2002
DOI: 10.1088/1464-4258/4/3/313
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Coherent backscattering of turbid samples containing large Mie spheres

Abstract: We found that the coherent backscattering cone of turbid samples containing spherical Mie scatterers with a size parameter larger than about 20 strongly deviates from known analytical curve shapes. We compare experimental data with numerical simulations of Monte Carlo type. Moreover, we present a new wide-angle coherent backscattering setup .

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Cited by 33 publications
(20 citation statements)
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“…8,27,28,42,43 Using this method, a portion of scattered intensity is collected after a photon reaches each new position within the medium. This "partial photon" intensity I partial is calculated by multiplying the probability that the photon is scattered in the direction of the surface Fðθ s ; 0Þ by the probability that it will reach surface according to the Beer-Lambert law e −ðμ s þμ a Þz :…”
Section: Semi-analytical Approachmentioning
confidence: 99%
See 1 more Smart Citation
“…8,27,28,42,43 Using this method, a portion of scattered intensity is collected after a photon reaches each new position within the medium. This "partial photon" intensity I partial is calculated by multiplying the probability that the photon is scattered in the direction of the surface Fðθ s ; 0Þ by the probability that it will reach surface according to the Beer-Lambert law e −ðμ s þμ a Þz :…”
Section: Semi-analytical Approachmentioning
confidence: 99%
“…Of particular importance for this paper are CBS codes that have been developed to model and calculate tissue optical properties, 18,23,24 electric field tracking codes, 25,26 and codes that implement the semi-analytical approach (also known as the partial photon technique). 8,27,28 In this paper, we have developed a polarized light Monte Carlo algorithm written in the C programming language that tracks the progression of the electric field in scattering and absorbing media containing birefringent materials. This code enables the modeling of tissue as a statistically homogeneous continuous random media under the Whittle-Matérn model or as a composition of discrete spherical scatterers under Mie theory.…”
Section: Introductionmentioning
confidence: 99%
“…A diffusive approximating is applicable when it is possible to neglect an absorption and when a thickness of sample is much greater than the transport path length of photons [7][8][9]. In this case, the radiation transfer can be described by the diffusion …”
Section: Discussionmentioning
confidence: 99%
“…This problem can be avoided by using a movable fiber, which scans the angular dependence of the backscattered light. 11,12 In this case, care has to be taken that the recorded light always passes the polarization filter ͑and QWP, see below͒ at right angles, such that singly scattered light can be efficiently and homogeneously reduced. Otherwise the polarization properties will change, leading to a misestimation of the incoherent background and hence a distortion of the CBC.…”
Section: B Former Setup Designsmentioning
confidence: 99%
“…10,12 Our setup uses a lens with a focal distance of 0.1 m which is also the distance between the lens and the CCD chip. The CCD chip has a resolution of 512 ϫ 512 pixels, which in this setup results in an angular resolution of 0.012°over a range of ±3°.…”
Section: -4mentioning
confidence: 99%