2000
DOI: 10.1088/0741-3335/42/3/303
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Comparative analysis of two formulations of geometrical optics. The effective dielectric tensor

Abstract: Two apparently diverse formulations of geometrical optics relevant to space-and timevarying dispersive, anisotropic media are shown to be equivalent by virtue of the relationship between the effective dielectric tensor and the plane-wave dielectric tensor. As a counterpart of the wave kinetic equation governing the wave-action density in phase space, the equation for the transport of action density in physical configuration space is obtained, which entails, in particular, a wavepacket adiabatic invariant in th… Show more

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Cited by 20 publications
(20 citation statements)
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References 18 publications
(31 reference statements)
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“…It should be noted that the operator presented above satisfies the needed symmetry condition [provided by the condition K ( r , s , ω) = K ( r , − s , −ω)]. As is well known (Kadomtsev 1965; Bornatici & Kravtsov 2000), it is this symmetrical form of permittivity tensor that is used for the calculation of the components of the permittivity tensor ɛ ij (ω, k , r ) Here, η = ( r + r ′ )/2 and ξ = r − r ′ . It is important that the above tensor (equation 43) only describes correctly wave–particle interaction in inhomogeneous media with slowly varying parameters (Bernstein & Friedland 1984).…”
Section: Tensor Derivationmentioning
confidence: 75%
“…It should be noted that the operator presented above satisfies the needed symmetry condition [provided by the condition K ( r , s , ω) = K ( r , − s , −ω)]. As is well known (Kadomtsev 1965; Bornatici & Kravtsov 2000), it is this symmetrical form of permittivity tensor that is used for the calculation of the components of the permittivity tensor ɛ ij (ω, k , r ) Here, η = ( r + r ′ )/2 and ξ = r − r ′ . It is important that the above tensor (equation 43) only describes correctly wave–particle interaction in inhomogeneous media with slowly varying parameters (Bernstein & Friedland 1984).…”
Section: Tensor Derivationmentioning
confidence: 75%
“…They are not related to Joule dissipation and appear because of an additional phase shift between the induction vector and the electric field. This phase shift results from the finite time needed to set the polarization in the plasma with dispersion [26]. Such a phase shift in the plasma with space dispersion appears due to the medium inhomogeneity.…”
Section: Resultsmentioning
confidence: 99%
“…Further, it is well known that for calculating the dielectric permittivity tensor, only the symmetrized form of ε ij (ω, k, r) must be used [93,94]:…”
Section: Calculation Of the Dielectric Permittivity Tensormentioning
confidence: 99%