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Wave propagation in complex coordinates

Classical Physics · Submitted 17 Jul 2015

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim Extending this property to all angles of incidence leads us to a generalized form of the Poschl Teller potentials.

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arXiv ID1508.04461 (version 1)
Pith IDAIJEEYLE, Pith's permanent record of this paper and its review
CitationC. G. King, S. A. R. Horsley, T. G. Philbin. "Wave propagation in complex coordinates." arXiv:1508.04461 (2015). https://pith.science/paper/AIJEEYLE
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What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.33 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.05 · compares with prior results 0.33 · mentions code or data availability 0.01.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

We investigate the analytic continuation of wave equations into the complex position plane. For the particular case of electromagnetic waves we provide a physical meaning for such an analytic continuation in terms of a family of closely related inhomogeneous media. For bounded permittivity profiles we find the phenomenon of reflection can be related to branch cuts in the wave that originate from poles of the permittivity at complex positions. Demanding that these branch cuts disappear, we derive a large family of inhomogeneous media that are reflectionless for a single angle of incidence. Extending this property to all angles of incidence leads us to a generalized form of the Poschl Teller potentials. We conclude by analyzing our findings within the phase integral (WKB) method.

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#sentencerolethe authors' own workstates the main conclusionstrength
s0 We investigate the analytic continuation of wave equations into the complex position plane. contribution 0.98 0.92 0.04 asserted 0.86
s1 For the particular case of electromagnetic waves we provide a physical meaning for such an analytic continuation in terms of a family of closely related inhomogeneous media. interpretation 0.70 0.92 0.08 asserted 1.00
s2 For bounded permittivity profiles we find the phenomenon of reflection can be related to branch cuts in the wave that originate from poles of the permittivity at complex positions. result 0.96 0.92 0.10 asserted 1.00
s3 Demanding that these branch cuts disappear, we derive a large family of inhomogeneous media that are reflectionless for a single angle of incidence. result 0.77 0.94 0.17 asserted 1.00
s4 Extending this property to all angles of incidence leads us to a generalized form of the Poschl Teller potentials. result 0.93 0.91 0.37 asserted 1.00
s5 We conclude by analyzing our findings within the phase integral (WKB) method. method 0.55 0.90 0.26 asserted 0.68

What kind of paper the classifier reports this is: theoretical result 0.99 · evidence from proof or derivation 1.00.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

We investigate the analytic continuation of wave equations into the complex position plane. For the particular case of electromagnetic waves we provide a physical meaning for such an analytic continuation in terms of a family of closely related inhomogeneous media. For bounded permittivity profiles we find the phenomenon of reflection can be related to branch cuts in the wave that originate from poles of the permittivity at complex positions. Demanding that these branch cuts disappear, we derive a large family of inhomogeneous media that are reflectionless for a single angle of incidence. Extending this property to all angles of incidence leads us to a generalized form of the Poschl Teller potentials. We conclude by analyzing our findings within the phase integral (WKB) method.

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3 arXiv papers cite this in 11 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 6 sentences without a confident label

Uses its method or tool 2 papers
  • The generalized reflection and transmission coefficients are then given by [equation] Integrating formally both sides of Eq.(19) from $-∞$ to $∞$ and using Eqs.(20) and (22), one can write [equation] Note that, as compared to more conventional WKB analysis of Ref. [ref] , following Ref. [ref] we use for the asymptotic states the expression (9) , which offers the advantage of avoiding branch cuts arising form square root of the potential and simplifies the analysis when extending the equations into the complex plane.

    Wave reflection in dielectric media obeying spatial Kramers-Kronig relations · 3. One-way reflectionless property of Kramers-Kronig dielectric media · 0.82

  • For perpendicular incidence we do not need to distinguish between two independent polarizations of the wave and we can consider the scalar Helmholtz equation [equation] A simple method of generating materials that do not reflect from one side (utilized in [ref] , for example) is to write down an expression for $E(x,ω)$ that for $x→±∞$ becomes a plane wave moving to the right (or left).

    All-frequency reflectionlessness · Introduction · 0.86

Cites it as background 3 papers
  • In a recent work, Horsley et al. introduced the idea of spatial KK relations in planar inhomogeneous dielectric media [ref] (see also Ref. [ref] ).

    Wave reflection in dielectric media obeying spatial Kramers-Kronig relations · 1. Introduction · 0.96

  • Recent work [ref] has shown that complex inhomogenous media satisfying the spatial Kramers–Kronig relations have curious scattering properties, being generally reflectionless from one side and in many cases having unit transmission.

    The KdV hierarchy in optics · Kramers–Kronig media · 0.86

  • The question of what governs reflection is subtle and a completely general answer is still elusive [ref] .

    All-frequency reflectionlessness · Introduction · 0.92

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