The amplitude of the coherent backscattering intensity peak for discrete random media: effect of packing density

The amplitude of the coherent backscattering intensity peak is computed for a medium composed of densely packed, randomly positioned particles. The cyclical component of the Stokes reflection matrix at exactly the back scatter ing direction is expressed in terms of the ladder component, and the ladd...

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Збережено в:
Бібліографічні деталі
Видавець:Головна астрономічна обсерваторія НАН України
Дата:2010
Автор: Mishchenko, M.I.
Формат: Стаття
Мова:English
Опубліковано: Головна астрономічна обсерваторія НАН України 2010
Назва видання:Кинематика и физика небесных тел
Теми:
Онлайн доступ:http://dspace.nbuv.gov.ua/handle/123456789/73239
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Цитувати:The amplitude of the coherent backscattering intensity peak for discrete random media: effect of packing density / M.I. Mishchenko // Кинематика и физика небесных тел. — 2010. — Т. 26, № 3. — С. 3-14. — Бібліогр.: 29 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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Резюме:The amplitude of the coherent backscattering intensity peak is computed for a medium composed of densely packed, randomly positioned particles. The cyclical component of the Stokes reflection matrix at exactly the back scatter ing direction is expressed in terms of the ladder component, and the ladder component is rigorously computed by numerically solving the vector radiative transfer equation. The effect of packing density is accounted for by multiplying the single-scattering Mueller matrix by the static structure factor computed in the Percus — Yevick approximation. It is shown that increasing packing density can substantially reduce the amplitude of the copolarized coherent backscattering peak, especially for smaller particles, and can make it significantly lower than 2. The effect of packing density on the amplitude of the cross-polarized peak is significantly weaker.