

0

4.517E+05 4.517E+05 3.403E+06 NUBASE

140 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 141: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3623 96-Cm-238 0.0+ 2.4 h 4.17

β+:90.00; α:10.00

0

4.410E+04 8.820E+04 6.625E+05 NUBASE

3624 96-Cm-239 3.5- 2.9 h 100

β+:99.90; α:0.10

0

5.987E+05 5.987E+05 6.581E+03 NUBASE

3625 96-Cm-240 0.0+ 27 d 3.70

α:99.70

1

6.370E+06 ENSDF

3626 96-Cm-241 0.5+ 32.8 d 0.61

β+:99.00; α:1.00

5

1.408E+05 4.968E+05 6.029E+04 UKHEDD25

3627 96-Cm-242 0.0+ 162.931 d 0.04

α:100.00; SF:~

6

1.017E+04 1.373E+03 6.206E+06 UKHEDD25

3628 96-Cm-243 2.5+ 30.001 y 6.67

β+:0.24; α:99.76

5

1.392E+05 1.332E+05 5.940E+06 UKHEDD25

3629 96-Cm-244 0.0+ 18 y 0.56

α:100.00; SF:~

6

8.874E+03 1.211E+03 5.894E+06 UKHEDD25

3630 96-Cm-244M 6.0+ 1.040E+06 0.034 s 5.88

IT:100.00

0

1.040E+06 NUBASE

3631 96-Cm-245 3.5+ 8500.194 y 2.35

α:100.00

4

8.129E+04 9.380E+04 5.448E+06 UKHEDD25

3632 96-Cm-246 0.0+ 4730.087 y 3.17

α:99.97; SF:0.03

6

8.200E+03 3.002E+03 5.514E+06 UKHEDD25

3633 96-Cm-247 4.5- 1.6E+07 y 3.12

α:100.00

4

2.239E+04 3.028E+05 5.028E+06 UKHEDD25

3634 96-Cm-248 0.0+ 3.4E+05 y 1.18

α:91.74; SF:8.26

6

6.291E+03 5.791E+05 1.981E+07 UKHEDD25

3635 96-Cm-249 0.5+ 1.069 h 0.05

β-:100.00

4

2.837E+05 1.968E+04 UKHEDD25

3636 96-Cm-250 0.0+ 8000.177 y 50

α:30.00; SF:70.00

4

4.900E+06 1.296E+08 UKHEDD25

3637 96-Cm-251 0.5+ 16.8 m 1.19

β-:100.00

4

4.507E+05 1.104E+05 ENSDF

3638 96-Cm-252 0.0+ 1 d 100

β-:100.00

0

1.767E+05 1.767E+05 NUBASE

3639 97-Bk-235 ? 20 s 100

β+:50.00; α:50.00

0

7.983E+05 7.983E+05 3.918E+06 NUBASE

3640 97-Bk-236 ? 1 m 100

β+:50.00; α:50.00

0

9.183E+05 9.183E+05 3.788E+06 NUBASE

3641 97-Bk-237 3.5+ 1 m 100

β+:50.00; α:50.00

0

6.367E+05 6.367E+05 3.753E+06 NUBASE

3642 97-Bk-238 ? 2.4 m 4.17

β+:99.75; α:0.20;

β+,SF:0.05

0

1.626E+06 1.626E+06 1.467E+04 NUBASE

3643 97-Bk-239 3.5+ 3 m 100

β+:50.00; α:50.00

0

5.167E+05 5.167E+05 3.603E+06 NUBASE

3644 97-Bk-240 ? 4.8 m 16.67

β+:90.00; α:10.00;

β+,SF:~

0

1.183E+06 1.183E+06 7.065E+05 NUBASE

3645 97-Bk-241 3.5+ 4.6 m 8.70

α:50.00; β+:50.00

0

3.994E+05 3.994E+05 3.553E+06 NUBASE

3646 97-Bk-242 2.0- 7 m 18.57

β+:100.00; β+,SF:~

0

9.783E+05 9.783E+05 NUBASE

3647 97-Bk-243 1.5- 4.5 h 4.44

β+:99.85; α:0.15

0

5.017E+05 5.017E+05 1.031E+04 NUBASE

3648 97-Bk-244 4.0- 4.35 h 3.45

β+:99.99; α:0.01

0

7.541E+05 7.541E+05 4.067E+02 NUBASE

3649 97-Bk-245 1.5- 4.94 d 0.61

α:0.12; β+:99.88

5

1.190E+05 2.347E+05 7.460E+03 ENSDF

3650 97-Bk-246 2.0- 1.8 d 1.11

β+:99.90; α:0.05;

