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Characterization of Solution-Grown Stilbene for Nonproliferation Applications M.M. Bourne, A. Di Fulvio, S.D. Clarke Department of Nuclear Engineering & Radiological Sciences, University of Michigan, Ann Arbor, MI 48109, USA S.A. Pozzi, [email protected] Consortium for Verification Technology (CVT) Motivation New neutron detectors are needed for nonproliferation applications such as NPT verification Solution-grown stilbene developed by LLNL (Fig. 1) Can be grown to diameters of 5 cm or larger Excellent pulse-shape discrimination (PSD) capabilities (Fig. 2) Solid scintillator has built-in advantages over liquid scintillators in field Objectives Characterize detector resolution, neutron detection efficiency, and PSD capabilities of solution-grown stilbene detectors Fig. 1. Photos of stilbene scintillation cells and a detector assembly. Detector Resolution Stilbene is an organic scintillator, where Compton scattering is the dominant gamma interaction Backscatter gate technique was developed to isolate energy deposition from Compton scatter [1] (Figs. 3 & 4) So far, 137 Cs and 54 Mn were used, both monoenergetic gamma sources Measurement set to record correlated interactions only Threshold set to isolate a monoenergetic peak from scattered gamma rays Neutron Efficiency Important for characterizing stilbene in safeguards applications such as multiplicity counting Stilbene crystals with length ranging from 1”-4” were used to measure a 252 Cf source (Fig. 6) 33-keVee threshold Room return neglected 2” stilbene crystal has intrinsic neutron efficiency Eff of 27% (Table I) 4” crystal improves to 39% Time-of-Flight Measurement Speed of particle allows for identification independent of PSD and neutron energy Allows for characterizing PSD of scintillator Can use to measure response function, light output, even resolution (requires long flight path and much longer measurement times) Measured 252 Cf using each stilbene at 1 meter (Fig. 7) Time difference be tween start and stop detector gives time-of-flight (Fig. 8) 5”x 5” EJ-309 start detector 39-keVee measurement threshold Gamma misclassification rate measured as low as 10 -6 for stilbene, an order-of-magnitude lower than EJ-309 Fig. 5. Measured stilbene resolution as function of light output, compared directly to a EJ-309 liquid scintillator. Fig. 3. Schematic of measurement for stilbene detector resolution. Fig. 2. Tail-vs-total integral plot for stilbene measuring 252 Cf at a 60-keVee threshold. Fig. 6. Schematic of measurement for intrinsic neutron efficiency. Table I. Measured neutron intrinsic efficiency for stilbene as a function of scintillator length. Fig. 7. Time-of-flight measurement setup. Fig. 8. Time-of-flight distribution for each stilbene detector. This work was funded in-part by the Consortium for Verification Technology under Department of Energy National Nuclear Security Administration award number DE-NA0002534 References 1. G. Pausch, K. Roemer, C. Herbach, Y. Kong, R. Lentering, C. Plettner, F. Scherwinski, and J. Stein, Characterization and Calibration of Large-Volume PVT Detectors by Backscatter Gating, transactions of the 2011 IEEE Nuclear Science Symposium. N. Zaitseva, S. Payne Source, Angle Measured Light Output 137 Cs, 45° 182 keVee 137 Cs, 180° 470 keVee 54 Mn, 180° 633 keVee 252 Cf 1” stilbene 2” stilbene 3” stilbene 4” stilbene 2” 20 cm Crystal Photomultiplier tube Base Stilbene NaI Stilbene NaI Measurement was modeled using MCNPX-PoliMi to determine the geometric uncertainty from this experiment Resolution of stilbene found to be 8.5% at 470 keVee (fig. 5) Eff = 252 Cf neutron counts 252 Cf incident neutrons Gamma Region Neutron Region Most probable neutron energy ~ 2 MeV Fig. 4. Correlated pulse height spectrum for stilbene measuring 54 Mn scattered gammas. 252 Cf EJ-309 start detector 2.54-cm stilbene stop detector 5.08-cm stilbene stop detector 7.62-cm stilbene stop detector 10.16-cm stilbene stop detector Stilbene Thickness Neutron Efficiency 2.54 cm 17.7% 5.08 cm 26.9% 7.62 cm 35.1% 10.16 cm 38.6%

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  • Characterization of Solution-Grown Stilbene for Nonproliferation Applications M.M. Bourne, A. Di Fulvio, S.D. Clarke

