Status of Current Deployments by LLNL/SNLhanohano/post/AAP2012/... · Sandia National Laboratories...
Transcript of Status of Current Deployments by LLNL/SNLhanohano/post/AAP2012/... · Sandia National Laboratories...
Sandia National Laboratories is a multi-program laboratory managed and operated by Sandia Corporation, a
wholly owned subsidiary of Lockheed Martin Corporation, for the U.S. Department of Energy’s National
Nuclear Security Administration under contract DE-AC04-94AL85000
This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore
National Laboratory in part under Contract W-7405-Eng-48 and in part under Contract DE-AC52-07NA27344.
Status of Current Deployments by
LLNL/SNL
David Reyna Sandia National Laboratories, CA
Lawrence Livermore National Laboratory
David Reyna
A Novel Technology for Reactor Safeguards
Antineutrino Monitoring of Reactors provides independent measurements of Thermal Power and Fissile Inventory
Non-intrusive with NO connection to plant systems
Continuous Remote Monitoring
Highly tamper resistant
Potential Applications to Present and Future Safeguards
Independent Confirmation of Operator Declarations
Reduction in needed Inspector visits
Provide fissile content information for Next-Generation fuel cycles (MOX, Th, bulk process)
Lawrence Livermore National Laboratory
Recent IAEA interactions and
interest
IAEA convened an ad-hoc physicist/inspector working
group in Vienna in September 2011
Expressed interest by IAEA after 2008 expert’s
workshop in Vienna:
• Shipper-receiver differences,
• Bulk Process/ Online Refuel Reactor
Verification
• Research reactor power
• Safeguards by Design, Integrated Safeguards
• Aboveground Detection
David Reyna
Lawrence Livermore National Laboratory
CANDU and Bulk Process Reactors
The daily movement of fuel bundles at a CANDU plant presents a safeguards challenge - item accountancy remains a primary strategy
Close analogue to future Bulk Process Reactors
Item accountancy is not possible on the
―continuous‖ or finely divided fuel of a
BPR – a Bulk Materials Accountancy
approach will be necessary.
Loss of Continuity of Knowledge over
the core contents would be difficult to
recover
David Reyna
Lawrence Livermore National Laboratory
May 2007: Visit to AECL Chalk River
Mar. 2008: PLGS shutdown; first CANDU6 to undergo full
refurbishment (e.g. all reactor tubes to be replaced); planned restart
late 2009
Early 2009: AECL provides introduction to PLGS Rx Physics group
April 2009: First visit to PLGS; enthusiastic reception
Sept. 2009: Approval letter for deployment with PLGS support ―after
unit is back at power‖
Oct. 2009: Meeting at PLGS: AECL, SNL, LLNL, NA-22
Jan. 2010: 15 month refurbishment delay officially announced
Oct. 2010: Second refurbishment delay announced: full return to
service in Fall 2012 (all new tubes to be removed and replaced)
Mar 2012: Approval received for site prep work
Sep 2012 : Data collection begins – TBD
• Materials are staged at PLGS awaiting installation
Timeline
David Reyna
Lawrence Livermore National Laboratory
Deployment Location
David Reyna
Distance:
~77 m from
reactor core
Overburden:
~18 m.w.e.
Lawrence Livermore National Laboratory
Detector Design
David Reyna
To compensate for reduced flux, target will be 4m3 of BC-525 (0.1% Gd);
• expect ~20% overall efficiency
• Per m2 of footprint, ~10x as efficient as SONGS1
Double ended readout using 24x10‖ R7081 PMTs
• Acrylic windows, sealed via PTFE encapsulated o-rings
Optical coupling and hydrostatic support via mineral oil
Shielding from 6 interlocking water tanks (0.5m) and 2.5cm Borated Poly.
5cm thick muon veto on 5 sides.
Lawrence Livermore National Laboratory
Quantity SONGS 1
CANDU
estimates
Reactor thermal power 3.4 GW 2.2 GW
Core distance ~25 m ~77 m
Relative Flux 1.00 0.08
Detector active mass 0.64 tons 3.6 tons
Deployed Footprint 6 m2 10 m2
Overburden ~25 m.w.e. ~ 18 m.w.e.
n interaction rate *
efficiency = detection rate
~ 4000/day * 10% =
~ 400/day
~2000/day *20% =
~ 400/day
Comparison to previous experiment
David Reyna
Lawrence Livermore National Laboratory
Scintillator level Filling
Buffer tank: Mineral Oil
Inner Tank: Gd-doped Scintillator
10‖ PMT
LED Calibration device
•Inner tank and Buffer tank fully constructed
•Inner detector electronics completed
•Inner detector assembled, filled and tested at LLNL.