α n:0.05

0

4.501E+05 4.501E+05 4.975E+03 NUBASE

3651 97-Bk-247 1.5- 1380.001 y 18.12

α:100.00

4

6.583E+04 1.415E+05 5.657E+06 ENSDF

3652 97-Bk-248 6.0+ 9 y 100

α:100.00

0

5.774E+06 NUBASE

3653 97-Bk-248M 1.0- 3.000E+04 23.7 h 0.84

β+:30.00; β-:70.00

5

1.775E+05 5.338E+04 ENSDF

3654 97-Bk-249 3.5+ 320 d 1.88

β-:100.00; α:~;

SF:~

7

3.304E+04 3.147E+01 7.902E+01 UKHEDD25

3655 97-Bk-250 2.0- 3.217 h 0.16

β-:100.00

4

2.970E+05 9.054E+05 UKHEDD25

3656 97-Bk-251 1.5- 55.6 m 1.98

β-:100.00

0

3.643E+05 3.643E+05 NUBASE

3657 97-Bk-252 ? 1.8 m 27.78

β-:50.00; α:50.00

0

4.160E+05 4.160E+05 2.773E+06 NUBASE

3658 97-Bk-253 ? 10 m 100

β-:100.00

0

5.430E+05 5.430E+05 NUBASE

3659 97-Bk-254 ? 1 m 100

β-:100.00

0

1.016E+06 1.016E+06 NUBASE

3660 98-Cf-237 2.5+ 2.1 s 14.29

α:45.00; SF:10.00;

β+:45.00

0

7.080E+05 7.080E+05 3.647E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 141

MAIN DATA TABLES

Page 142: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3661 98-Cf-238 0.0+ 0.021 s 6.16

SF:99.80; α:0.20

0

1.607E+04 NUBASE

3662 98-Cf-239 2.5+ 1 m 50

α:50.00; β+:50.00

0

6.433E+05 6.433E+05 3.908E+06 NUBASE

3663 98-Cf-240 0.0+ 57.6 s 15.62

α:98.00; SF:2.00

0

7.561E+06 NUBASE

3664 98-Cf-241 3.5- 3.8 m 18.42

β+:75.00; α:25.00

0

8.150E+05 8.150E+05 1.914E+06 NUBASE

3665 98-Cf-242 0.0+ 3.49 m 3.44

α:80.00; β+:19.99;

SF:0.01

0

1.066E+05 1.066E+05 6.012E+06 NUBASE

3666 98-Cf-243 0.5+ 10.7 m 4.67

β+:86.00; α:14.00

0

6.476E+05 6.476E+05 1.027E+06 NUBASE

3667 98-Cf-244 0.0+ 19.4 m 3.09

α:100.00

0

7.329E+06 NUBASE

3668 98-Cf-245 2.5+ 45 m 3.33

β+:64.00; α:36.00

0

3.353E+05 3.353E+05 2.613E+06 NUBASE

3669 98-Cf-246 0.0+ 1.488 d 1.40

α:100.00

4

3.977E+03 1.190E+03 6.857E+06 ENSDF

3670 98-Cf-247 3.5+ 3.11 h 0.96

β+:99.97; α:0.03

0

3.229E+04 6.458E+04 2.285E+03 NUBASE

3671 98-Cf-248 0.0+ 333.5 d 0.84

α:100.00

3

5.053E+03 2.696E+01 6.352E+06 ENSDF

3672 98-Cf-249 4.5- 351.007 y 0.57

α:100.00; SF:~

6

2.985E+04 3.292E+05 5.928E+06 UKHEDD25

3673 98-Cf-250 0.0+ 13.08 y 0.69

α:99.92; SF:0.08

6

5.958E+03 6.343E+03 6.262E+06 UKHEDD25

3674 98-Cf-251 0.5+ 898.018 y 4.90

α:100.00

4

1.817E+05 1.203E+05 5.878E+06 UKHEDD25

3675 98-Cf-252 0.0+ 2.645 y 0.30

α:96.91; SF:3.09

6

6.006E+03 2.174E+05 1.181E+07 UKHEDD25

3676 98-Cf-253 3.5+ 17.81 d 0.45

β-:99.69; α:0.31

5

8.046E+04 8.369E+01 1.882E+04 UKHEDD25

3677 98-Cf-254 0.0+ 60.5 d 0.33

SF:99.69; α:0.31

0

1.832E+04 NUBASE

3678 98-Cf-255 3.5+ 1.417 h 21.18

β-:100.00; SF:~;

