Abstract:In the last decade, consistent and successful innovations have been achieved in the field of lasers and optics, collectively known as ‘photonics’, founding new applications in biomedicine, including clinical biopsy. Non-invasive photonics-based diagnostic modalities are rapidly expanding, and with their exponential improvement, there is a great potential to develop practical instrumentation for automatic detection and identification of different types and/or sub-types of diseases at a very early stage. While u… Show more
“… 10 – 14 In biophotonics, MC methods, such as MCML, 15 created by L. Wang and S. Jacques, were originally designed to simulate scalar light transport within turbid scattering medium 16 , 17 and were fundamentally relying on the radiative transfer equation (RTE). 18 – 20 As significant role of polarized light in extending diagnostic capabilities of biomedical tools became apparent, 21 , 22 MC methods evolved accordingly resulting in many practical and popular tools particularly developed by Ramella-Roman, Prahl, and Jacques, 23 , 24 Hielscher, 25 , 26 Wang, 27 and Xu. 28 Fundamental ground for these polarized MC approaches was established by the vector radiative transfer equation (VRTE), which represents a system of equations for each Stokes parameter and can be rigorously derived from the Maxwell electromagnetic theory.…”
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Significance
Phase retardation of circularly polarized light (CPL), backscattered by biological tissue, is used extensively for quantitative evaluation of cervical intraepithelial neoplasia, presence of senile Alzheimer’s plaques, and characterization of biotissues with optical anisotropy. The Stokes polarimetry and Mueller matrix approaches demonstrate high potential in definitive non-invasive cancer diagnosis and tissue characterization. The ultimate understanding of CPL interaction with tissues is essential for advancing medical diagnostics, optical imaging, therapeutic applications, and the development of optical instruments and devices.
Aim
We investigate propagation of CPL within turbid tissue-like scattering medium utilizing a combination of Jones and Stokes–Mueller formalisms in a Monte Carlo (MC) modeling approach. We explore the fundamentals of CPL memory effect and depolarization formation.
Approach
The generalized MC computational approach developed for polarization tracking within turbid tissue-like scattering medium is based on the iterative solution of the Bethe–Salpeter equation. The approach handles helicity response of CPL scattered in turbid medium and provides explicit expressions for assessment of its polarization state.
Results
Evolution of CPL backscattered by tissue-like medium at different conditions of observation in terms of source–detector configuration is assessed quantitatively. The depolarization of light is presented in terms of the coherence matrix and Stokes–Mueller formalism. The obtained results reveal the origins of the helicity flip of CPL depending on the source–detector configuration and the properties of the medium and are in a good agreement with the experiment.
Conclusions
By integrating Jones and Stokes–Mueller formalisms, the combined MC approach allows for a more complete representation of polarization effects in complex optical systems. The developed model is suitable to imitate propagation of the light beams of different shape and profile, including Gaussian, Bessel, Hermite–Gaussian, and Laguerre–Gaussian beams, within tissue-like medium. Diverse configuration of the experimental conditions, coherent properties of light, and peculiarities of polarization can be also taken into account.
“… 10 – 14 In biophotonics, MC methods, such as MCML, 15 created by L. Wang and S. Jacques, were originally designed to simulate scalar light transport within turbid scattering medium 16 , 17 and were fundamentally relying on the radiative transfer equation (RTE). 18 – 20 As significant role of polarized light in extending diagnostic capabilities of biomedical tools became apparent, 21 , 22 MC methods evolved accordingly resulting in many practical and popular tools particularly developed by Ramella-Roman, Prahl, and Jacques, 23 , 24 Hielscher, 25 , 26 Wang, 27 and Xu. 28 Fundamental ground for these polarized MC approaches was established by the vector radiative transfer equation (VRTE), which represents a system of equations for each Stokes parameter and can be rigorously derived from the Maxwell electromagnetic theory.…”
.
Significance
Phase retardation of circularly polarized light (CPL), backscattered by biological tissue, is used extensively for quantitative evaluation of cervical intraepithelial neoplasia, presence of senile Alzheimer’s plaques, and characterization of biotissues with optical anisotropy. The Stokes polarimetry and Mueller matrix approaches demonstrate high potential in definitive non-invasive cancer diagnosis and tissue characterization. The ultimate understanding of CPL interaction with tissues is essential for advancing medical diagnostics, optical imaging, therapeutic applications, and the development of optical instruments and devices.