•Modular water shield constructed and installed.
•Full assembly test with shield and veto completed.
•DAQ software upgrade ongoing.
Detector Assembly/Testing
David Reyna
Lawrence Livermore National Laboratory
Detector Assembly/Testing
Shield Installation
Filling
Mineral Oil
Scintillator
David Reyna
Lawrence Livermore National Laboratory
Reconstructed event position(Cf-252 source
data) Initial calibrations have been
performed with a Cf-252 and Th-
228 source located on the outer
edge of the buffer tank
Initial Data/Calibration
David Reyna
Neutron Capture Spectrum
Lawrence Livermore National Laboratory
Significantly
Improved:
1. Energy
Resolution
2. Gd g-ray
shower
containment
The energy
resolution
improvements
lead to a
potential
positron spectral
analysis
Performance Comparison:
Neutron Capture Response (data)
David Reyna
Lawrence Livermore National Laboratory
PLGS is currently completing a full refurbishment.
• For only the second (and likely last) time, it will have a fresh core load at
restart
We hoped to measure the initial evolution to an equilibrium core.
• Online refueling will begin at about FPD75
• The current delays suggest we may miss the heart of this burn-in
David Reyna
Expected Observation
Lawrence Livermore National Laboratory
CANDU Summary
Barring unforeseen problems, a deployment at a CANDU reactor is scheduled for later this year.
• This will be our first antineutrino measurement of a reactor under safeguards.
• This will be the first antineutrino measurement of a CANDU core
This measurement will provide insight into Bulk Process Reactor operations.
• We had hoped to get fresh startup, but may still measure some fuel evolution
This detector represents our best performing homogeneous design yet
David Reyna
Lawrence Livermore National Laboratory
Aboveground Challenge is all about
Backgrounds
Without overburden or passive shielding, a detector is exposed to: • High muon rates • Hadronic showers • Electromagnetic showers • Secondary particles produced by all of the above in the
detector and its surroundings
Most of detector size is passive shielding
• Active detector in SONGS 1 design was less than 6% of total volume
• A shield can reduce backgrounds in a simple and cost effective way
Belowground (only a few meters) many of these
cosmic backgrounds are significantly reduced • To date, even below ground detectors have required
additional passive shielding
With good detector design, the need for shielding may be reduced or eliminated entirely
• Conceivably, SONGS1 performance could be achieved with a 1m2 footprint
Particle Identification (PID) is a powerful tool
• Identify and reject fast neutrons and multi-neutron events
• Explicitly tag final state Positron and thermal neutron (capture)
David Reyna
Lawrence Livermore National Laboratory
David Reyna
Standard Detection of
Inverse Beta-decay
We use the same antineutrino detection technique used to first detect (anti)neutrinos:
ne + p g e+ + n
Standard detectors of gammas and neutrons are sufficient to find this correlated signature
Positron
• Immediate
• 1- 8 MeV (incl 511 keV gs)
Neutron
• Thermalization then capture
• Delayed capture (t = 30-100 ms)
n
ne p
511 keV
511 keV e+
Gd, Li, …
t ~ 30 ms
prompt signal + n capture on Gd
Switch to Lithium-6 yields good detection efficiency for compact detectors
Lawrence Livermore National Laboratory
David Reyna
Segmented Scintillator Detector
Individual Segments contain organic scintillator with ZnS:Ag/6LiF screens on outer surface
• 4 cells with plastic or liquid scintillator
Use of ZnS:Ag with 6LiF allows identification of neutron capture
• ZnS:Ag is sensitive to alpha from n-capture on Li
• Very slow scintillator time constant (~100ns) allows pulse shape discrimination to separate n-capture from γ events
With Liquid Scintillator, proton recoils are also easily identified
• Allows a comparison to test need for additional rejection
Ultimate design would be for 16 or 64 cells but this 4-cell prototype was sufficient for first testing
Lawrence Livermore National Laboratory
David Reyna
Particle Identification (PID)
Positron Identification through Topology
Positrons are rare in nature
• Deposit most of their kinetic energy very quickly through standard ionization losses
Positrons will annihilate into two back-to-back 511 keV gammas
• Very distinctive signature
