2001
DOI: 10.1063/1.1383025
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Inverse bremsstrahlung of hot, weakly coupled plasmas

Abstract: The free–free absorption coefficient for radiation in hot, weakly coupled plasmas is determined from a systematic approach to the dynamical conductivity. Based on a generalized linear-response theory, it is expressed in terms of determinants of equilibrium correlation functions permitting a perturbative treatment. Within a Gould–DeWitt-type approach, dynamical screening is accounted for by a partial summation of loop diagrams, while strong collisions are treated by a ladder approximation. Known expressions for… Show more

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Cited by 44 publications
(63 citation statements)
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“…(1) and (2) we have shown the second order diagrams for the bremsstrahlung and inverse bremsstrahlung process. These processes are well known and expressions were given by QED S-matrix calculations [15] as well as by a non-relativistic treatment [16]. We will draw our attention to the inverse bremsstrahlung within our formalism in the next section.…”
Section: Inclusion Of Collisionsmentioning
confidence: 99%
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“…(1) and (2) we have shown the second order diagrams for the bremsstrahlung and inverse bremsstrahlung process. These processes are well known and expressions were given by QED S-matrix calculations [15] as well as by a non-relativistic treatment [16]. We will draw our attention to the inverse bremsstrahlung within our formalism in the next section.…”
Section: Inclusion Of Collisionsmentioning
confidence: 99%
“…In [16] non-relativistic results for the absorption coefficient in different approximations are derived. The expression given in the paper in terms of the transition matrix correspond to the non-relativistic result of Eq.…”
Section: Evaluation Of the Correlation Functionmentioning
confidence: 99%
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“…We show in this paper how the Gaunt factor can be derived from linear response theory [18] in a general way. Within this framework, modifications of the emission spectrum beyond Born aproximation can be included in a systematic manner [19] as will be discussed later.…”
Section: Introductionmentioning
confidence: 99%
“…The Kramers result, given below in Eq. (19), is derived from the assumption of Keplerian trajectories of the emitting electron in the Coulomb field of an ion and integration over all initial velocities weighted with the Maxwellian velocity distribution function. Quantum features are only accounted for in a semiclassical way: The velocity integral extends over velocities v, fulfilling the condition mv 2 /2 ≥ ω, i.e.…”
Section: Introductionmentioning
confidence: 99%