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JAEA 2018 Symposium on Nuclear Data
Development of Active Neutron NDA System
Yosuke Toh
Nuclear Science and Engineering Center Japan Atomic Energy Agency
JAEA
Collaborators
This research was implemented under the subsidiary for nuclear security promotion of MEXT.
Y. Toh1, A. Ohzu1, H. Tsuchiya1, K.Furutaka1,F. Kitatani1, M. Komeda1, M. Maeda1, M. Kureta1, M. Koizumi1, M. Seya1, J. Heyse2, C. Paradela2, W. Mondelaers2, P. Schillebeeckx2
T. Bogucarska3, J. Crochemore3, G. Varasano3, K. Abbas3 B. Pedersen3
1 Japan Atomic Energy Agency 2 Joint Research Centre – Geel 3 Joint Research Centre – Ispra
JAEA
Outline
2 Active neutron NDA techniques
3 Development of
Active-N @ NUCEF
4 Summary
1 Objectives
JAEA
Action Sheet -1 (2012 - 2015)
JRC-JAEA Collaboration
Neutron Resonance Densitometry (NRD) For characterization of debris of melted fuel
Action Sheet -7 (2015 – 2017) Developments of active neutron NDA techniques for Nuclear Non-Proliferation, Security and Safety
JRC-JAEA Collaboration:AS-7 JAEA
Investigate and demonstrate active neutron NDA technologies to quantify special nuclear materials and other elements in the presence of high radioactive materials
TRP-PCDF @ Tokai
NUCEF-BECKY @ Tokai
PUNITA @ Ispra
GELINA @ Geel
Experimental facilities JAEA
DT neutron generator
Neutrons
Neutrons can lead to nuclear fission and neutron capture reactions which produce gamma-rays and neutron.
DDA (Differential Die-away Analysis)
PGA (Prompt Gamma-ray Analysis)
NRTA (Neutron Resonance Transmission Analysis)
DGA (Delayed Gamma-ray Analysis)
Nuclear fission
Neutron capture reaction
U
N
239Pueffective
Ratio 235U/Pu
Specific Nuclei of SNA,MA
Explosive,Neutron poison
Excited state
Stable nucleus
Unstable nucleus
Prompt gamma-ray
Delayed gamma-ray
Fission neutron
JAEA
Active neutron NDA techniques
Excited state
Stable nucleus
Stable nucleus 2×109
neutrons/s
14MeV
Sodern Genie35
JAEA
Ideal concept design of NDA system
A D-T Pulsed Neutron Source
Differential Die-away Analysis(DDA)
Delayed Gamma-ray Analysis (DGA)
Prompt Gamma-ray Analysis (PGA)
Neutron Detector Bank
A Li-glass Neutron Detector
(Inside)
Gamma-ray Detector
Transmitted Neutrons
Neutron Resonance Transmission Analysis
(NRTA)
Samples to be Verified Neutron reflector
Neutron Shielding and Transportation
Gamma-ray Detectors
Monte Carlo simulation (PHITS, MVP, MCNP)
DDA
PGA
(DDA,PGA,NRTA,DGA)
Radiation shields for licensing process
Neutron reflector
Neutron moderator Neutron & gamma-ray shields
Collimator Correction methods
Neutron flux distribution
Development of Active-N(DDA,PGA) JAEA
Active-N-II
Developments of detectors
Polyethylene
SUS
Detector bank DT neutron source
Air Air
JAEA
Simulation studies of DDA and PGA
Sample
Simulation studies for prototype system (Active-N) which can measure DDA and PGA have been performed by MCNP (MVP and PHITS).
Differential Die-away Analysis(DDA)
JAEA
Differential Die-Away (DDA) is an active neutron interrogation technique
200L Drum
Shields
DT neutron source Detector bank
Interrogation neutron
Fission neutron
Neutr
on c
ounts
Elaspsed time
Fission neutron(∝ fissile)
Interrogation neutron
Neutron die-away time
1/e
Neutron signal counts DDA measurements
In DDA, a neutron detector measures the time-dependent decay of neutrons from the sample.
