2011
DOI: 10.1063/1.3586171
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Using Quasi-Monoenergetic Photon Sources To Probe Photo-Fission Resonances

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Cited by 4 publications
(6 citation statements)
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“…To penetrate a given target thicknesses using doses approaching the lowest obtainable values, a first shot at each position can be taken with low flux, and the measured transmission used to determine attenuation for further shots at higher flux. Narrow bandwidth sources at the 10% level near 9 MeV, and at similar fluxes, also improve photofission-based interrogation and characterization by suppressing extraneous signals that can be generated with broader bandwidth or higher energy sources [14]. NRF methods, at isotope specific energies near 2 MeV, offer powerful isotope-specific identification for verification of absence of a substance [15], NDA of fuel [5], and the full range of applications.…”
Section: Monoenergetic Photon Applicationsmentioning
confidence: 98%
“…To penetrate a given target thicknesses using doses approaching the lowest obtainable values, a first shot at each position can be taken with low flux, and the measured transmission used to determine attenuation for further shots at higher flux. Narrow bandwidth sources at the 10% level near 9 MeV, and at similar fluxes, also improve photofission-based interrogation and characterization by suppressing extraneous signals that can be generated with broader bandwidth or higher energy sources [14]. NRF methods, at isotope specific energies near 2 MeV, offer powerful isotope-specific identification for verification of absence of a substance [15], NDA of fuel [5], and the full range of applications.…”
Section: Monoenergetic Photon Applicationsmentioning
confidence: 98%
“…From the physical point of view the term ϕ 0 a(ξ) 2 dξ in (12) means that the electron rides the laser wave, so, during the interaction one observes a Doppler red-shifted signal on the detector. Hence, looking at the detected signal, one can say, that the initial pulse is "stretched" during the interaction.…”
Section: Detector Time Stretchingmentioning
confidence: 99%
“…During the last decades scattering of light on high-energy electron beams has become an indispensable tool for generating tunable wide range X-and γ-radiation [1][2][3][4][5][6][7][8]. These Thomson scattering (TS) sources have found applications in spectroscopy [9][10][11][12], medicine [13], ultrafast radiography [14,15], and nuclear nonproliferation [16][17][18]. The conversion of laser photons to γ-radiation occurs as the Doppler upshift of the laser frequency while scattering on electrons with high gamma-factor.…”
Section: Introductionmentioning
confidence: 99%
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