1990
DOI: 10.1016/0550-3213(90)90508-b
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Soft amplitudes in hot gauge theories: A general analysis

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Cited by 1,213 publications
(1,248 citation statements)
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“…2 (right). Both results are compared to a dilepton spectrum calculated within the hard thermal loop approximation [13]. In the limit of vanishing ω one can read of the electrical conductivity (2.7) from Fig.…”
Section: Results For Correlators and Spectral Function Fitsmentioning
confidence: 99%
“…2 (right). Both results are compared to a dilepton spectrum calculated within the hard thermal loop approximation [13]. In the limit of vanishing ω one can read of the electrical conductivity (2.7) from Fig.…”
Section: Results For Correlators and Spectral Function Fitsmentioning
confidence: 99%
“…of the kinetic equation (6.14) in terms of HTL-amplitudes [9,27,28]. Actually, by the definition of theΣ-function (5.9) the coefficient in front of…”
Section: Htl-amplitudesmentioning
confidence: 99%
“…(25)- (26)) would break gauge invariance in a gauge theory. As is well-known from the Ward identities for Hard Thermal Loops (HTLs) [39,40], both propagators and vertices must be HTL resummed to preserve gauge invariance. In our case, throwing away these independent scattering processes would prevent getting the necessary thermal corrections to the vertices needed for preserving gauge invariance.…”
Section: First Consider Point (I)mentioning
confidence: 99%
“…(39). First, K A is made of the thermal propagators G 11 (q) and G 22 (q) while {p j }|M|k, {l i } contains only the vacuum ones (G 0 F (q) and G 0 * F (q)).…”
Section: Approximationsmentioning
confidence: 99%