New evaluation of d+Li data up to 50 MeV for IFMIF
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Transcript of New evaluation of d+Li data up to 50 MeV for IFMIF
New evaluation of d+Li data up to 50 MeV for IFMIF
P. Pereslavtsev, U. Fischer
Association FZK-EuratomForschungszentrum Karlsruhe, Germany
Technical Meeting on International Fusion Materials Irradiation Facility
Forschungszentrum Karlsruhe, 4-6 October 2005
Forschungszentrum Karlsruhein der Helmholtz-Gemeinschaft
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 2
HistoryHistory 1998 – FZK (P. Wilson) simple evaporation model; Serber stripping model; experimental data for thick target at 32 MeV analytical formulas used in MCNP source subroutine (McDeli) 1999 – INPE-FZK analytical formulas for deuteron elastic scattering; optical model potentials; intranuclear cascade model; Serber stripping model; experimental data for thick target at 32 MeV ENDF-6 formatted files for deuteron energies up to 50 MeV new source subroutine for MCNP based on NJOY processed files
2001 – FZK revisions of INPE evaluated data based on experimental data for thick targets at 32 and 40 MeV 2004 – FZK revisions of INPE evaluated data (new deuteron elastic scattering data based on phenomenological OMP from 1 to 50 MeV)
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 3
Status of d+Li data (EStatus of d+Li data (Edd=17 MeV)=17 MeV)
0 10 20 30 4010-2
10-1
100
101
102
Bem, 2003 Bem, 2003 FZK, 1999
Li(d,xn), E
d=17 MeV
d2 /d/
dE [
mb/
sr M
eV]
Emitted neutron energy [MeV]
0 5 10 15 20 25 30
10-4
10-3
10-2
10-1
100
101
Li(d,xn), E
d=17 MeV
d2 /d/
dE [
mb/
sr M
eV]
Emitted neutron energy [MeV]
0 10 20 3010-5
10-4
10-3
10-2
10-1
=1200
Li(d,xn), Ed=17 MeV
Bem FZK, 1999
Neu
tron
yie
ld [
1010
n/s
r/M
eV
/C]
Emitted neutron energy [MeV]
0 10 20 30 4010-5
10-4
10-3
10-2
10-1
100
=00
Li(d,xn), Ed=17 MeV
Bem FZK, 1999
N
eutr
on y
ield
[10
10 n
/sr/
MeV
/C]
Emitted neutron energy [MeV]
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 4
Status of d+Li data (EStatus of d+Li data (Edd=40 MeV)=40 MeV)
0 10 20 30 40 50 6010-5
10-4
10-3
10-2
10-1
100
101
=00
Li(d,xn), Ed=40 MeV
Baba FZK, 1999
Neu
tron
yie
ld [
1010
n/s
r/M
eV/C
]
Emitted neutron energy [MeV]
0 10 20 30 40 50 6010-2
10-1
100
101
102
Baba,2003 FZK, 1999
Li(d,xn), E
d=40 MeV
d2/
d/d
E [
mb/
sr M
eV]
Emitted neutron energy [MeV]
0 10 20 30 40 50 6010-7
10-6
10-5
10-4
10-3
10-2
10-1
100
101
=450
Li(d,xn), Ed=40 MeV
Baba FZK, 1999
Neu
tron
yie
ld [
1010
n/s
r/M
eV/C
]
Emitted neutron energy [MeV]
0 10 20 30 40 50 6010-4
10-3
10-2
10-1
100
101
Li(d,xn), E
d=40 MeV
d2/
d/d
E [
mb/
sr M
eV]
Emitted neutron energy [MeV]
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 5
Background and goalsBackground and goals
The neutron source for IFMIF is based on d+Li reactions;
Available high energy general purpose d+Li data files fail in description of the experimental data;
General purpose deuteron cross section data files have to cover energies up to 50 MeV;
Data should include particle and photons emission spectra to enable nuclear heating calculations;
Data files should be ENDF-6 formatted for processing with the standard NJOY99 code.