α:~

0

2.403E+05 2.403E+05 1.147E-02 NUBASE

3679 98-Cf-256 0.0+ 12.3 m 9.76

SF:100.00; α:~

0

3.444E-02 NUBASE

3680 99-Es-240 ? 1 s 100

α:50.00; β+:50.00

0

1.028E+06 1.028E+06 4.188E+06 NUBASE

3681 99-Es-241 1.5- 10 s 50

α:50.00; β+:50.00

0

7.467E+05 7.467E+05 4.158E+06 NUBASE

3682 99-Es-242 ? 13.5 s 18.52

α:50.00; β+:49.40;

β+,SF:0.60

0

9.271E+05 9.271E+05 4.128E+06 NUBASE

3683 99-Es-243 1.5- 21 s 9.52

β+:70.00; α:30.00

0

8.937E+05 8.937E+05 2.420E+06 NUBASE

3684 99-Es-244 ? 37 s 10.81

β+:94.99; α:5.00;

β+,SF:0.01

0

1.441E+06 1.441E+06 3.968E+05 NUBASE

3685 99-Es-245 1.5- 1.1 m 9.09

β+:60.00; α:40.00

0

6.106E+05 6.106E+05 3.166E+06 NUBASE

3686 99-Es-246 4.0- 7.7 m 6.49

β+:90.10; α:9.90;

β+,SF:~

0

1.144E+06 1.144E+06 7.658E+05 NUBASE

3687 99-Es-247 3.5+ 4.6 m 6.52

β+:93.00; α:7.00;

SF:~

0

7.666E+05 7.666E+05 5.246E+05 NUBASE

3688 99-Es-248 ? 27 m 18.52

β+:99.75; α:0.25;

β+,SF:~

0

1.017E+06 1.017E+06 1.790E+04 NUBASE

3689 99-Es-249 3.5+ 1.703 h 0.59

α:0.57; β+:99.43

5

3.050E+04 4.119E+05 3.860E+04 ENSDF

3690 99-Es-250 6.0+ 8.6 h 1.16

β+:97.00; α:3.00

0

6.655E+05 6.655E+05 2.051E+05 NUBASE

3691 99-Es-250M 1.0- 2.000E+05 2.22 h 2.25

β+:100.00

4

2.035E+04 5.434E+05 ENSDF

3692 99-Es-251 1.5- 1.375 d 3.03

β+:99.50; α:0.50

0

1.876E+04 3.751E+04 3.298E+04 NUBASE

3693 99-Es-252 5.0- 1.291 y 0.40

α:78.00; β+:22.00

0

1.382E+04 2.763E+04 5.292E+06 NUBASE

3694 99-Es-253 3.5+ 20.47 d 0.15

α:100.00; SF:~

6

4.561E+03 1.075E+03 6.734E+06 UKHEDD25

3695 99-Es-254 7.0+ 275.7 d 0.18

α:100.00

4

1.199E+04 6.215E+04 6.503E+06 ENSDF

142 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 143: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3696 99-Es-254M 2.0+ 8.370E+04 1.637 d 0.51

β-:96.65; IT:2.96;

α:0.32; β+:0.07

0

3.774E+05 3.800E+05 2.114E+04 NUBASE

3697 99-Es-255 3.5+ 39.8 d 3.02

β-:92.00; α:8.00;

SF:~

0

8.893E+04 8.893E+04 5.149E+05 NUBASE

3698 99-Es-256 ? 25.4 m 9.45

β-:100.00

0

5.680E+05 5.680E+05 NUBASE

3699 99-Es-256M 8.0+ 7.6 h 100

β-:100.00; β-,SF:~

0

5.680E+05 5.680E+05 NUBASE

3700 99-Es-257 3.5+ 7.7 d 2.60

β-:100.00; α:~

0

2.703E+05 2.703E+05 2.418E+01 NUBASE

3701 99-Es-258 ? 3 m 100

β-:50.00; α:50.00

0

3.783E+05 3.783E+05 2.943E+06 NUBASE

3702 100-Fm-242 0.0+ 8E-04 s 25

SF:50.00; α:50.00

0

4.388E+06 NUBASE

3703 100-Fm-243 3.5- 0.21 s 28.57

α:60.00; β+:39.43;

SF:0.57

0

5.888E+05 5.888E+05 5.211E+06 NUBASE

3704 100-Fm-244 0.0+ 3.3E-03 s 15.15

SF:99.60; α:0.40

0

3.422E+04 NUBASE

3705 100-Fm-245 0.5+ 4.2 s 30.95

α:95.67; β+:4.20;

