Appl Opt. 2022 Jan 10;61(2):375-385. doi: 10.1364/AO.443854.
Using integrating spheres (ISs) in conjunction with the inverse adding-doubling algorithm (IAD) offers a well-established, rigorous protocol for determining optical absorption () and reduced scattering () coefficients of thin, optically homogeneous, turbid media. Here, we report the performance and use of a single IS system for experimentally retrieving optical properties in phantom media whose optical properties were well controlled. The IS system was used to measure the total reflectance and transmittance between 500 and 800 nm in liquid phantoms that were prepared to span a wide range of optical scattering and absorption coefficients. Measurements on phantoms were sequentially made using one of two broadband light sources-a halogen lamp or a supercontinuum laser. We report on the accuracy of IAD-derived optical coefficients using IS measurements made on phantoms-directly or by employing one of two previously reported correction methods. The first (sample-substitution error) correction was experimentally achieved while the second used Monte Carlo-based corrections with IAD. When experimentally calibrated reflectance and transmittance values were directly used as inputs to the IAD, mean absolute errors in recovered optical coefficients were larger than 0.4 for absorption and more than 6 for scattering across all phantoms and wavelengths measured. These errors reduced to 0.06-0.17 and 0.7-2 for and , respectively, with the use of corrections. Choice of light sources used, sample geometry (relative to optical coefficients), signal-to-noise of measurements, and the selection of correction methods are discussed.
利用积分球(ISs)结合逆加-加倍算法(IAD)为确定薄的、光学均匀的、混浊介质的光学吸收()和散射()系数提供了一种成熟的、严格的方法。在这里,我们报告了单个 IS 系统的性能和使用情况,该系统用于在光学性质得到很好控制的模拟介质中实验性地获取光学性质。IS 系统用于测量在 500 到 800nm 之间的液体模拟体的总反射率和透射率,这些模拟体的光学散射和吸收系数范围很广。使用两种宽带光源之一-卤素灯或超连续激光-对模拟体进行了顺序测量。我们报告了使用 IS 测量在模拟体上直接或使用两种先前报道的校正方法之一获得的 IAD 衍生光学系数的准确性。第一种(样品替代误差)校正通过实验实现,而第二种使用基于蒙特卡罗的 IAD 校正。当直接将实验校准的反射率和透射率值用作 IAD 的输入时,在所有测量的模拟体和波长下,恢复光学系数的平均绝对误差在吸收方面大于 0.4,在散射方面大于 6。通过使用校正,这些误差分别减少到 0.06-0.17 和 0.7-2。讨论了光源的选择、样品几何形状(相对于光学系数)、测量的信噪比以及校正方法的选择。