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 6
Flowchart of the evaluation processFlowchart of the evaluation process
EvaporationEvaporation PreequilibriumPreequilibrium StrippingStripping DirectDirect
SerberSerber
modelmodelDWUCKDWUCK
Neutron spectraNeutron spectra
processingprocessing
GNASHGNASHECIS95ECIS95
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 7
Optical model calculationsOptical model calculations
DEUTERONS
NEUTRONS
PROTONS
TRITONS
ALPHAS
1 Ed 50 MeV, M. Avrigeanu, local for 6Li and 7Li
0.01 En 12 MeV, S. Chiba, for 6Li, modified
12 En 70 MeV, A. Koning & Delaroche, modified
0.1 Ep 50 MeV, Beccheti & Greenless
0.1 Et 50 MeV, Beccheti & Greenless
0.1 E 70 MeV, V. Avrigeanu & Hodgson
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 8
Deuteron OMP (reaction cross-section)Deuteron OMP (reaction cross-section)
0 10 20 30 40 500
200
400
600
800
1000
1200
1400
Maddison, 62 Satchler, 66 Abramovich, 76 FZK-99 present results
(Avrigeanu OMP)
7Li+d reaction cross section
Cro
ss s
ectio
n [m
b]
Neutron energy [MeV]
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 9
Deuteron OMP (elastic scattering)Deuteron OMP (elastic scattering)
0 20 40 60 80 100 120 140 160 180100
101
102
103
104
Abramovich, 76 Bojowald Avregeanu
d + 7Li Elastic scatteringE
d= 10 MeV
d/d
[mb
/sr]
c.m.
[deg]
0 20 40 60 80 100 120 140 160 180100
101
102
103
104
Matsuki, 69 Bojowald Avregeanu
d + 7Li Elastic scatteringE
d= 14.7 MeV
d/d
[mb
/sr]
c.m.
[deg]
0 20 40 60 80 100 120 140 160 180100
101
102
103
104
Bingham, 71 Bojowald Avregeanu
d + 6Li Elastic scatteringE
d= 12 MeV
d/d
[mb
/sr]
c.m.
[deg]
0 20 40 60 80 100 120 140 160 18010-3
10-2
10-1
100
101
102
103
Rudchik, 96 Bojowald Avregeanu
d + 6Li Elastic scatteringE
d= 50 MeV
d/d
[mb
/sr]
c.m.
[deg]
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 10
Neutron OMPsNeutron OMPs
10-2 10-1 100 101
0
1000
2000
3000
4000
5000
6000
7000
Baba, 79 Drake, 77 Olsson, 90 Langsdorf, 57 Templon, 85 Levin, 60 Chiba (orig.) Koning (orig.) evaluation
9Be+n elastic scattering
Cros
s se
ctio
n [m
b]Neutron energy [MeV]
10-2 10-1 100 101
0
1000
2000
3000
4000
5000
6000
7000
Schwartz, 71 Bubb, 74 Peterson, 60 Bilpuch, 61 Chiba (orig.) Koning (orig.) evaluation
9Be+n total cross section
Cr
oss
sect
ion
[mb]
Neutron energy [MeV]
Chiba OMP modifications:Chiba OMP modifications:
VVrr=V=V00ee--(E-E(E-Eff))++VV11energy energy
dependentdependent
Koning OMP modifications:Koning OMP modifications:
rrWd Wd and aand aWd Wd – 20 % less – 20 % less
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 11
Neutron OMP (elastic scattering)Neutron OMP (elastic scattering)
0 20 40 60 80 100 120 140 160 180102
103
104
105
106
107
108
109
Chiba (mod.)
n+9Be
6 MeV (*106)
4 MeV (*104)
2 MeV (*102)
0.5 MeV
d/d
[m
b/sr
]
c.m.
[deg]
0 20 40 60 80 100 120 140 160 180100
101
102
103
104
105
106
107
108
109
Koning (mod.) Chiba (mod.)
22 MeV (*106)
18 MeV (*104)
14 MeV (*102)
10 MeV
n+9Be
d/d
[m
b/sr
]
c.m.
