dorsal/arxiv
View SchemaPropagation of an electromagnetic pulse through a waveguide with a barrier: A time domain solution within classical electrodynamics
| Authors | Thorsten Emig |
|---|---|
| Categories | |
| ArXiv ID | physics/9711017 |
| URL | https://arxiv.org/abs/physics/9711017 |
| DOI | 10.1103/PhysRevE.54.5780 |
| Journal | Phys. Rev. E 54, 5780 (1996) |
Abstract
An electromagnetic truncated Gaussian pulse propagates through a waveguide with piecewise different dielectric constants. The waveguide contains a barrier, namely a region of a lower dielectric constant compared to the neighboring regions. This set-up yields a purely imaginary wave vector in the region of the barrier ('electromagnetic tunneling'). We exactly calculate the time-dependent Green's function for a slightly simplified dispersion relation. In order to observe the plain tunneling effect we neglect the distortions caused by the wave guide in obtaining the transmitted pulse. The wave front of the pulse travels with the vacuum speed of light. Nevertheless, behind the barrier, the maximum of the transmitted pulse turns up at an earlier time than in the case without an barrier. This effect will be explained in terms of the energy flow across the barrier. The solutions obtained reproduce the shape of the pulses measured in the tunneling experiments of Enders and Nimtz [J. Phys. (France) I2, 1693 (1992); Phys. Rev. E48, 632 (1993); Phys. Rev. B47, 9605 (1993); J. Phys. (France) I3, 1089 (1993); 4, 565 (1994)].
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"abstract": "An electromagnetic truncated Gaussian pulse propagates through a waveguide\nwith piecewise different dielectric constants. The waveguide contains a\nbarrier, namely a region of a lower dielectric constant compared to the\nneighboring regions. This set-up yields a purely imaginary wave vector in the\nregion of the barrier (\u0027electromagnetic tunneling\u0027). We exactly calculate the\ntime-dependent Green\u0027s function for a slightly simplified dispersion relation.\nIn order to observe the plain tunneling effect we neglect the distortions\ncaused by the wave guide in obtaining the transmitted pulse. The wave front of\nthe pulse travels with the vacuum speed of light. Nevertheless, behind the\nbarrier, the maximum of the transmitted pulse turns up at an earlier time than\nin the case without an barrier. This effect will be explained in terms of the\nenergy flow across the barrier. The solutions obtained reproduce the shape of\nthe pulses measured in the tunneling experiments of Enders and Nimtz [J. Phys.\n(France) I2, 1693 (1992); Phys. Rev. E48, 632 (1993); Phys. Rev. B47, 9605\n(1993); J. Phys. (France) I3, 1089 (1993); 4, 565 (1994)].",
"arxiv_id": "physics/9711017",
"authors": [
"Thorsten Emig"
],
"categories": [
"physics.class-ph",
"cond-mat"
],
"doi": "10.1103/PhysRevE.54.5780",
"journal_ref": "Phys. Rev. E 54, 5780 (1996)",
"title": "Propagation of an electromagnetic pulse through a waveguide with a barrier: A time domain solution within classical electrodynamics",
"url": "https://arxiv.org/abs/physics/9711017"
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