SF:0.13

0

5.292E+04 5.292E+04 8.070E+06 NUBASE

3706 100-Fm-246 0.0+ 1.1 s 18.18

α:85.50; SF:4.50;

β+,SF:10.00

0

7.161E+06 NUBASE

3707 100-Fm-247 2.5+ 35 s 11.43

α:50.00; β+:50.00

0

4.950E+05 4.950E+05 4.103E+06 NUBASE

3708 100-Fm-248 0.0+ 36 s 8.33

α:92.91; β+:6.99;

SF:0.10

0

3.744E+04 3.744E+04 7.434E+06 NUBASE

3709 100-Fm-249 3.5+ 2.6 m 26.92

β+:67.00; α:33.00

0

5.449E+05 5.449E+05 2.577E+06 NUBASE

3710 100-Fm-250 0.0+ 30 m 10

α:89.99; β+

m:10.00;

SF:0.01

0

3.220E+03 6.440E+03 6.801E+06 NUBASE

3711 100-Fm-250M ? 1.500E+06 1.8 s 5.56

IT:80.00; α:20.00;

SF:~

0

1.200E+06 1.811E+06 NUBASE

3712 100-Fm-251 4.5- 5.3 h 1.51

β+:98.20; α:1.80

0

4.828E+05 4.828E+05 1.337E+05 NUBASE

3713 100-Fm-252 0.0+ 1.058 d 0.20

α:100.00

3

4.208E+03 3.952E+01 7.144E+06 ENSDF

3714 100-Fm-253 0.5+ 3 d 4

β+:88.00; α:12.00

0

1.480E+04 2.959E+04 8.639E+05 NUBASE

3715 100-Fm-254 0.0+ 3.24 h 0.06

α:99.94

4

4.329E+03 1.397E+03 7.298E+06 ENSDF

3716 100-Fm-255 3.5+ 20.07 h 0.35

α:100.00

4

7.211E+04 1.145E+04 7.167E+06 ENSDF

3717 100-Fm-256 0.0+ 2.627 h 0.82

SF:91.90; α:8.10

0

5.692E+05 NUBASE

3718 100-Fm-257 4.5+ 100.5 d 0.20

α:99.79

4

1.157E+05 1.191E+05 6.660E+06 ENSDF

3719 100-Fm-258 0.0+ 3.7E-04 s 3.78

SF:100.00

0

NUBASE

3720 100-Fm-259 1.5+ 1.5 s 20

SF:100.00

0

NUBASE

3721 101-Md-245 0.5- 9E-04 s 27.78

SF:50.00; α:50.00

0

4.513E+06 NUBASE

3722 101-Md-245M 3.5+ 1.000E+05 0.4 s 50

α:50.00; β+:50.00

0

8.617E+05 8.617E+05 4.563E+06 NUBASE

3723 101-Md-246 ? 1 s 40

α:33.33; β+:33.33;

SF:33.33

0

6.822E+05 6.822E+05 2.962E+06 NUBASE

3724 101-Md-247 0.5- 0.27 s 59.26

SF:50.00; α:50.00

0

4.418E+06 NUBASE

3725 101-Md-247M 3.5+ 5.000E+04 1.12 s 19.64

α:100.00; SF:~

0

8.885E+06 NUBASE

3726 101-Md-248 ? 7 s 42.86

β+:79.95; α:20.00;

β+,SF:0.05

0

1.398E+06 1.398E+06 1.739E+06 NUBASE

3727 101-Md-249 3.5- 24 s 16.67

α:60.00; β+:40.00

0

4.947E+05 4.947E+05 5.079E+06 NUBASE

3728 101-Md-249M 0.5- 1.000E+05 1.9 s 47.37

α:100.00

0

8.565E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 143

MAIN DATA TABLES

Page 144: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3729 101-Md-250 ? 52 s 11.54

β+:46.49; β+

m:46.49;

α:7.00; β+,SF:0.02

0

1.183E+06 1.183E+06 5.821E+05 NUBASE

3730 101-Md-251 3.5- 4 m 12.50

β+:95.00; α:5.00

0

9.636E+05 9.636E+05 3.998E+05 NUBASE

3731 101-Md-252 ? 2.3 m 34.78

β+:50.00; α:50.00

0

6.355E+05 6.355E+05 3.953E+06 NUBASE

3732 101-Md-253 3.5- 12 m 66.67

β+:99.40; α:0.60

0

6.461E+05 6.461E+05 4.617E+04 NUBASE

3733 101-Md-254 0.0- 10 m 30

β+:100.00

0

8.686E+05 8.686E+05 NUBASE

3734 101-Md-254M 3.0- 5.000E+04 28 m 28.57

β+:100.00

0

8.853E+05 8.853E+05 NUBASE

3735 101-Md-255 3.5- 27 m 7.41

β+:91.86; α:7.99;