• Gammas will travel ~2-5‖ through most scintillators
en
e+
n
Liquid or Plastic
scintillator
Neutron identification through Pulse Shape Discrimination (PSD)
Liquid Cell Plastic Cell
Lawrence Livermore National Laboratory
David Reyna
Aboveground Performance
Detector Performance looks stable
• Detector efficiencies look reasonable
N-capture efficiency of 18%
Positron efficiency 2—87%
Background rates are reasonable for a
possible observation of reactor
transition
• 2 – 4 orders of magnitude rejection
• 2 methods of analysis agree
Very encouraged by technology
performance
• Operational Difficulties prevented
measurement of reactor transition
• Tested operation outside of the
shield and saw only minimal
increase in detected background
rates
Only Neutron PID
1,830 ev/day
Max PID info
23 ev/day
No PID
225,200 ev/day
Lawrence Livermore National Laboratory
PID = Simple Analysis
Signal Background
David Reyna
Independent measure of uncorrelated backgrounds allows simple subtraction
Automated energy calibration
using naturally occurring
Potassium and
Thorium endpoints
Lawrence Livermore National Laboratory
David Reyna
Preliminary Results of
Aboveground Data (events/day)
Event Definition
Shielded operation (30 days) Unshielded Operation (20 days)
Correlated Un-
correlated
Subtracted
Signal Correlated
Un-
correlated
Subtracted
Signal
1) Using only neutron PID 1118 8 368 5 750 9 15930 32 13835 30 2095 44
2) Neutron + positron PID 119.1 2.6 28.7 1.3 90.4 2.9 1371 9 1168 9 203 13
Event
Def.
Antineutrino Rate
Expectation from MC
1) 18
2) 6
Measured Errors on Subtracted Signal are already
below expected antineutrino signal
• Prototype 4-Cell array is still highly inefficient
Unshielded Operation Shows Promise
• Uncorrelated rates increase by x 40
• Correlated only goes up by x 2—3
• Motivation for subsequent testing
Lawrence Livermore National Laboratory
Segmented Scintillator
Belowground Deployment
Re-packaged 4-cell prototype for optimal deployment • Total system (detector, electronics, HV,
computer) fits within a single rack • Shipped fully assembled (no assembly required)
Deployed below ground, without shield or muon veto • Fully operational within 2 hours of being
placed at location
Stable operation since January 2012 at SONGS • Began data taking during a reactor
refueling outage
• Reactor turn-on delayed until December 2012 (or later)
Lawrence Livermore National Laboratory
Detector Performance Belowground
David Reyna
Expected Signal (~40 ev/day) is larger
than error on background (~7ev/day)
Robust/Continuous unattended operation for several months
Automated calibration/analysis
shows stable performance Neutron Candidates
Positron Candidates
Selected Event Candidates
Lawrence Livermore National Laboratory
David Reyna
Road to a Full System
We believe that a larger version of this detector would demonstrate worthwhile reactor antineutrino sensitivity
Size would depend on desired sensitivity
Without a shield, this is a compact detector system
• Up to 9 cells could fit within the existing rack
• 64-cells could still be contained within a single square meter footprint
16-Cell Array 64-Cell Array
Increase for
Event Def.
1
Increase for
Event Def. 2
Increase for
Event Def. 1
Increase for
Event Def. 2
Increase in Mass x 4 x 4 x 16 x 16
Neutron Capture Efficiency x 2 x 2 x 2.5 x 2.5
Positron Detection Efficiency no change x 1.8 no change x 2
Total Signal Increase x 8 x 14 x 40 x 80
Total Background Increase x 4 x 4 x 16 x 16
Improvement in S/B x 4 x 7 x 10 x 20
Lawrence Livermore National Laboratory
David Reyna
Conclusion
Previously demonstrated short and long
term relative monitoring of power operational
status, and fissile content in reactors
Very encouraged by performance of
Segmented Scintillator prototype • This project aims to expand the range of utility by
reducing the overall footprint and enabling deployment
in high-background or unshielded locations
• Demonstrated rejection of backgrounds of 3+ orders of
magnitude even without an external shield
• Reasonable efficiencies have been achieved even with a
small 4-cell detector
• Increase to a 16 or 64 cell system would show marked
improvement
Looking forward to deployment at a CANDU
reactor scheduled for late 2012. • First deployment at bulk process reactor
• First deployment at reactor currently under safeguards