Physical Review Special Topics. Accelerators and Beams (Jun 2014)

High-power, photofission-inducing bremsstrahlung source for intense pulsed active detection of fissile material

  • J. C. Zier,
  • D. Mosher,
  • R. J. Allen,
  • R. J. Commisso,
  • G. Cooperstein,
  • D. D. Hinshelwood,
  • S. L. Jackson,
  • D. P. Murphy,
  • P. F. Ottinger,
  • A. S. Richardson,
  • J. W. Schumer,
  • S. B. Swanekamp,
  • B. V. Weber

DOI
https://doi.org/10.1103/PhysRevSTAB.17.060401
Journal volume & issue
Vol. 17, no. 6
p. 060401

Abstract

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Intense pulsed active detection (IPAD) is a promising technique for detecting fissile material to prevent the proliferation of special nuclear materials. With IPAD, fissions are induced in a brief, intense radiation burst and the resulting gamma ray or neutron signals are acquired during a short period of elevated signal-to-noise ratio. The 8 MV, 200 kA Mercury pulsed-power generator at the Naval Research Laboratory coupled to a high-power vacuum diode produces an intense 30 ns bremsstrahlung beam to study this approach. The work presented here reports on Mercury experiments designed to maximize the photofission yield in a depleted-uranium (DU) object in the bremsstrahlung far field by varying the anode-cathode (AK) diode gap spacing and by adding an inner-diameter-reducing insert in the outer conductor wall. An extensive suite of diagnostics was fielded to measure the bremsstrahlung beam and DU fission yield as functions of diode geometry. Delayed fission neutrons from the DU proved to be a valuable diagnostic for measuring bremsstrahlung photons above 5 MeV. The measurements are in broad agreement with particle-in-cell and Monte Carlo simulations of electron dynamics and radiation transport. These show that with increasing AK gap, electron losses to the insert and outer conductor wall increase and that the electron angles impacting the bremsstrahlung converter approach normal incidence. The diode conditions for maximum fission yield occur when the gap is large enough to produce electron angles close to normal, yet small enough to limit electron losses.