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Optical scattering properties of soft tissue: a discrete particle model

机译:软组织的光学散射特性:离散粒子模型

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摘要

We introduce a micro-optical model of soft biological tissue that permits numerical computation of the absolute magnitudes of its scattering coefficients. A key assumption of the model is that the refractive-index variations caused by microscopic tissue elements can be treated as particles with sizes distributed according to a skewed log-normal distribution function. In the limit of an infinitely large variance in the particle size, this function has the same power-law dependence as the volume fractions of the subunits of an ideal fractal object. To compute a complete set of optical coefficients of a prototypical soft tissue (single-scattering coefficient, transport scattering coefficient, backscattering coefficient, phase function, and asymmetry parameter), we apply Mie theory to a volume of spheres with sizes distributed according to the theoretical distribution. A packing factor is included in the calculation of the optical cross sections to account for correlated scattering among tightly packed particles. The results suggest that the skewed log-normal distribution function, with a shape specified by a limiting fractal dimension of 3.7, is a valid approximation of the size distribution of scatterers in tissue. In the wavelength range 600 less than or equal to lambda less than or equal to 1400 nm, the diameters of the scatterers that contribute most to backscattering were found to be significantly smaller (lambda/4-lambda/2) than the diameters of the scatterers that cause the greatest extinction of forward-scattered Light(3-4 lambda). (C) 1998 Optical Society of America. [References: 40]
机译:我们介绍了一种软生物组织的微光学模型,该模型允许对其散射系数的绝对大小进行数值计算。该模型的关键假设是,可以将由微观组织元素引起的折射率变化视为具有根据对数正态正态分布函数偏斜分布的大小的粒子。在无限大的粒径变化范围内,此函数与理想分形对象的亚基的体积分数具有相同的幂律依赖性。为了计算原型软组织的完整光学系数(单散射系数,传输散射系数,后向散射系数,相位函数和不对称参数),我们将Mie理论应用于一定体积的球体,并根据该理论分配尺寸分配。在光学横截面的计算中包括堆积因子,以说明紧密堆积的颗粒之间的相关散射。结果表明,偏斜对数正态分布函数具有由3.7的极限分形维数指定的形状,是组织中散射体大小分布的有效近似值。在小于或等于λ小于或等于1400 nm的波长范围内,发现对背向散射影响最大的散射体的直径显着小于散射体的直径(lambda / 4-lambda / 2)导致最大的前向散射光(3-4λ)的消光。 (C)1998年美国眼镜学会。 [参考:40]

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