1967
DOI: 10.1016/0029-554x(67)90373-4
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Tissue current-to-dose conversion factors for neutrons with energies from 0.5 to 60 MeV

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Cited by 18 publications
(4 citation statements)
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“…The neutron transport code MCNP4B (Briesmeister 1991) was utilized to calculate the spectral fluence ⌽ E (E) and the neutron-induced photon kerma K ␥ at 14 penetration depths between 0.1 and 19.9 cm in the tissue equivalent slab. The standard soft tissue composition indicated by ICRU report 33 (1980) was used (mass fractions 0.101 H, 0.111 C, 0.026 N, and 0.762 O), and this presents a nitrogen content lower than in previous calculations (Snyder and Neufeld 1957;Irving et al 1967). ENDF/VI cross sections and light water data for thermal neutrons with hydrogen binding corrections at thermal energies were used for neutrons; standard MCNP4B cross sections were used for photons.…”
Section: Monte Carlo Calculationsmentioning
confidence: 99%
“…The neutron transport code MCNP4B (Briesmeister 1991) was utilized to calculate the spectral fluence ⌽ E (E) and the neutron-induced photon kerma K ␥ at 14 penetration depths between 0.1 and 19.9 cm in the tissue equivalent slab. The standard soft tissue composition indicated by ICRU report 33 (1980) was used (mass fractions 0.101 H, 0.111 C, 0.026 N, and 0.762 O), and this presents a nitrogen content lower than in previous calculations (Snyder and Neufeld 1957;Irving et al 1967). ENDF/VI cross sections and light water data for thermal neutrons with hydrogen binding corrections at thermal energies were used for neutrons; standard MCNP4B cross sections were used for photons.…”
Section: Monte Carlo Calculationsmentioning
confidence: 99%
“…Progressive improvement of modelling the human anatomy has had a formative influence on the development of computational phantoms. Early radiation transport studies used semi-infinite homogeneous 30 cm slab phantoms (Snyder 1950, Alsmiller and Moran 1968, Alsmiller et al 1970, Beck 1970, Irving et al 1967, then homogeneous elliptical cylinders (Auxier et al 1969, Sidewell et al 1969, Snyder 1971, also with embedded inhomogeneous parts to simulate the lungs (Sidewell and Burlin 1973), later a homogeneous (Snyder 1965) and finally a heterogeneous human phantom, which became to be known as the MIRD5 phantom (Snyder et al 1968(Snyder et al , 1978. Body and organs of this stylized human phantom and of its derivations (Cristy 1980, Kramer et al 1982, Stabin et al 1995 were based on mathematical equations of geometrical bodies, like ellipsoids, truncated cones, tori, planes and intersections between them.…”
Section: Computational Phantomsmentioning
confidence: 99%
“…Emax > 25 For convenience, we use a polynomial fit of PER(Ep). Values from the fit are compared in Table 6 with those from Equation (16). The correction factor CP(Ep) is related to PER(Ep) by , .…”
Section: Packing Of Track Coordinate Datamentioning
confidence: 99%