proof of concept demonstration of confidante peter marleau ...€¦ · proof of concept...

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Proof of concept demonstration of CONFIDANTE Sandia National Laboratories is a multimission laboratory managed and operated by National Technology and Engineering Solutions of Sandia, LLC, a wholly owned subsidiary of Honeywell International, Inc., for the U.S. Department of Energy’s National Nuclear Security Administration under contract DE-NA0003525. Approved for Unlimited Release: SAND2017-9204 C Peter Marleau 1 , Rebecca Krentz-Wee 2 1 Sandia National Laboratories, [email protected] 2 Dept. Of Nuclear Engineering, University of California Berkeley Motivation Future nuclear arms reduction treaties are likely to require technical means to verify declarations that items being dismantled and/or removed from a regime are in fact nuclear warheads. Because the radiation signatures of nuclear warheads carry information sensitive to key attributes unique to their nature, radiation detection measurements are often looked to as a means of providing confidence in confirming these declarations. However, for the same reason, the act of confirming certain attributes might reveal critical design information that treaty parties will likely wish to protect. Overcoming the hurdle of verifiably using unique radiation signatures to provide confidence while simultaneously protecting sensitive design data is the primary goal of this work. CONFIDANTE CONfirmation using a Fast-neutron Imaging Detector with Anti-image Null- positive Time Encoding (CONFIDANTE) is a physical implementation of a Zero Knowledge Protocol 12 (ZKP) that uses time encoded imaging (TEI) to provide confidence that the nuclear material in two objects is identical in geometry and activity. TEI is a method which consists of a single fast neutron detector pixel surrounded by a rotating cylindrical coded mask 3 . A TEI with a mask designed such that the pattern on one half of the cylinder is accompanied by its anti-pattern on the opposite side exhibits an unmodulated detection rate if and only if two objects placed on opposite sides of the system are identical in geometry and activity. A positive confirmation is indicated by a constant rate at all times, revealing no additional information. Neutron Detector Rate Rotation Angle (deg) Single neutron detector Mask pattern Anti-mask pattern A pair of 252 Cf sources on the left side Neutron Detector Rate Rotation Angle (deg) Two identical pairs of 252 Cf sources on opposite sides A pair of 252 Cf sources on the right side Neutron Detector Rate Rotation Angle (deg) Measurement of two identical Plutonium Oxide Hemispheres on opposite sides of CONFIDANTE Object 1 Object 2 mean counts /deg σ 2 /deg χ2/NDF P(χ 2 ,NDF) Two 252 Cf at 130° 202.61 872.25 4.39 9E-152 Two 252 Cf at -50° 228.17 1219.55 5.43 2E-216 Two 252 Cf at -50° Two 252 Cf at 130° 377.92 391.31 1.05 0.25 PuO 2 hemi at 130° 9.97 12.45 1.28 3E-4 PuO 2 hemi at -50° 24.73 47.77 1.98 2E-25 PuO 2 hemi at -50° PuO 2 hemi at 130° 19.16 19.56 1.04 0.27 PuO 2 hemi at -50° PuO 2 hemi rotated by 90° at 130° 30.00 39.73 1.36 7E-6 Proof of concept measurements The table (left) reports the results of two sets of proof of concept measurements: a pair of matched 252 Cf sources separated by 20 cm and a pair of matched PuO 2 hemispheres. Neutron counts as a function of rotation angle and reconstructed images of the 252 Cf pairs are shown above. It can be seen that when identical sources are exactly opposite, the rate is consistent with Poisson noise as indicated by the near equivalence of the count mean and variance and a χ 2 /NDF of close to 1 against the null hypothesis of a constant rate. When one of the PuO 2 hemis is rotated by 90°, the null hypothesis is no longer consistent with the data. MLEM reconstructed image (source on left) Azimuthal Position (deg) Vertical Position (cm) MLEM reconstructed image (source on right) Azimuthal Position (deg) Vertical Position (cm) 1 A. Glaser, B. Barak, R. J. Goldston, Nature. 13457, June 26, 2014, Vol. 510, pp. 497-502. 2 P. Marleau, R. Krentz-Wee, Sandia Technical Report SAND2017-1649 3 J. Brennan, E. Brubaker, M. Gerling, P. Marleau, et al, Nuclear Instruments and Methods A., Vol. 802, pgs. 76-81, 2015.

