2015
DOI: 10.1007/978-3-319-21045-2_18
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Extreme Waves and Branching Flows in Optical Media

Abstract: We address light propagation properties in complex media consisting of random distributions of lenses that have specific focusing properties. We present both analytical and numerical techniques that can be used to study emergent properties of light organization in these media. As light propagates, it experiences multiple scattering leading to the formation of light bundles in the form of branches; these are random yet occur systematically in the the medium, particularly in the weak scattering limit. On the oth… Show more

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Cited by 7 publications
(7 citation statements)
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References 40 publications
(147 reference statements)
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“…This special characteristic of the Luneburg lens can be analyzed by using geometrical optics based on Fermat's principle [37]. For this purpose, a quasi-two-dimensional (2D) ray solution is conducted by using the 2D medium which has the same index distribution characteristic as Luneburg lenses [38]. By combining Fermat's principle with the Lagrangian optics, the ray tracing equation for a single Luneburg lens can be represented as follows [39][40][41]:…”
Section: Ray-theory Model Of the Cloaking By Luneburg Lensmentioning
confidence: 99%
See 1 more Smart Citation
“…This special characteristic of the Luneburg lens can be analyzed by using geometrical optics based on Fermat's principle [37]. For this purpose, a quasi-two-dimensional (2D) ray solution is conducted by using the 2D medium which has the same index distribution characteristic as Luneburg lenses [38]. By combining Fermat's principle with the Lagrangian optics, the ray tracing equation for a single Luneburg lens can be represented as follows [39][40][41]:…”
Section: Ray-theory Model Of the Cloaking By Luneburg Lensmentioning
confidence: 99%
“…Since the refractive index distribution of the Luneburg lens is a function of r, so differential length ds can be rewritten as ds = Here, the shortest path that is followed by a light ray according to Fermat's principle can be obtained by the minimization of the integral of (A2). In this regard, to obtain the derivative of (A2), the Euler-Lagrange equation can be used where the Lagrangian is L(ϕ, φ, r) = n(r) 1 + r 2 φ2 [38,41]:…”
Section: Appendix: Derivation Of Ray Trajectory Equationmentioning
confidence: 99%
“…The general demonstration of the equivalence between classical and wave-mechanical Helmholtz-like equations and exact, trajectory-based Hamiltonian systems was given in Refs. [23] [24] [25] [26] [27], and led to extensive application both in relativistic electrodynamics and in the analysis of experimental arrangements and devices employed for light transmission and guiding [28] [29] [30]. Let us finally remind that the equivalence between the time-dependent Schrödinger equation and Hamiltonian Me-Journal of Applied Mathematics and Physics chanics was demonstrated in Ref.…”
Section: An Experimentally Tested Hamiltonian Description Of Wave-likmentioning
confidence: 99%
“…The light branching is attributed to variations of the film's refractivity, which bends and bundles the light rays at favorable locations and form caustics [21]. Despite its complexity, branched flow is usually a linear phenomenon [22] and the distance d 0 from the source to the first branching point follows the scaling 18,23], where l c is the correlation length of the medium's unevenness, and v 0 is a strength parameter (to be defined later).…”
mentioning
confidence: 99%