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Electromagnetic fields of a massless particle and the eikonal
High Energy Physics - Theory · Submitted 9 Dec 1991
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The exact S-matrix of this reduced theory coincides with the eikonal approximation, and represents the generalisatin to electrodynamics of the approach of 't Hooft and the Verlinde's to Planckian scattering.
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The abstract, sentence by sentence
Electromagnetic fields of a massless charged particle are described by a gauge potential that is almost everywhere pure gauge. Solution of quantum mechanical wave equations in the presence of such fields is therefore immediate and leads to a new derivation of the quantum electrodynamical eikonal approximation. The elctromagnetic action in the eikonal limit is localised on a contour in a two-dimensional Minkowski subspace of four-dimensional space-time. The exact S-matrix of this reduced theory coincides with the eikonal approximation, and represents the generalisatin to electrodynamics of the approach of 't Hooft and the Verlinde's to Planckian scattering.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Electromagnetic fields of a massless charged particle are described by a gauge potential that is almost everywhere pure gauge. | result 0.68 | 0.50 | 0.20 | asserted 1.00 |
| s1 | Solution of quantum mechanical wave equations in the presence of such fields is therefore immediate and leads to a new derivation of the quantum electrodynamical eikonal approximation. | result 0.68 | 0.82 | 0.23 | asserted 1.00 |
| s2 | The elctromagnetic action in the eikonal limit is localised on a contour in a two-dimensional Minkowski subspace of four-dimensional space-time. | result 0.98 | 0.72 | 0.16 | asserted 1.00 |
| s3 | The exact S-matrix of this reduced theory coincides with the eikonal approximation, and represents the generalisatin to electrodynamics of the approach of 't Hooft and the Verlinde's to Planckian scattering. | result 0.72 | 0.77 | 0.59 | asserted 1.00 |
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Original abstract
Electromagnetic fields of a massless charged particle are described by a gauge potential that is almost everywhere pure gauge. Solution of quantum mechanical wave equations in the presence of such fields is therefore immediate and leads to a new derivation of the quantum electrodynamical eikonal approximation. The elctromagnetic action in the eikonal limit is localised on a contour in a two-dimensional Minkowski subspace of four-dimensional space-time. The exact S-matrix of this reduced theory coincides with the eikonal approximation, and represents the generalisatin to electrodynamics of the approach of 't Hooft and the Verlinde's to Planckian scattering.
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References
How the literature uses it
23 arXiv papers cite this in 37 sentences
Papers citing it · 29 sentences without a confident label
Compares with it 1 paper
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Our $A_1,c^-$ is almost the solution written in [ref] and (2.24) of [ref] (see also [ref] ).
Do null defects dream of conformal symmetry? · Direct Solution for the Massless Charged Particle · 0.99
Cites it as background 6 papers
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While the solution of the scalar wave equations in electromagnetic (and gravitational) shockwaves [ref] is well-covered in the literature (cf., [ref] ), the Dirac equation is less commonly studied (though see [ref] for the eikonal calculation).
Particle-beam scattering from strong-field QED · Fermion wavefunctions on ultraboosted beam backgrounds · 0.90
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Simplifications arise under assumptions such as small momentum exchange, ultrarelativistic limits or a perturbative description of the background (e.g., [ref] ).
Scattering amplitudes for self-force · Semiclassical scalar wavefunctions & elastic scattering · 0.82
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The problem of electromagnetic radiation from massless charges was considered in [ref] in the framework of classical electrodynamics.
On the creation of charged massless fermion pair by a photon in crossed electromagnetic field · Introduction · 0.98
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