0%
100%
200%
300%
400%
500%
0.01g 0.1g 0.5g 1g 5g 10g 15g
3cm4cm5cm6cm7cm8cm9cm10cm
Optimization of moderator thickness
JAEA
DDA:Simulation spectra
Optimum thickness 5cm~6cm
239Pu
Rela
tive
dete
ctio
n
eff
icie
ncy
(fo
r 3cm
)
Elapsed time (μsec)
Neutr
on c
ount
s
Moderator thickness
Moderator
Sample
Detector bank DT neutron source
1.E+0
1.E+2
1.E+4
1.E+6
1.E+8
1.E+10
0 200 400 600 800 1000
Pu-239 15.0g Pu-239 10.0gPu-239 5.0g Pu-239 1.0gPu-239 0.5g Pu-239 0.1gPu-239 0.01g blank
U & Pu
MA
Each nuclide has resonances at specific energies.
Resonances can be used to identify & quantify SNM and MA.
Total cross sections(JENDL-4)
Pulsed Neutron
Sample Neutron Detector
Transmitted neutrons
JAEA
Neutron Resonance Transmission Analysis(NRTA)
240Pu 242Pu
JAEA
Simulation model of a compact NRTA system
DT neutron source
Neutron detector (6Li-glass detector)
Sample
Pb
Flight path length: 5 m
Neutrons
Polyethylene + Stainless steel (SUS) Boron-Polyethylene + Pb
Air Polyethylene Boron-Poly. SUS Al
y [c
m]
The fluxes of neutrons and γ rays
SUS
Polyethylene
Neutron and γ ray fluxes: 1cm or 3cm
30 GWd/t spent fuel (t 1cm)
240Pu (1.03 eV)
242Pu (2.6 eV)
238U (6.7 eV)
Electron linac : 1 us
238Pu (18.6 eV)
241Pu (4.28 eV)
235U (8.76 eV)
239Pu (0.3 eV)
DT tube : 10 us
All Pu, 235U and 238U can be measured with a pulse width (<1 us)
JAEA
Effects of a pulse width of a neutron beam
239Pu, 240Pu, 242Pu and 238U can be measured with DT tube
238U (6.7 eV)
Pulse widths
JAEA
Nuclear data of Radioactive Isotopes
JENDL-4.0
NRTA (and NRCA) can’t be used to measure Se-79
Se-79 is important for long-term safety assessment of a geological repository
ー Exp. ー Cal.
NRTA spectra of Cu-63
Large discrepancy
NRTA measurements of Cu-63 JAEA
Optimization of Γn
Γn =0.59±0.02eV
Γn =0.899±0.005eV
ー Exp. ー Cal.
NRTA measurements of Cu-63 JAEA
C/E = Experiment (Areal density) Calculation (Areal density)
New Γn =0.899±0.005eV Old Γn=0.59±0.02eV
<±2%
C/E
Decision tree of HE, CW, n poisons WP:White phosphorus munitions VX:VX gas (nerve agent) GB:Sarin (nerve agent) HE:High Explosive L:Lewisite gas
H:Sulfur mustard gas CG:Phosgene CK:cyanogen chloride HN:Nitrogen mustard gas FM:Smoke
JAEA
Active-N system can detect all of these elements.
High S/N ratio in the high energy region
• Capture cross section small (sg(25.3meV)~80mb) • Includes high-energy gamma rays (e.g. 10,829keV)
14N, 10,829keV
53Cr, 8884keV
56Fe
, 7
63
1+
76
46
keV
w/ : 330 min. w/o : 140 min.
Detection of Nitrogen gammas (HE) JAEA
JAEA
Summary
Active neutron NDA techniques have been studied and improved in JRC-JAEA collaboration: AS-7.
Nuclear data is still lacking.
Developments of Active-N(DDA,PGA) has been completed successfully in Phase I and Phase II has started.