[deg]
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 12
The use of GNASH codeThe use of GNASH code
Hauser-Feshbach statistical model for equilibrium;
Exciton preequlibrium model by Kalbach;
Transmission coefficients prepared by ECIS96 (DWBA);
Gilbert-Cameron level density form;
Nuclear structure data from RIPL-2 collection;
Kalbach systematics for secondary particle angular distributions
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 13
LevelLevel scheme used for scheme used for 77Li(d,n) Li(d,n) 88Be calculationsBe calculations
Elevel (MeV) Q (MeV) Parity (MeV)
0.0 15.03 0+ 0.007
3.04 11.99 2+ 1.500
11.40 3.63 4+ 3.500
16.63 -1.60 2+ 0.108
18.10 -3.07 1+ 0.138
18.91 -3.88 2- 0.122
19.07 -4.04 3+ 0.270
19.24 -4.21 3+ 0.230
19.40 -4.37 1- 0.650
19.86 -4.83 4+ 0.700
20.20 -5.17 0+ 1.000
20.90 -5.87 4- 1.600
21.50 -6.47 3+ 1.000
22.00 -6.97 1- 4.000
22.20 -7.17 2+ 0.800
24.00 -8.97 2- 7.000
level 1level 1level 1level 1
level 2level 2level 2level 2
““level” 3level” 3““level” 3level” 3
level 4level 4level 4level 4
level 5level 5level 5level 5
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 14
Level scheme used for Level scheme used for 66Li(d,n) Li(d,n) 77Be calculationsBe calculations
Elevel (MeV) Q (MeV) Parity (MeV)
0.00 3.38 3/2-
0.43 2.95 1/2-
4.57 -1.19 7/2- 0.175
6.73 -3.35 5/2- 1.200
7.21 -3.83 5/2- 0.500
9.27 -5.89 7/2-
9.90 -6.52 3/2- 1.800
11.01 -7.63 3/2- 0.320
17.00 -13.62 1/2- 6.500
level 1level 1level 1level 1
level 3level 3level 3level 3
level 1level 1level 1level 1
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 15
Direct reactions (angular distributions)Direct reactions (angular distributions)
0 20 40 60 80 100 120 140 160 18010-1
100
101
Gangadharan, 69 DWUCK4
Ed=17 MeV
6Li(d,n)7Be(g.s.)
d/d
[m
b/sr
]
cm
[deg]
0 20 40 60 80 100 120 140 160 18010-2
10-1
100
101
Rudchik, 96 DWUCK4
Ed=50 MeV
6Li(d,n)7Be (g.s.)
d/d
[m
b/sr
]
cm
[deg]
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 16
Neutron spectra calculations (ENeutron spectra calculations (Edd=17 MeV)=17 MeV)
0 5 10 15 20 25 30 3510-3
10-2
10-1
100
101
102
Bem, 03 Bem, 03 evaporation prequilibrium stripping 1 level 2 level 3 level 4 level 5 level total
7Li(d,xn), Ed=17 MeV
d2 /d/
dE [
mb/
sr M
eV]
Emitted neutron energy [MeV]
0 5 10 15 20 25 30 3510-3
10-2
10-1
100
101
102
Bem, 03 Bem, 03 evaporation prequilibrium stripping 1 level 2 level 3 level 4 level 5 level total
7Li(d,xn), Ed=17 MeV
d2 /d/
dE [
mb/
sr M
eV]
Emitted neutron energy [MeV]
0 5 10 15 20 25 30 3510-3
10-2
10-1
100
101
102
Bem, 03 Bem, 03 evaporation prequilibrium stripping 1 level 2 level 3 level 4 level 5 level total
7Li(d,xn), Ed=17 MeV
d2 /d/
dE [
mb/
sr M
eV]
Emitted neutron energy [MeV]
0 5 10 15 20 25 30 3510-3
10-2
10-1
100
101
102
Bem, 03 Bem, 03 evaporation prequilibrium stripping 1 level 2 level 3 level 4 level 5 level total
7Li(d,xn), Ed=17 MeV
d2 /d/
dE [
mb/
sr M
eV]
Emitted neutron energy [MeV]
0 5 10 15 20 25 30 3510-3
10-2
10-1