    Department of Nuclear Engineering & Radiological Sciences,

    University of Michigan, Ann Arbor, MI 48109, USA

    S.A. Pozzi, [email protected]

    Consortium for Verification Technology (CVT)

    Motivation New neutron detectors are needed for nonproliferation applications such as NPT verification

    Solution-grown stilbene developed by LLNL (Fig. 1)

    – Can be grown to diameters of 5 cm or larger

    – Excellent pulse-shape discrimination (PSD) capabilities (Fig. 2)

    – Solid scintillator has built-in advantages over liquid scintillators in field

    Objectives Characterize detector resolution, neutron detection efficiency, and PSD capabilities of solution-grown stilbene detectors

    Fig. 1. Photos of stilbene scintillation cells and a detector assembly.

    Detector Resolution Stilbene is an organic scintillator, where Compton scattering is the dominant gamma interaction

    Backscatter gate technique was developed to isolate energy deposition from Compton scatter [1] (Figs. 3 & 4)

    – So far, 137Cs and 54Mn were used, both monoenergetic gamma sources

    – Measurement set to record correlated interactions only

    – Threshold set to isolate a monoenergetic peak from scattered gamma rays

    Neutron Efficiency Important for characterizing stilbene in safeguards applications such as multiplicity counting

    Stilbene crystals with length ranging from 1”-4” were used to measure a 252Cf source (Fig. 6)

    – 33-keVee threshold

    – Room return neglected

    2” stilbene crystal has intrinsic neutron efficiency Eff of 27% (Table I)

    – 4” crystal improves to 39%

    Time-of-Flight Measurement Speed of particle allows for identification independent of PSD and neutron energy

    – Allows for characterizing PSD of scintillator

    – Can use to measure response function, light output, even resolution (requires long flight path and much longer measurement times)

    Measured 252Cf using each stilbene at 1 meter (Fig. 7)

    – Time difference be tween start and stop detector gives time-of-flight (Fig. 8)

    – 5”x 5” EJ-309 start detector

    – 39-keVee measurement threshold

    Gamma misclassification rate measured as low as 10-6 for stilbene, an order-of-magnitude lower than EJ-309

    Fig. 5. Measured stilbene resolution as function of light output, compared directly to a EJ-309 liquid

    scintillator.

    Fig. 3. Schematic of measurement for stilbene detector resolution.

    Fig. 2. Tail-vs-total integral plot for stilbene measuring 252Cf at a 60-keVee threshold.

    Fig. 6. Schematic of measurement for intrinsic neutron efficiency.

    Table I. Measured neutron intrinsic efficiency for stilbene as a function of scintillator length.

    Fig. 7. Time-of-flight measurement setup.

    Fig. 8. Time-of-flight distribution for each stilbene detector.

    This work was funded in-part by the Consortium for Verification Technology under Department of Energy National Nuclear Security Administration award number DE-NA0002534

    References 1. G. Pausch, K. Roemer, C. Herbach, Y. Kong, R. Lentering, C. Plettner, F. Scherwinski, and J. Stein, Characterization and Calibration of Large-Volume PVT Detectors by Backscatter Gating, transactions of the 2011 IEEE Nuclear Science Symposium.

    N. Zaitseva, S. Payne

    Source, Angle

    Measured Light Output

    137Cs, 45° 182 keVee 137Cs, 180° 470 keVee 54Mn, 180° 633 keVee

    252Cf

    1” stilbene

    2” stilbene 3” stilbene

    4” stilbene

    2”

    20 cm

    Crystal Photomultiplier tube

    Base

    Stilb

    ene

    NaI

    Stilb

    ene

    NaI

    Measurement was modeled using MCNPX-PoliMi to determine the geometric uncertainty from this experiment Resolution of stilbene found to be 8.5% at 470 keVee (fig. 5)

    Eff =252Cf neutron counts

    252Cf incident neutrons

    Gamma Region

    Neutron Region

    Most probable neutron energy ~ 2 MeV

    Fig. 4. Correlated pulse height spectrum for stilbene measuring 54Mn scattered gammas.

    252Cf

    EJ-309 start detector

    2.54-cm stilbene stop detector

    5.08-cm stilbene stop detector

    7.62-cm stilbene stop detector

    10.16-cm stilbene stop detector

    Stilbene Thickness

    Neutron Efficiency

    2.54 cm 17.7%

    5.08 cm 26.9%

    7.62 cm 35.1%

    10.16 cm 38.6%