2001
DOI: 10.1006/aphy.2001.6170
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A Wigner Quasi-distribution Function for Charged Particles in Classical Electromagnetic Fields

Abstract: A gauge-invariant Wigner quasi-distribution function for charged particles in classical electromagnetic fields is derived in a rigorous way. Its relation to the axial gauge is discussed, as well as the relation between the kinetic and canonical momenta in the Wigner representation. Gauge-invariant quantum analogs of Hamilton-Jacobi and Boltzmann kinetic equations are formulated for arbitrary classical electromagnetic fields in terms of the 'slashed' derivatives and momenta, introduced for this purpose. The kin… Show more

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Cited by 37 publications
(40 citation statements)
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“…The transposition of (72) toward the ξ-integrated representation of the quasi-classical Green function is straightforward, except for the collision integral which we discuss now separately. If we suppose the disorder to be weakly and isotropically interacting with the electrons and randomly distributed along the sample, a convenient approximation to describe it is the Born approximation (66). There, we substitute d 3 p/ (2π ) 3 ≈ N 3d 0 dξ p dΩ p /4π in 3D, d 2 p/ (2π ) 2 ≈ N 2d 0 dξ p dΩ p /2π in 2D or dp/2π = N 1d 0 dξ p in 1D, with Ω p the solid-angle in the momentum space and N 3d 0 = mp F /2π 2 3 , N 2d 0 = m/2π 2 or N 1d 0 = m/p F 2π the density of state in the normal metal in 3D, 2D and 1D, respectively.…”
Section: Eilenberger Equationmentioning
confidence: 99%
“…The transposition of (72) toward the ξ-integrated representation of the quasi-classical Green function is straightforward, except for the collision integral which we discuss now separately. If we suppose the disorder to be weakly and isotropically interacting with the electrons and randomly distributed along the sample, a convenient approximation to describe it is the Born approximation (66). There, we substitute d 3 p/ (2π ) 3 ≈ N 3d 0 dξ p dΩ p /4π in 3D, d 2 p/ (2π ) 2 ≈ N 2d 0 dξ p dΩ p /2π in 2D or dp/2π = N 1d 0 dξ p in 1D, with Ω p the solid-angle in the momentum space and N 3d 0 = mp F /2π 2 3 , N 2d 0 = m/2π 2 or N 1d 0 = m/p F 2π the density of state in the normal metal in 3D, 2D and 1D, respectively.…”
Section: Eilenberger Equationmentioning
confidence: 99%
“…Moreover also the Wigner distribution function (Levanda and Fleurov, 2001), although providing significant information about the quantum states, presents conceptual difficulties: It cannot be really regarded like a probability distribution in the classical sense, rather it is a quasi-probability that can take even negative values; moreover it can represent the average value of an observable but not, in general, also its higher power moments. Both these difficulties are bypassed exploiting the statistical formulation of the quantum uncertainty, regarded as a fundamental assumption itself; it reads in one space dimension:…”
Section: Quantum Backgroundmentioning
confidence: 99%
“…The properties of the GIWF have been detailed in [4,5]. Nevertheless for completeness we discuss some of them once again.…”
Section: Basic Properties Of the Gauge Invariant Wigner Functionmentioning
confidence: 99%