100
101
102
Bem, 03 Bem, 03 evaporation prequilibrium stripping 1 level 2 level 3 level 4 level 5 level total
7Li(d,xn), Ed=17 MeV
d2 /d/
dE [
mb/
sr M
eV]
Emitted neutron energy [MeV]
0 5 10 15 20 25 30 3510-3
10-2
10-1
100
101
102
Bem, 03 Bem, 03 evaporation prequilibrium stripping 1 level 2 level 3 level 4 level 5 level
7Li(d,xn), Ed=17 MeV
d2 /d/
dE [
mb/
sr M
eV]
Emitted neutron energy [MeV]
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 17
Neutron spectra calculations (ENeutron spectra calculations (Edd=40 MeV)=40 MeV)
0 10 20 30 40 50 6010-2
10-1
100
101
102
Li(d,xn), E
d=40 MeV
d2/
d/d
E [
mb/
sr M
eV]
Emitted neutron energy [MeV]
0 10 20 30 40 50 6010-2
10-1
100
101
102
Li(d,xn), E
d=40 MeV
d2/
d/d
E [
mb/
sr M
eV]
Emitted neutron energy [MeV]
0 10 20 30 40 50 6010-2
10-1
100
101
102
Li(d,xn), E
d=40 MeV
d2/
d/d
E [
mb/
sr M
eV]
Emitted neutron energy [MeV]
0 10 20 30 40 50 6010-2
10-1
100
101
102
Li(d,xn), E
d=40 MeV
d2/
d/d
E [
mb/
sr M
eV]
Emitted neutron energy [MeV]
0 10 20 30 40 50 6010-2
10-1
100
101
102
Li(d,xn), E
d=40 MeV
d2/
d/d
E [
mb/
sr M
eV]
Emitted neutron energy [MeV]
0 10 20 30 40 50 6010-2
10-1
100
101
102
Li(d,xn), E
d=40 MeV
d2/
d/d
E [
mb/
sr M
eV]
Emitted neutron energy [MeV]
0 10 20 30 40 50 6010-2
10-1
100
101
102
Baba, 03 evaporation preequilibrium stripping 1st level 2nd level total
Li(d,xn), E
d=40 MeV
d2/
d/d
E [
mb/
sr M
eV]
Emitted neutron energy [MeV]
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 18
Results of the evaluationResults of the evaluation
0 5 10 15 20 25 30 3510-410-310-210-1100101102103104105106107108109
101010111012101310141015101610171018
Bem, 03 Bem, 03 evaluation
=120o(*1016)
=75o(*1012)
=45o(*108)
=20o(*104)
=0o
Ed=17 MeV
d+7Li
d2
/d/
dE [m
b/sr M
eV]
Emitted neutron energy [MeV]
0 10 20 30 40 50 6010-310-210-1100101102103104105106107108109
101010111012101310141015101610171018
Baba, 03 evaluation
=110o (*1016)
=60o (*1012)
=30o (*108)
=15o (*104)
=0o
Ed=40 MeV
d+Li
d2/d
/dE
[mb/s
r MeV
]
Emitted neutron energy [MeV]
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 19
Benchmark calculationsBenchmark calculations
10-3
10-2
10-1
100
(new d-Li data)
MannMCNPX
Baba
McDeLicious
0o
Ed = 40 MeV
100
10-3
10-2
10-1
100
(2001 d-Li data)
15o
200
10-5
10-4
10-3
10-2
10-1
100
300
Neu
tro
n Y
ield
[
10
10 n
/sr/
MeV
/C
]
450
10-6
10-5
10-4
10-3
10-2
10-1
600
900
0 10 20 30 40 5010-6
10-5
10-4
10-3
10-2
10-1
Neutron Energy, MeV
1100
0 10 20 30 40 50 60
Technical Meeting on IFMIF, Forschungszentrum Karlsruhe, October 4-6 2005 20
ConclusionsConclusions
Complete Complete evaluated deuteron general purpose files prepared for lithium isotopes 6Li and 7Li, incident energy 0 -50 MeV, the data are stored in MT=2,5 and MF=3 and 6.
Processed with standard ENDF-6 format checkersProcessed with standard ENDF-6 format checkers
Processed with Processed with NJOY99NJOY99 system system
Tested by Tested by MCNP4C MCNP4C benchmark calculationsbenchmark calculations