2017
DOI: 10.1364/ol.42.000362
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Reciprocity relation for the vector radiative transport equation and its application to diffuse optical tomography with polarized light

Abstract: We derive a reciprocity relation for the 3D vector radiative transport equation that describes propagation of polarized light in multiple-scattering media. We then show how this result, together with translational invariance of a plane-parallel sample, can be used to efficiently compute the sensitivity kernel of diffuse optical tomography by Monte Carlo simulations. Numerical examples of polarization-selective sensitivity kernels are given.

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Cited by 15 publications
(18 citation statements)
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“…The Green's function is calculated with N = 10 8 number of photons for a slab of thickness L = 1 * . In addition, the reciprocity relation [26] is applied to the Green's function propagating to the detector (although here we do not consider polarization). Then, an expansion in spherical harmonics of all angularly dependent functions is used; details of angular integration of (10) are explained in Appendix A.…”
Section: Resultsmentioning
confidence: 99%
See 2 more Smart Citations
“…The Green's function is calculated with N = 10 8 number of photons for a slab of thickness L = 1 * . In addition, the reciprocity relation [26] is applied to the Green's function propagating to the detector (although here we do not consider polarization). Then, an expansion in spherical harmonics of all angularly dependent functions is used; details of angular integration of (10) are explained in Appendix A.…”
Section: Resultsmentioning
confidence: 99%
“…We first make use of the reciprocity relation for the Green's function as introduced in Ref. [26] (although here we do not consider polarization). The sensitivity kernel can then be rewritten as As noted in Ref.…”
Section: Appendix: Angular Integrationmentioning
confidence: 99%
See 1 more Smart Citation
“…[18][19][20][21][22][23][24] In some cases, where a linearized approximation is assumed for the inverse problem, the cost of rerunning the forward model can be avoided using techniques such as perturbation Monte Carlo (PMC) methods. 11,25,26 However, for the full nonlinear problem, although PMC can be used for calculation of the problem Jacobian, this has to be recomputed at each iteration of, for example, a Gauss-Newton optimization scheme. 27 In this study, if we are to accept a level of variance and imperfection in our forward/adjoint models, this of course raises the question of how much variance is acceptable in order for SGD to be successful?…”
Section: Stochastic-gradient Descentmentioning
confidence: 99%
“… 18 24 In some cases, where a linearized approximation is assumed for the inverse problem, the cost of rerunning the forward model can be avoided using techniques such as perturbation Monte Carlo (PMC) methods. 11 , 25 , 26 However, for the full nonlinear problem, although PMC can be used for calculation of the problem Jacobian, this has to be recomputed at each iteration of, for example, a Gauss–Newton optimization scheme. 27 …”
Section: Modeling and Inversion Problems In Optical Tomographymentioning
confidence: 99%