Aim
We investigate propagation of CPL within turbid tissue-like scattering medium utilizing a combination of Jones and Stokes–Mueller formalisms in a Monte Carlo (MC) modeling approach. We explore the fundamentals of CPL memory effect and depolarization formation.
Approach
The generalized MC computational approach developed for polarization tracking within turbid tissue-like scattering medium is based on the iterative solution of the Bethe–Salpeter equation. The approach handles helicity response of CPL scattered in turbid medium and provides explicit expressions for assessment of its polarization state.
Results
Evolution of CPL backscattered by tissue-like medium at different conditions of observation in terms of source–detector configuration is assessed quantitatively. The depolarization of light is presented in terms of the coherence matrix and Stokes–Mueller formalism. The obtained results reveal the origins of the helicity flip of CPL depending on the source–detector configuration and the properties of the medium and are in a good agreement with the experiment.
Conclusions
By integrating Jones and Stokes–Mueller formalisms, the combined MC approach allows for a more complete representation of polarization effects in complex optical systems. The developed model is suitable to imitate propagation of the light beams of different shape and profile, including Gaussian, Bessel, Hermite–Gaussian, and Laguerre–Gaussian beams, within tissue-like medium. Diverse configuration of the experimental conditions, coherent properties of light, and peculiarities of polarization can be also taken into account.
“…Polarimetry is gaining popularity due to its unique capacity to collect microstructural and optical information from tissue samples label-freely [1][2][3][4]. The Mueller matrix (MM) imaging method, as one of the available polarimetric techniques, can thoroughly characterize the polarization-related properties of media, such as diattenuation, retardance, and depolarization, which are crucial in biomedical studies and clinical trials [5][6][7].…”
Backscattering polarimetry can detect substantial microstructure information of media label-freely. Among the available polarimetric techniques, the backscattering Mueller matrix polarimetry provides a promising non-contact and quantitative tool for in-vivo tissue detection and clinical diagnosis. To eliminate the surface reflection from the sample cost-effectively, the non-collinear backscattering Mueller matrix imaging setup always has an oblique incidence. Meanwhile, for practical organ cavities imaged using polarimetric gastrointestinal endoscopy, the uneven tissue surfaces can induce various relative oblique incidences inevitably, which can affect the polarimetry in a complicated manner and needs to be considered for detailed study. Therefore, it is a critical issue to figure out the influence from oblique incidence on backscattering tissue polarimetry. To systematically analyze such the influence, we measured the Mueller matrices of experimental phantom and ex-vivo tissues with different incident angles, adopted a Monte Carlo simulation program based on cylindrical scattering model for further verification and analysis. Meanwhile, the results were quantitively evaluated using the Fourier transform, basic statistics and frequency distribution histograms. Both the experimental and simulated results demonstrate that, oblique incidence can induce different variations on non-periodic, two-periodic and four-periodic Mueller matrix elements, leading to false-positive and false-negative polarization information for tissue polarimetry. Moreover, a prominent oblique incidence can bring more dramatic signal variations such as phase drift and element transposition. The findings presented in this study give some crucial criterions of appropriate incident angle selections for in-vivo polarimetric endoscopy and other applications, and can also be valuable references for studying how to minimize the influence furtherly.
“…In the biomedical field, it has been proposed as a marker to identify cancerous tissue in its early stages [5]. In the ophthalmic field, researchers combine polarization with OCT techniques for retinal imaging implementations [6,7].…”
Section: Introductionmentioning
confidence: 99%
“…Retardance represents the phase variation dependence where its circularity is useful for glucose measurements, and its linearity is associated with stress analysis. Depolarization is the ability to maintain the polarization properties of the light, and its commonly used for cancer detection [5][6][7].…”
In this research, we propose a demodulation algorithm for the dual rotation polarizer-analyzer polarimeter. The proposal retrieves the partial Mueller matrix from the complex coefficients, theoretically calculated from the Fourier transform of the output intensity. As calibration parameters, the initial orientations of the polarizer-analyzer are used. Experimental results for air and a rotating dichroic film polarizer show our proposal's feasibility.
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