1996
DOI: 10.13182/nse96-a24184
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Improvement of Gamma-Ray SnTransport Calculations Including Coherent and Incoherent Scatterings and Secondary Sources of Bremsstrahlung and Fluorescence: Determination of Gamma-Ray Buildup Factors

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Cited by 22 publications
(7 citation statements)
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“…The TRIPOLI-4 TTB implementation proceeds along the lines indicated by Kitsos, Diop, Assad, et al [16] and Riz [17]. The most notable difference with respect to the MCNP6 implementation concerns the fact that TRIPOLI-4 accounts for the angular straggling of the condensed electrons; therefore, the bremsstrahlung photons are not necessarily emitted around the initial electron direction.…”
Section: E Thick-target Bremsstrahlung Modementioning
confidence: 99%
“…The TRIPOLI-4 TTB implementation proceeds along the lines indicated by Kitsos, Diop, Assad, et al [16] and Riz [17]. The most notable difference with respect to the MCNP6 implementation concerns the fact that TRIPOLI-4 accounts for the angular straggling of the condensed electrons; therefore, the bremsstrahlung photons are not necessarily emitted around the initial electron direction.…”
Section: E Thick-target Bremsstrahlung Modementioning
confidence: 99%
“…They have been calculated by running a discrete ordinates transport code, TWODANT [8], and following a method described by KITSOS, et al [9]. Energy groups, angular mesh and space mesh have met the following features: 218 energy groups from 1 keV to 10 MeV, P7 for the Legendre expansion of the scattering cross sections, S96 for the Gauss-Legendre angular quadrature and at least 28 spatial meshes per mean free path.…”
Section: Single-layer Shield Build-up Factorsmentioning
confidence: 99%
“…The application of two modules, RECONR and GAMINR, in the NJOY [15] cross-section processing code constructed the pointwise, energy dependent cross sections from the ENDF photoatomic files into a multigroup photon structure that could be used for primary photon interactions. Scattering cross section calculations were determined with the Legrende order P 7 approximation and a 1/E weight function based on Kitsos' analysis of Legrende expansions [17]. The Legrende order is a polynomial equation that is fitted to the stated ENDF probability P(u) of a photon's interaction as a function of the cosine of the angle at which it interacts, whereas the Monte Carlo code tabulates the probability from the specific ENDF curve.…”
Section: Group Structure and Cross Sectionsmentioning
confidence: 99%