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On the QED Effective Action in Time Dependent Electric Backgrounds

High Energy Physics - Theory · Submitted 3 Jul 1998

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

The authors' main claim This expression is remarkably similar in form to Schwinger's classic result for the constant electric background.

how it is stated · asserted 1.00 read the record →

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arXiv IDhep-th/9807031 (version 2)
Pith IDGKI5QEVA, Pith's permanent record of this paper and its review
CitationGerald Dunne, Theodore Hall (U. Connecticut). "On the QED Effective Action in Time Dependent Electric Backgrounds." arXiv:hep-th/9807031 (1998). https://pith.science/paper/GKI5QEVA
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What the abstract itself states, as probabilities: claims first 0.08 · states limitation 0.12 · human participants 0.01 · controlled comparison 0.05 · randomized assignment 0.01 · states quantitative result 0.05 · compares with prior results 0.95 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v2. Results and the main claim are underlined; .

We apply the resolvent technique to the computation of the QED effective action in time dependent electric field backgrounds. The effective action has both real and imaginary parts, and the imaginary part is related to the pair production probability in such a background. The resolvent technique has been applied previously to spatially inhomogeneous magnetic backgrounds, for which the effective action is real. We explain how dispersion relations connect these two cases, the magnetic case which is essentially perturbative in nature, and the electric case where the imaginary part is nonperturbative. Finally, we use a uniform semiclassical approximation to find an expression for very general time dependence for the background field. This expression is remarkably similar in form to Schwinger's classic result for the constant electric background.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 We apply the resolvent technique to the computation of the QED effective action in time dependent electric field backgrounds. contribution 0.79 0.95 0.07 asserted 1.00
s1 The effective action has both real and imaginary parts, and the imaginary part is related to the pair production probability in such a background. background 0.86 0.18 0.08 asserted 1.00
s2 The resolvent technique has been applied previously to spatially inhomogeneous magnetic backgrounds, for which the effective action is real. background 1.00 0.04 0.02 asserted 1.00
s3 We explain how dispersion relations connect these two cases, the magnetic case which is essentially perturbative in nature, and the electric case where the imaginary part is nonperturbative. contribution 0.77 0.76 0.11 asserted 1.00
s4 Finally, we use a uniform semiclassical approximation to find an expression for very general time dependence for the background field. method 0.63 0.96 0.21 asserted 1.00
s5 This expression is remarkably similar in form to Schwinger's classic result for the constant electric background. result 0.80 0.89 0.41 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 0.98 · 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 apply the resolvent technique to the computation of the QED effective action in time dependent electric field backgrounds. The effective action has both real and imaginary parts, and the imaginary part is related to the pair production probability in such a background. The resolvent technique has been applied previously to spatially inhomogeneous magnetic backgrounds, for which the effective action is real. We explain how dispersion relations connect these two cases, the magnetic case which is essentially perturbative in nature, and the electric case where the imaginary part is nonperturbative. Finally, we use a uniform semiclassical approximation to find an expression for very general time dependence for the background field. This expression is remarkably similar in form to Schwinger's classic result for the constant electric background.

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References
How the literature uses it

10 arXiv papers cite this in 10 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 · 5 sentences without a confident label

Compares with it 1 paper
Cites it as background 4 papers
  • Such investigations were undertaken in a series of works developing exact methods for evaluating quantum effective actions in solvable electromagnetic backgrounds [ref] .

    QCD Vacuum in an Inhomogeneous Magnetic Field · Introduction · 0.83

  • Apart from this, higher-loop results in constant fields and lower space-time dimensions [ref] , as well as one-loop results for specific purely electric or magnetic (one-dimensional) field inhomogeneities are available [ref] .

    Derivative corrections to the Heisenberg-Euler effective action · Introduction · 0.99

  • This can happen either thanks to some time-dependent potential [ref] (e.g. a scattering process or the Schwinger effect) or to some dynamical background geometry (e.g. an expanding universe [ref] or a collapsing black hole [ref] ).

    Is the information loss problem a paradox? · Particle creation · 0.82

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