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Lecture 4
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statistical description
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stochastic equation is a random function
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Parabolic (paraxial) approximation
< > < > Small Perturbations; Local Perturbations; Smooth Perturbations; Path Integral Feynman diagrams Fokker-Plank Equation Random Matrix Theory Supersymmetry Parabolic (paraxial) approximation
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propagator
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< > < > < > < > < >
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1 2 3
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single scattering (first Born) approximation
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random function < > < >
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in the far zone
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far zone
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resonant Bragg scattering
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V energy flux density Differential SCS
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Total SCS
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INVERSE PROBLEM
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energy conservation
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energy conservation ?
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Extinction Length energy conservation !
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small perturbation, weak total scattering
(Energy of the scattered field) (Energy of the incident field)
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smooth perturbations is not necessarily small new small parameter
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Parabolic Approximation
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Parabolic Equation
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forward scattering backscattering
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small angle of scattering
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Geometrical Optics
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eikonal amplitude
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Phase fluctuations
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Amplitude fluctuations
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Multiple scattering! Compare to the result of the first Born approximation (single scattering) Gaussian random function
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Transverse Ray Deflection
Optical Magnus effect Transverse Ray Deflection POLARIZATION helicity
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there is neither no polarization in the equations of rays
helicity
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Transverse Ray Deflection
linear polarization
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Limits of validity of GO approximation
rays, no diffraction
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Multiple scattering
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<….……………………………… >
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odd even Gaussian
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