2001
DOI: 10.1103/physrevd.63.125022
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Hard thermal loops and beyond in the finite temperature world-line formulation of QED

Abstract: We derive the hard thermal loop action for soft electromagnetic fields in the finite temperature world-line formulation at imaginary time, by first integrating out the hard fermion modes from the microscopic QED action. Further, using the finite T world-line method, we calculate all static higher order terms in the soft electromagnetic field. At high T , the leading non-linear terms are independent of the temperature and, except for a term quartic in the time component of the vector potential, they cancel exac… Show more

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Cited by 11 publications
(5 citation statements)
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“…During the last two decades, these "string-inspired" representations have already found a considerable number of applications in QED, both for the calculation of photon amplitudes [8,14,23] and the effective action itself [24][25][26][27][28]. They have been generalised to include constant external fields [23,[29][30][31][32][33] as well as finite temperature [34][35][36][37][38][39]. Their…”
Section: Jhep08(2020)018mentioning
confidence: 99%
“…During the last two decades, these "string-inspired" representations have already found a considerable number of applications in QED, both for the calculation of photon amplitudes [8,14,23] and the effective action itself [24][25][26][27][28]. They have been generalised to include constant external fields [23,[29][30][31][32][33] as well as finite temperature [34][35][36][37][38][39]. Their…”
Section: Jhep08(2020)018mentioning
confidence: 99%
“…For the case of worldline path integrals on the circle, i.e. with periodic boundary conditions, several applications soon followed these papers, ranging from multiloop calculations [6], finite temperature computations [7,8], the inclusion of constant external electromagnetic fields [9][10][11] and Heisenberg-Euler lagrangians [12], and many more. Worldline path integrals on the line were used instead to compute, for instance, thermal Green's functions [13], to represent scalar and Dirac propagators [14,15], as well as open line spin factors [16], and more recently in the worldgraph approach [17,18] and to obtain master formulas from the photon-dressed Dirac propagators [19]-see the review papers [20,21] for an extensive bibliography and a summary of classic and more recent applications.…”
Section: Introductionmentioning
confidence: 99%
“…For the case of worldline path integrals on the circle, i.e. with periodic boundary conditions, several applications soon followed these papers, ranging from multiloop calculations [6], finite temperature computations [7,8], the inclusion of constant external electromagnetic fields [9][10][11] and Heisenberg-Euler lagrangians [12], and many more. Worldline path integrals on the line were used instead to compute, for instance, thermal Green's functions [13], to represent scalar and Dirac propagators [14,15], as well as open line spin factors [16], and more recently in the worldgraph approach [17,18] and to obtain master formulas from the photon-dressed Dirac propagators [19]-see the review papers [20,21] for an extensive bibliography and a summary of classic and more recent applications.…”
Section: Introductionmentioning
confidence: 99%