SF:0.15

0

3.197E+05 3.197E+05 6.315E+05 NUBASE

3736 101-Md-256 1.0- 1.283 h 2.60

β+:87.80; α:9.20;

SF:3.00

0

6.245E+05 6.245E+05 7.273E+05 NUBASE

3737 101-Md-257 3.5- 5.52 h 0.91

β+:81.73; α:14.42;

SF:3.85

0

1.664E+04 3.328E+04 1.090E+06 NUBASE

3738 101-Md-258 8.0- 51.5 d 0.58

α:100.00; β+:~;

β-:~

0

7.330E+00 7.330E+00 7.271E+06 NUBASE

3739 101-Md-258M 1.0- 57 m 1.58

β+:68.80; SF:20.00;

β-:10.00; α m:1.20

0

5.021E+04 9.348E+04 8.625E+04 NUBASE

3740 101-Md-259 3.5- 1.6 h 3.12

SF:98.70; α:1.30

0

9.238E+04 NUBASE

3741 101-Md-260 ? 27.8 d 2.88

SF:91.50; α:2.50;

α m:2.50; β-:3.50

0

1.097E+04 1.097E+04 3.468E+05 NUBASE

3742 101-Md-261 3.5- 40 m 100

α:100.00

0

6.655E+06 NUBASE

3743 102-No-249 2.5+ 5.7E-05 s 21.05

β+:25.00; β+

m:25.00;

α:50.00

0

7.400E+05 7.400E+05 4.588E+06 NUBASE

3744 102-No-250 0.0+ 5.7E-06 s 14.04

SF:99.90; α:0.10;

β+:~

0

2.400E+00 2.400E+00 8.955E+03 NUBASE

3745 102-No-251 3.5+ 0.8 s 37.50

α:100.00

1

8.745E+06 ENSDF

3746 102-No-251M 4.5- 1.100E+05 1.7 s 58.82

α:100.00

0

9.015E+06 NUBASE

3747 102-No-252 0.0+ 2.44 s 1.64

α:67.00; SF:32.20;

β+:0.80

0

6.003E+03 6.003E+03 5.729E+06 NUBASE

3748 102-No-253 4.5- 1.62 m 9.26

α:80.00; β+:20.00;

SF:~

0

2.113E+05 2.113E+05 6.740E+06 NUBASE

3749 102-No-254 0.0+ 51 s 19.61

α:89.85; β+:9.98;

SF:0.17

0

4.040E+04 4.040E+04 7.390E+06 NUBASE

3750 102-No-254M ? 5.000E+05 0.28 s 14.29

IT:80.00; α:10.00;

α m:10.00

0

4.000E+05 1.595E+06 NUBASE

3751 102-No-255 0.5+ 3.1 m 6.45

α:61.00; β+:39.00

0

2.614E+05 2.614E+05 5.150E+06 NUBASE

3752 102-No-256 0.0+ 2.91 s 1.72

α:99.50

1

8.533E+06 ENSDF

3753 102-No-257 3.5+ 25 s 8

α:100.00

1

8.383E+06 ENSDF

3754 102-No-258 0.0+ 1.2E-03 s 16.67

SF:100.00; α:~

0

8.151E+01 NUBASE

3755 102-No-259 4.5+ 58 m 8.62

α:68.18; β+:22.73;

SF:9.09

0

5.568E+03 1.114E+04 5.377E+06 NUBASE

3756 102-No-260 0.0+ 0.106 s 7.55

SF:100.00

0

NUBASE

3757 102-No-261 1.5+ 3 h 100

α:100.00

0

7.486E+06 NUBASE

3758 102-No-262 0.0+ 5E-03 s 100

SF:100.00

0

NUBASE

144 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 145: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3759 103-Lr-251 ? 1.5E-04 s 100

β+:25.00; β+

m:25.00;

α:25.00; α m:25.00

0

8.225E+05 8.225E+05 4.705E+06 NUBASE

3760 103-Lr-252 ? 0.39 s 23.08

β+:71.00; α:28.00;

SF:1.00

0

1.410E+06 1.410E+06 2.594E+06 NUBASE

3761 103-Lr-253 3.5- 0.58 s 12.07

α:96.15; SF:2.78;

