1989
DOI: 10.1016/0021-9991(89)90067-3
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Similarity relations for anisotropic scattering in Monte Carlo simulations of deeply penetrating neutral particles

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Cited by 62 publications
(29 citation statements)
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“…(1), which we rewrite as (8) with the same boundary conditions (2). Once again expanding the single scattering phase function f in Legendre polynomials, and rearranging, (8) may be rewritten (9) where is the scattering mean free path in the medium. Now by introducing a parameter called the excess mean free path, λ s and constants a n (λ s ) that depend on it by means of the equation the equation (10) where replaces (9) and is algebraically identical to it.…”
Section: Improved Models: Transport Condensed History (Tch) Methodsmentioning
confidence: 99%
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“…(1), which we rewrite as (8) with the same boundary conditions (2). Once again expanding the single scattering phase function f in Legendre polynomials, and rearranging, (8) may be rewritten (9) where is the scattering mean free path in the medium. Now by introducing a parameter called the excess mean free path, λ s and constants a n (λ s ) that depend on it by means of the equation the equation (10) where replaces (9) and is algebraically identical to it.…”
Section: Improved Models: Transport Condensed History (Tch) Methodsmentioning
confidence: 99%
“…Once again expanding the single scattering phase function f in Legendre polynomials, and rearranging, (8) may be rewritten (9) where is the scattering mean free path in the medium. Now by introducing a parameter called the excess mean free path, λ s and constants a n (λ s ) that depend on it by means of the equation the equation (10) where replaces (9) and is algebraically identical to it. This equation incorporates an enlarged scattering mean free path λ + λ s that approaches the original scattering mean free path λ as the excess mean free path, λ s , approaches 0.…”
Section: Improved Models: Transport Condensed History (Tch) Methodsmentioning
confidence: 99%
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