首页> 外文会议>Conference on Biomedical Applications of Light Scattering; 20080119-21; San Jose,CA(US) >Measuring tissue optical properties in vivo using reflectance-mode confocal microscopy and OCT
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Measuring tissue optical properties in vivo using reflectance-mode confocal microscopy and OCT

机译:使用反射模式共聚焦显微镜和OCT测量体内组织光学性质

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The ability to separately measure the scattering coefficient (μ_s [cm~(-1)]) and the anisotropy (g) is difficult, especially when measuring an in vivo site that can not be excised for bench-top measurements. The scattering properties μ_s and g) can characterize the ultrastructure of a biological tissue (nuclear size, mitochondra, cytoskeletion, collagen fibers, density of membranes) without needing an added contrast agent. This report describes the use of reflectance-mode confocal scanning laser microscopy (rCSLM) to measure optical properties. rCSLM is the same as optical coherence tomography (OCT) when the OCT is conducted in focus-tracking mode. The experimental measurement involves translating the depth of focus, z_f, of an objective lens, down into a tissue. As depth z increases, the reflected signal R decreases due to attenuation by the tissue scattering (and absorption, μ_a). The experimental data behaves as a simple exponential, R(z) = ρ exp(-μz_f) where p is the local reflectivity (dimensionless) and μ [cm~(-1)] is an attenuation coefficient. The relationship between (ρ,μ) and (μ_s,g) is: μ=(μ_s a(g)+μ_a)2G(g,NA) ρ =μ_s L_f b(g,NA) where a(g) is a factor that drops from 1 to 0 as g increases from 0 to 1 (determined by Monte Carlo simulations) allowing photons to reach the focus despite scattering, G is a geometry factor describing the average photon pathlength that depends on the numerical aperture (NA) of the lens and the anisotropy (g), L_f is the axial extent of the focus, and b(g,NA) is the fraction of scattered light that backscatters into the lens for detection.
机译:分别测量散射系数(μ_s[cm〜(-1)])和各向异性(g)的能力非常困难,尤其是在测量无法从台式测量中切除的体内部位时。散射特性(μs和g)可以表征生物组织的超微结构(核大小,线粒体,细胞骨架,胶原纤维,膜的密度),而无需添加造影剂。该报告介绍了使用反射模式共聚焦扫描激光显微镜(rCSLM)来测量光学性能。当在焦点跟踪模式下进行OCT时,rCSLM与光学相干断层扫描(OCT)相同。实验测量包括将物镜的聚焦深度z_f向下转换为组织。随着深度z的增加,反射信号R由于组织散射(和吸收μ_a)引起的衰减而减小。实验数据表现为简单指数,R(z)=ρexp(-μz_f),其中p是局部反射率(无量纲),μ[cm〜(-1)]是衰减系数。 (ρ,μ)与(μ_s,g)之间的关系为:μ=(μ_sa(g)+μ_a)2G(g,NA)ρ=μ_sL_f b(g,NA)其中a(g)为a当g从0增加到1(由蒙特卡洛模拟确定)时,因数从1下降到0(允许蒙特卡罗模拟确定),尽管有散射,光子仍能到达焦点,G是一个几何因子,描述了平均光子光程,它取决于透镜和各向异性(g),L_f是焦点的轴向范围,b(g,NA)是散射光向后散射到透镜中以进行检测的比例。

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