β+:1.07

0

1.503E+04 1.503E+04 8.591E+06 NUBASE

3762 103-Lr-253M 0.5- 3.000E+04 1.5 s 20

α m:90.91; SF:8.08;

β+:1.01

0

1.431E+04 1.431E+04 8.059E+06 NUBASE

3763 103-Lr-254 ? 13 s 23.08

α:76.00; β+:12.00;

β+m:12.00

0

3.901E+05 3.901E+05 6.677E+06 NUBASE

3764 103-Lr-255 3.5- 22 s 18.18

α:69.00; β+:30.00;

SF:1.00

0

3.206E+05 3.206E+05 5.938E+06 NUBASE

3765 103-Lr-256 ? 27 s 11.11

α:84.97; β+:15.00;

SF:0.03

0

2.022E+05 2.022E+05 7.491E+06 NUBASE

3766 103-Lr-257 4.5+ 0.646 s 3.87

α:100.00

1

8.990E+06 ENSDF

3767 103-Lr-258 ? 4.1 s 7.32

α:47.50; α m:47.50;

β+:5.00

0

5.600E+04 5.600E+04 8.436E+06 NUBASE

3768 103-Lr-259 4.5+ 6.2 s 4.84

α:77.53; SF:21.87;

β+:0.60

0

3.459E+03 3.459E+03 6.654E+06 NUBASE

3769 103-Lr-260 ? 3 m 16.67

α:80.00; β+:20.00

0

1.780E+05 1.780E+05 6.588E+06 NUBASE

3770 103-Lr-261 ? 39 m 30.77

SF:50.00; α:50.00

0

4.069E+06 NUBASE

3771 103-Lr-262 ? 4 h 100

β+:45.00; SF:10.00;

α:22.50; α m:22.50

0

3.255E+05 3.255E+05 3.603E+06 NUBASE

3772 103-Lr-263 ? 5 h 100

α:100.00

0

7.625E+06 NUBASE

3773 104-Rf-253 3.5+ 0.013 s 38.46

SF:50.00; α:50.00

0

4.773E+06 NUBASE

3774 104-Rf-254 0.0+ 2.3E-05 s 13.04

SF:98.50; α:1.50

0

1.406E+05 NUBASE

3775 104-Rf-255 4.5- 1.64 s 6.71

α m:48.00; SF:52.00

0

4.298E+06 NUBASE

3776 104-Rf-255M 2.5+ 1 s 40

α:100.00

0

9.065E+06 NUBASE

3777 104-Rf-256 0.0+ 6.45E-03 s 3.88

SF:99.68; α:0.32

0

2.858E+04 NUBASE

3778 104-Rf-257 0.5+ 4.7 s 6.38

α:87.60; β+:11.00;

SF:1.40

0

1.170E+05 1.170E+05 7.915E+06 NUBASE

3779 104-Rf-257M 5.5- 1.140E+05 3.9 s 10.26

α:99.30; SF:0.70

0

9.086E+06 NUBASE

3780 104-Rf-258 0.0+ 0.012 s 16.67

SF:87.00; α:13.00

0

1.203E+06 NUBASE

3781 104-Rf-259 3.5+ 2.8 s 14.29

α:91.72; SF:7.98;

β+:0.30

0

2.542E+03 2.542E+03 8.366E+06 NUBASE

3782 104-Rf-260 0.0+ 0.021 s 4.76

SF:97.99; α:2.00;

β+:0.01

0

4.350E+00 8.700E+00 1.780E+05 NUBASE

3783 104-Rf-261 1.5+ 5.5 s 45.45

α:60.00; SF:40.00

0

5.189E+06 NUBASE

3784 104-Rf-261M 4.5+ 7.000E+04 1.35 m 11.11

α:75.00; β+:15.00;

SF:10.00

0

9.125E+04 9.125E+04 6.539E+06 NUBASE

3785 104-Rf-262 0.0+ 2.3 s 17.39

SF:99.20; α:0.80

0

6.788E+04 NUBASE

3786 104-Rf-262M ? 6.000E+05 0.047 s 10.64

SF:100.00

0

NUBASE

3787 104-Rf-263 1.5+ 11 m 27.27

SF:70.00; α:30.00

0

2.492E+06 NUBASE

3788 104-Rf-264 0.0+ 1 h 100

α:100.00

0

8.145E+06 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 145

MAIN DATA TABLES

Page 146: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3789 104-Rf-265 1.5+ 13 h 100

α:100.00

0

7.785E+06 NUBASE

3790 105-Db-255 ? 1.7 s 29.41

α:80.00; SF:20.00

0

7.772E+06 NUBASE

3791 105-Db-256 ? 1.9 s 21.05

α:32.00; β+:36.00;