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Page 1: Proof of concept demonstration of CONFIDANTE Peter Marleau ...€¦ · Proof of concept demonstration of CONFIDANTE. Sandia National Laboratories is a multimission laboratory managed

Proof of concept demonstration of CONFIDANTE

Sandia National Laboratories is a multimission laboratory managed and operated by National Technology and Engineering Solutions of Sandia, LLC, a wholly owned subsidiary of Honeywell International, Inc., for the U.S. Department of Energy’s National Nuclear Security Administration under contract DE-NA0003525. Approved for Unlimited Release: SAND2017-9204 C

Peter Marleau1, Rebecca Krentz-Wee2

1Sandia National Laboratories, [email protected]. Of Nuclear Engineering, University of California Berkeley

MotivationFuture nuclear arms reduction treaties are likely to require technical means to verify declarations that items being dismantled and/or removed from a regime are in fact nuclear warheads. Because the radiation signatures of nuclear warheads carry information sensitive to key attributes unique to their nature, radiation detection measurements are often looked to as a means of providing confidence in confirming these declarations. However, for the same reason, the act of confirming certain attributes might reveal critical design information that treaty parties will likely wish to protect. Overcoming the hurdle of verifiably using unique radiation signatures to provide confidence while simultaneously protecting sensitive design data is the primary goal of this work.

CONFIDANTECONfirmation using a Fast-neutron Imaging Detector with Anti-image Null-positive Time Encoding (CONFIDANTE) is a physical implementation of a Zero Knowledge Protocol12 (ZKP) that uses time encoded imaging (TEI) to provide confidence that the nuclear material in two objects is identical in geometry and activity. TEI is a method which consists of a single fast neutron detector pixel surrounded by a rotating cylindrical coded mask3. A TEI with a mask designed such that the pattern on one half of the cylinder is accompanied by its anti-pattern on the opposite side exhibits an unmodulated detection rate if and only if two objects placed on opposite sides of the system are identical in geometry and activity. A positive confirmation is indicated by a constant rate at all times, revealing no additional information.

Neutron Detector Rate

Rotation Angle (deg)

Single neutron detector

Mask pattern

Anti-mask pattern

A pair of 252Cf sources on the left side

Neutron Detector Rate

Rotation Angle (deg)

Two identical pairs of 252Cf sources on opposite sides A pair of 252Cf sources on the right side

Neutron Detector Rate

Rotation Angle (deg)

Measurement of two identical Plutonium Oxide Hemispheres on opposite sides of CONFIDANTE

Object 1 Object 2

mean counts/deg σ2/deg χ2/NDF P(χ2,NDF)

Two 252Cf at 130° 202.61 872.25 4.39 9E-152

Two 252Cf at -50° 228.17 1219.55 5.43 2E-216

Two 252Cf at -50°

Two 252Cf at 130° 377.92 391.31 1.05 0.25

PuO2 hemi at 130° 9.97 12.45 1.28 3E-4

PuO2 hemi at -50° 24.73 47.77 1.98 2E-25

PuO2 hemi at -50°

PuO2 hemi at 130° 19.16 19.56 1.04 0.27

PuO2 hemi at -50°

PuO2 hemi rotated by 90° at 130° 30.00 39.73 1.36 7E-6

Proof of concept measurementsThe table (left) reports the results of two sets of proof of concept measurements: a pair of matched 252Cf sources separated by 20 cm and a pair of matched PuO2 hemispheres. Neutron counts as a function of rotation angle and reconstructed images of the 252Cf pairs are shown above. It can be seen that when identical sources are exactly opposite, the rate is consistent with Poisson noise as indicated by the near equivalence of the count mean and variance and a χ2/NDF of close to 1 against the null hypothesis of a constant rate. When one of the PuO2 hemis is rotated by 90°, the null hypothesis is no longer consistent with the data.

MLEM reconstructed image (source on left)

Azimuthal Position (deg)

Vert

ical

Pos

ition

(cm

)

MLEM reconstructed image (source on right)

Azimuthal Position (deg)

Vert

ical

Pos

ition

(cm

)

1 A. Glaser, B. Barak, R. J. Goldston, Nature. 13457, June 26, 2014, Vol. 510, pp. 497-502.2 P. Marleau, R. Krentz-Wee, Sandia Technical Report SAND2017-16493 J. Brennan, E. Brubaker, M. Gerling, P. Marleau, et al, Nuclear Instruments and Methods A., Vol. 802, pgs. 76-81, 2015.