Low-frequency scattering defined by the Helmholtz equation in one
dimension
- URL: http://arxiv.org/abs/2105.07895v1
- Date: Fri, 14 May 2021 11:58:01 GMT
- Title: Low-frequency scattering defined by the Helmholtz equation in one
dimension
- Authors: Farhang Loran and Ali Mostafazadeh
- Abstract summary: The Helmholtz equation in one dimension describes the propagation of electromagnetic waves in effectively one-dimensional systems.
The fact that the potential term entering the latter is energy-dependent obstructs the application of the results on low-energy quantum scattering.
We use a recently developed dynamical formulation of stationary scattering to offer a comprehensive treatment of the low-frequency scattering of these waves for a general finite-range scatterer.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: The Helmholtz equation in one dimension, which describes the propagation of
electromagnetic waves in effectively one-dimensional systems, is equivalent to
the time-independent Schr\"odinger equation. The fact that the potential term
entering the latter is energy-dependent obstructs the application of the
results on low-energy quantum scattering in the study of the low-frequency
waves satisfying the Helmholtz equation. We use a recently developed dynamical
formulation of stationary scattering to offer a comprehensive treatment of the
low-frequency scattering of these waves for a general finite-range scatterer.
In particular, we give explicit formulas for the coefficients of the
low-frequency series expansion of the transfer matrix of the system which in
turn allow for determining the low-frequency expansions of its reflection,
transmission, and absorption coefficients. Our general results reveal a number
of interesting physical aspects of low-frequency scattering particularly in
relation to permittivity profiles having balanced gain and loss.
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