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海洋中辐照度场的非弹性散射贡献模拟:夫琅禾费线深度变化

Simulation of inelastic-scattering contributions to the irradiance field in the ocean: variation in Fraunhofer line depths.

作者信息

Ge Y, Gordon H R, Voss K J

出版信息

Appl Opt. 1993 Jul 20;32(21):4028-36. doi: 10.1364/AO.32.004028.

Abstract

Raman scattering and fluorescence are important processes in oceanic optics because of their influence on the natural light field in the water. Monte Carlo simulations are described that verify that measurements of the Fraunhofer line depth in the in-water irradiance can be used to separate the irradiance into elastic and inelastic components, i.e., components that are generated by elastic- and inelastic-scattering processes, respectively. Specifically, the upwelling and downwelling irradiances, including Raman scattering, are simulated for a variety of model oceans. The inherent optical properties of the ocean are derived from a bio-optical model in which the elastic-scattering and the absorption coefficients of the biological material depend only on the phytoplankton pigment concentration, C. The Fraunhofer line at 656 nm is found to fill in, i.e., disappear into, the background continuum rapidly with increasing depth. This indicates a rapid transition from a near-surface light field dominated by elastic s cattering to one composed of irradiance derived entirely from Raman scattering. Conversely the depth of the Fraunhofer line at 486 mm is nearly independent of depth in the water, indicating that Raman scattering never makes a significant contribution to the irradiance there. Between these two extremes, the lines at 518 and 589 nm show variations in line depths that depend significantly on C, e.g., at 518 nm the line fills in with increasing depth at low-C values but not at high-C values.

摘要

拉曼散射和荧光在海洋光学中是重要的过程,因为它们会影响水中的自然光场。本文描述了蒙特卡罗模拟,这些模拟验证了水中辐照度中夫琅禾费线深度的测量可用于将辐照度分离为弹性和非弹性分量,即分别由弹性散射和非弹性散射过程产生的分量。具体而言,针对各种模型海洋模拟了包括拉曼散射在内的向上和向下辐照度。海洋的固有光学特性源自一个生物光学模型,其中生物材料的弹性散射和吸收系数仅取决于浮游植物色素浓度C。发现656nm处的夫琅禾费线随着深度增加迅速融入背景连续谱,即消失。这表明从以弹性散射为主的近表面光场迅速过渡到完全由拉曼散射产生的辐照度组成的光场。相反,486nm处的夫琅禾费线深度在水中几乎与深度无关,这表明拉曼散射在那里对辐照度从未有过显著贡献。在这两个极端之间,518nm和589nm处的谱线深度变化显著取决于C,例如,在518nm处,低C值时谱线随着深度增加而融入,但高C值时并非如此。

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