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厚样本成像:相控蒙特卡罗辐射传递算法。

Imaging in thick samples, a phased Monte Carlo radiation transfer algorithm.

机构信息

University of St. Andrews, SUPA, School of Physics and Astronomy, St. Andrews, United Kingdom.

University of Dundee, School of Science and Engineering, Dundee, United Kingdom.

出版信息

J Biomed Opt. 2021 Sep;26(9). doi: 10.1117/1.JBO.26.9.096004.

DOI:10.1117/1.JBO.26.9.096004
PMID:34490761
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8421375/
Abstract

SIGNIFICANCE

Optical microscopy is characterized by the ability to get high resolution, below 1  μm, high contrast, functional and quantitative images. The use of shaped illumination, such as with lightsheet microscopy, has led to greater three-dimensional isotropic resolution with low phototoxicity. However, in most complex samples and tissues, optical imaging is limited by scattering. Many solutions to this issue have been proposed, from using passive approaches such as Bessel beam illumination to active methods incorporating aberration correction, but making fair comparisons between different approaches has proven to be challenging.

AIM

We present a phase-encoded Monte Carlo radiation transfer algorithm (φMC) capable of comparing the merits of different illumination strategies or predicting the performance of an individual approach.

APPROACH

We show that φMC is capable of modeling interference phenomena such as Gaussian or Bessel beams and compare the model with experiment.

RESULTS

Using this verified model, we show that, for a sample with homogeneously distributed scatterers, there is no inherent advantage to illuminating a sample with a conical wave (Bessel beam) instead of a spherical wave (Gaussian beam), except for maintaining a greater depth of focus.

CONCLUSION

φMC is adaptable to any illumination geometry, sample property, or beam type (such as fractal or layered scatterer distribution) and as such provides a powerful predictive tool for optical imaging in thick samples.

摘要

意义

光学显微镜的特点是能够获得高分辨率(低于 1μm)、高对比度、功能和定量图像。使用诸如光片显微镜的整形照明已经导致具有低光毒性的更大的各向同性三维分辨率。然而,在大多数复杂的样本和组织中,光学成像是受散射限制的。已经提出了许多解决这个问题的方法,从使用被动方法,如贝塞尔光束照明,到主动方法,包括像差校正,但证明在不同方法之间进行公平比较具有挑战性。

目的

我们提出了一种相位编码的蒙特卡罗辐射转移算法(φMC),能够比较不同照明策略的优点或预测单个方法的性能。

方法

我们展示了 φMC 能够模拟诸如高斯或贝塞尔光束的干涉现象,并将模型与实验进行比较。

结果

使用这个经过验证的模型,我们表明,对于具有均匀分布散射体的样本,除了保持更大的焦点深度外,用锥形波(贝塞尔光束)而不是球形波(高斯光束)照明样本并没有内在的优势。

结论

φMC 可适用于任何照明几何形状、样本特性或光束类型(例如分形或分层散射体分布),因此为厚样本中的光学成像提供了强大的预测工具。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/9f35c2ef6ed7/JBO-026-096004-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/528a10b920e0/JBO-026-096004-g001.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/69d859af3a10/JBO-026-096004-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/0f82201589b7/JBO-026-096004-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/a765b02b866b/JBO-026-096004-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/ea9addada64f/JBO-026-096004-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/87bc21d7db6c/JBO-026-096004-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/b01aa67681a0/JBO-026-096004-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/45b2dd002681/JBO-026-096004-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/1eee9432c636/JBO-026-096004-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/e231828549c8/JBO-026-096004-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/f251b958ff45/JBO-026-096004-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/9f35c2ef6ed7/JBO-026-096004-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/528a10b920e0/JBO-026-096004-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/baaf53b685b1/JBO-026-096004-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/69d859af3a10/JBO-026-096004-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/0f82201589b7/JBO-026-096004-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/a765b02b866b/JBO-026-096004-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/ea9addada64f/JBO-026-096004-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/87bc21d7db6c/JBO-026-096004-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/b01aa67681a0/JBO-026-096004-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/45b2dd002681/JBO-026-096004-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/1eee9432c636/JBO-026-096004-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/e231828549c8/JBO-026-096004-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/f251b958ff45/JBO-026-096004-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/315b/8421375/9f35c2ef6ed7/JBO-026-096004-g013.jpg

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