2020
DOI: 10.1007/978-3-030-48634-1_8
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Reconstructing the Optical Parameters of a Layered Medium with Optical Coherence Elastography

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Cited by 3 publications
(5 citation statements)
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“…Because of the linearity of the equation it is sufficient to solve the problem for every plane wave. The result for these backscattered fields for such a sample is well known in this plane wave case, see [ 25 , 26 ]. For the simplest case we consider an (arbitrary) plane wave as incident illumination from the top, with amplitude function and propagation vector which we consider implicitly as a function of and We obtain the reflected electric field where denotes an arbitrary point of the top boundary (that is ) of the object, the wave vector and the sum of the reflection coefficients of the differently polarized parts …”
Section: Mathematical Modelmentioning
confidence: 80%
See 1 more Smart Citation
“…Because of the linearity of the equation it is sufficient to solve the problem for every plane wave. The result for these backscattered fields for such a sample is well known in this plane wave case, see [ 25 , 26 ]. For the simplest case we consider an (arbitrary) plane wave as incident illumination from the top, with amplitude function and propagation vector which we consider implicitly as a function of and We obtain the reflected electric field where denotes an arbitrary point of the top boundary (that is ) of the object, the wave vector and the sum of the reflection coefficients of the differently polarized parts …”
Section: Mathematical Modelmentioning
confidence: 80%
“…For such a multi-layer structure, at least locally in the illuminated spot, the depth-dependent refractive index can be simplified to a piecewise constant function. The corresponding inverse problem has been examined in [3,8,26] and in [9] where additional inclusions have been discussed.…”
Section: Introductionmentioning
confidence: 99%
“…Because of the linearity of the equation it is sufficient to solve the problem for every plane wave. The result for these backscattered fields for such a sample is well known in this plane wave case, see [15,8]. For the simplest case L = 1, we consider an (arbitrary) plane wave as incident illumination from the top,…”
Section: The Sample Fieldmentioning
confidence: 97%
“…We additionally assign to every layer Ω j its width, which is given by the positive real number d j = a j − a j+1 . The light E : R × R 3 → C 3 in the presence of the sample, equation (7), is then modeled as a solution of the vectorial Helmholtz equation for all x ∈ R 3 :…”
Section: Light Scatteringmentioning
confidence: 99%
“…For such a multi-layer structure, at least locally in the illuminated spot, the depth-dependent refractive index can be simplified to a piecewise constant function. The corresponding inverse problem has been examined in [1,6,20] and in [7] where additional inclusions have been discussed.…”
Section: Introductionmentioning
confidence: 99%