SF:32.00

0

7.781E+05 7.781E+05 3.026E+06 NUBASE

3792 105-Db-257 4.5+ 1.53 s 11.11

α:46.53; α m:46.53;

SF:5.94; β+

m:0.99

0

1.418E+04 1.418E+04 8.572E+06 NUBASE

3793 105-Db-257M 0.5- 1.000E+05 0.79 s 16.46

α:43.07; α m:43.07;

SF:12.87; β+:0.99

0

1.488E+04 1.488E+04 8.020E+06 NUBASE

3794 105-Db-258 ? 4.5 s 13.33

α:63.37; β+:35.64;

SF:0.99

0

6.356E+05 6.356E+05 6.004E+06 NUBASE

3795 105-Db-258M ? 6.000E+04 20 s 50

β+:100.00

0

1.803E+06 1.803E+06 NUBASE

3796 105-Db-259 ? 0.51 s 31.37

α:100.00

0

9.615E+06 NUBASE

3797 105-Db-260 ? 1.52 s 8.55

α:88.20; SF:9.37;

β+:2.44

0

3.683E+04 3.683E+04 8.277E+06 NUBASE

3798 105-Db-261 ? 1.8 s 22.22

α:82.00; SF:18.00

0

7.556E+06 NUBASE

3799 105-Db-262 ? 35 s 14.29

α:67.00; SF:30.00;

β+:1.50; β+

m:1.50

0

3.580E+04 3.580E+04 6.033E+06 NUBASE

3800 105-Db-263 ? 29 s 31.03

SF:56.00; α:37.10;

β+:6.90

0

5.221E+04 5.221E+04 3.278E+06 NUBASE

3801 105-Db-264 ? 3 m 100

α:100.00

0

8.655E+06 NUBASE

3802 105-Db-265 ? 15 m 100

α:100.00

0

8.495E+06 NUBASE

3803 106-Sg-258 0.0+ 3.3E-03 s 30.30

SF:80.00; α:20.00

0

1.935E+06 NUBASE

3804 106-Sg-259 0.5+ 0.58 s 36.21

α m:81.82; SF:18.18

0

8.047E+06 NUBASE

3805 106-Sg-260 0.0+ 3.8E-03 s 21.05

SF:60.00; α:40.00

0

3.968E+06 NUBASE

3806 106-Sg-261 3.5+ 0.23 s 26.09

α:49.50; α m:49.50;

SF:1.00

0

9.651E+06 NUBASE

3807 106-Sg-262 0.0+ 8E-03 s 37.50

SF:78.00; α:22.00

0

2.111E+06 NUBASE

3808 106-Sg-263 4.5+ 1 s 20

α:70.00; SF:30.00

0

6.577E+06 NUBASE

3809 106-Sg-263M 1.5+ 1.000E+05 0.12 s 100

α:50.00; IT:50.00

0

5.000E+04 4.748E+06 NUBASE

3810 106-Sg-264 0.0+ 0.4 s 100

α:100.00

0

9.205E+06 NUBASE

3811 106-Sg-265 1.5+ 8 s 37.50

α m:50.00; SF:50.00

0

4.505E+06 NUBASE

3812 106-Sg-266 0.0+ 21 s 28.57

α:17.00; α m:17.00;

SF:66.00

0

2.919E+06 NUBASE

3813 106-Sg-269 ? 35 s 65.71

α:100.00

0

8.795E+06 NUBASE

3814 107-Bh-260 ? 3E-04 s 100

α:100.00

0

1.047E+07 NUBASE

3815 107-Bh-261 ? 0.013 s 30.77

α:45.24; α m:45.24;

SF:9.52

0

9.514E+06 NUBASE

3816 107-Bh-262 ? 0.29 s 55.17

α:40.00; α m:40.00;

SF:20.00

0

8.212E+06 NUBASE

3817 107-Bh-262M ? 3.000E+05 0.014 s 28.57

α:45.00; α m:45.00;

SF:10.00

0

9.509E+06 NUBASE

3818 107-Bh-263 ? 0.2 s 100

α:100.00

0

1.009E+07 NUBASE

3819 107-Bh-264 ? 1.3 s 38.46

α:50.00; β+:50.00

0

8.817E+05 8.817E+05 4.983E+06 NUBASE

3820 107-Bh-265 ? 0.5 s 100

α:100.00

0

9.765E+06 NUBASE

146 THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009

MAIN DATA TABLES

Page 147: JEFF-3.1/-3.1.1 radioactive decay data and fission yields ... · 1 JEFF-3.1 fission product mass distributions for seven fission ing systems..... 22 2 The calculated total decay heat

