2012
DOI: 10.1103/physrevd.86.125007
|View full text |Cite|
|
Sign up to set email alerts
|

Pair production in a plane wave by thermal background photons

Abstract: Ever since Schwinger published his influential paper [ J. Schwinger Phys. Rev. 82 664 (1951)], the maxim that there can be no pair creation in a plane wave has been often cited. We advance an analysis that indicates that in any real situation, where thermal effects are present, in a single plane-wave field, even in the limit of zero frequency (a constant crossed field), thermal photons can seed pair creation. Interestingly, the pair-production rate is found to depend nonperturbatively on both the amplitude of … Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
15
0

Year Published

2013
2013
2023
2023

Publication Types

Select...
8
1

Relationship

1
8

Authors

Journals

citations
Cited by 27 publications
(15 citation statements)
references
References 29 publications
0
15
0
Order By: Relevance
“…Above the kinematic threshold this process has cross section approximately equal to the classical size of the electron, σ BW ∼ e 4 /(16π 2 m 2 e ). Averaging this over the distribution of energies present in a thermal bath of photons one finds [77],…”
Section: Electrons and Positronsmentioning
confidence: 99%
“…Above the kinematic threshold this process has cross section approximately equal to the classical size of the electron, σ BW ∼ e 4 /(16π 2 m 2 e ). Averaging this over the distribution of energies present in a thermal bath of photons one finds [77],…”
Section: Electrons and Positronsmentioning
confidence: 99%
“…For weak coupling much has been done to generalise Schwinger's original result, including the effect of temporal and spatial variation in the external field [2][3][4][5][6][7][8][9]; the presence of an additional high energy photon or other particle [10][11][12][13][14]; a finite temperature [15][16][17][18][19][20][21][22][23][24]; higher loops [25][26][27][28][29] and back reaction [30][31][32][33][34]. However, at stronger coupling, where perturbation theory breaks down, much less is known.…”
Section: Introductionmentioning
confidence: 99%
“…This is true even in the long-wavelength limit, λmc/ → ∞, showing the collective, nonperturbative nature of the phenomenon. In this case, the Breit-Wheeler rate is additively enhanced by [53], This result is valid for k B T E/(mc 2 E c ) 1. The crucial difference from that of a constant electric field is that the electromagnetic invariant E 2 − c 2 B 2 of a plane wave vanishes.…”
Section: Theoretical Resultsmentioning
confidence: 64%