1997
DOI: 10.1063/1.593344
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Acoustic transparency of layered conductors

Abstract: The method for investigating the electron properties of metals, which was developed by I. M. Lifshits under the assumption that the form of the energy–momentum relation for charge carriers is known a priori, and for reconstructing the electron energy spectrum from experimental data is applied for studying acoustoelectronic effects in layered conductors with a strongly anisotropic conductivity of the metallic type. It is shown that the attenuation of acoustic waves propagating along the layers can become much w… Show more

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Cited by 5 publications
(3 citation statements)
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“…If an electron drifts along the sound wavevector (for instance, the sound wave propagates along the y-axis) the sound decrement reduces in (klη) 2 times for r/l ≪ krη ≪ 1 [47]. The solution of the kinetic equation in this case takes the form…”
Section: 33)mentioning
confidence: 99%
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“…If an electron drifts along the sound wavevector (for instance, the sound wave propagates along the y-axis) the sound decrement reduces in (klη) 2 times for r/l ≪ krη ≪ 1 [47]. The solution of the kinetic equation in this case takes the form…”
Section: 33)mentioning
confidence: 99%
“…We consider the propagation of acoustic waves and co-moving electromagnetic waves with reference to the electron-electron interaction [52][53][54]. Charge carriers are supposed to form, not a Fermi-gas but a Fermi-liquid in which the correlation effects are essential.…”
Section: Fermi-liquid Effectsmentioning
confidence: 99%
“…In a strong magnetic field H ( τ 1; τ is the charge-carrier relaxation time), all 0953-8984/98/5011765+08$19.50 c 1998 IOP Publishing Ltd of the kinetic and thermodynamic characteristics of conductors are very sensitive to the form of the electron energy spectrum. A series of effects exist which are typical for layered conductors with metal-type conductivity, but non-existent for ordinary metals [1][2][3][4][5][6]. Among these effects, arising from the quasi-two-dimensional nature of the charge-carrier energy spectrum, is the high acoustic transparency of a conductor in the absence of charge-carrier drift along the sound wavevector k in the range of the magnetic field for which 1 kr kl.…”
mentioning
confidence: 99%