Matn Nuclide

SpPa

Exc ener

Half-life (%-err)

Decay modes (%)

Nsp

<β> (eV)

<γ> (eV)

<α>

(eV)

Source

3821 107-Bh-266 ? 5 s 60

α:100.00

0

9.555E+06 NUBASE

3822 107-Bh-267 ? 22 s 45.45

α:100.00

0

9.375E+06 NUBASE

3823 107-Bh-269 ? 25 s 100

α:100.00

0

8.835E+06 NUBASE

3824 108-Hs-263 3.5+ 1E-03 s 100

α:100.00

0

1.067E+07 NUBASE

3825 108-Hs-264 0.0+ 5.4E-04 s 55.56

α:50.00; SF:50.00

0

5.298E+06 NUBASE

3826 108-Hs-265 4.5+ 2.1E-03 s 14.29

α:99.00; SF:1.00

0

1.048E+07 NUBASE

3827 108-Hs-265M 1.5+ 4.000E+05 7.8E-04 s 19.23

α:100.00

0

1.099E+07 NUBASE

3828 108-Hs-266 0.0+ 2.7E-03 s 37.04

α:98.60; SF:1.40

0

1.020E+07 NUBASE

3829 108-Hs-267 1.5+ 0.032 s 46.88

α m:100.00

0

1.002E+07 NUBASE

3830 108-Hs-268 0.0+ 2 s 100

α:100.00

0

9.905E+06 NUBASE

3831 108-Hs-269 ? 27 s 62.96

α:100.00

0

9.625E+06 NUBASE

3832 108-Hs-273 1.5+ 50 s 100

α:100.00

0

9.905E+06 NUBASE

3833 109-Mt-265 ? 2E-03 s 100

α:100.00

0

1.107E+07 NUBASE

3834 109-Mt-266 ? 1.2E-03 s 33.33

α:47.25; α m:47.25;

SF:5.50

0

1.025E+07 NUBASE

3835 109-Mt-266M ? 1.230E+06 6E-03 s 50

α:50.00; α m:50.00

0

1.208E+07 NUBASE

3836 109-Mt-267 ? 0.01 s 100

α:100.00

0

1.087E+07 NUBASE

3837 109-Mt-268 ? 0.053 s 39.62

α:100.00

0

1.073E+07 NUBASE

3838 109-Mt-269 ? 0.2 s 100

α:100.00

0

1.054E+07 NUBASE

3839 109-Mt-270 ? 2 s 100

α:100.00

0

1.035E+07 NUBASE

3840 109-Mt-271 ? 5 s 100

α:100.00

0

1.014E+07 NUBASE

3841 109-Mt-273 ? 20 s 100

α:50.00; SF:50.00

0

5.413E+06 NUBASE

3842 110-Ds-267 4.5+ 1E-05 s 80

α:100.00

0

1.228E+07 NUBASE

3843 110-Ds-268 0.0+ 1E-04 s 100

α:100.00

0

1.192E+07 NUBASE

3844 110-Ds-269 1.5+ 2.3E-04 s 47.83

α m:100.00

0

1.119E+07 NUBASE

3845 110-Ds-270 0.0+ 1.6E-04 s 62.50

α:99.80; SF:0.20

0

1.117E+07 NUBASE

3846 110-Ds-270M 10.0- 1.140E+06 0.01 s 60

α:50.00; IT:50.00

0

5.700E+05 6.168E+06 NUBASE

3847 110-Ds-271 5.5- 0.21 s 80.95

α:100.00

0

1.088E+07 NUBASE

3848 110-Ds-271M 4.5+ 2.900E+04 1.3E-03 s 38.46

α:100.00

0

1.090E+07 NUBASE

3849 110-Ds-272 0.0+ 1 s 100

SF:100.00

0

NUBASE

3850 110-Ds-273 6.5- 3.6E-04 s 77.78

α:100.00

0

1.138E+07 NUBASE

3851 110-Ds-273M 1.5+ 1.980E+05 0.12 s 100

α:100.00

0

1.157E+07 NUBASE

3852 111-Rg-272 ? 2E-03 s 40

α:100.00

0

1.145E+07 NUBASE

THE JEFF-3.1/-3.1.1 RADIOACTIVE DECAY DATA AND FISSION YIELDS SUB-LIBRARIES – © OECD/NEA 2009 147

MAIN DATA TABLES

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