1993
DOI: 10.1007/bf01135371
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Heat pulse experiments revisited

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Cited by 311 publications
(266 citation statements)
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“…The above choice involves the minimal number of moments necessary for describing the thermal energy transport, but this number, if required by the physical problem under study, can be easily extended to cover, for example, an arbitrary number of scalar and vector moments both for carriers and phonons, by taking into account, e.g., higher microscopic energy powers in the functions ψ [7,26].…”
Section: The 3d Semiclassical Macroscopic Modelsmentioning
confidence: 99%
See 1 more Smart Citation
“…The above choice involves the minimal number of moments necessary for describing the thermal energy transport, but this number, if required by the physical problem under study, can be easily extended to cover, for example, an arbitrary number of scalar and vector moments both for carriers and phonons, by taking into account, e.g., higher microscopic energy powers in the functions ψ [7,26].…”
Section: The 3d Semiclassical Macroscopic Modelsmentioning
confidence: 99%
“…However, these various closure assumptions are, at best, only phenomenological and often a consistent physical and mathematical justification is lacking. Lately, a closure assumption based on the Maximum Entropy Principle of extended thermodynamics [6,7] has been successfully applied, both in the parabolic and non-parabolic band approximation, to various types of semiconductors [8][9][10][11][12][13]. The resulting models, which differ for the choice of the moments to assume as field variables, are, in fact, able to describe charge transport due both to electrons and holes and also heat transport due to phonons.…”
Section: Introductionmentioning
confidence: 99%
“…where is the wavenumber vector and the mean free path associated with the heat flux of order n. We now select the latter as given path ln of order n in terms of n as = ( + 1) /(4( + 1) − 1), with l identified as the mean free path independent of the order of approximation, this being a natural choice in phonon's kinetic theory [18]. By identifying k (which becomes a scalar in our one-dimensional case) as = 2 / and using the definition (9) of the Knudsen number in expression (10) has the asymptotic limit [19] …”
Section: Heat Conductivity Of Nano-porous Si Devicesmentioning
confidence: 99%
“…This represents a nonlinear evolution equation for the heat flux which allows to consider in a simple way some nonlocal, nonlinear and memory effects, beside to study the propagation of heat waves, which is a well-known topic in current nonequilibrium thermodynamics [22,30,[46][47][48].…”
Section: Higher-order Fluxes and Hierarchy Of Nonlinear Transport Equmentioning
confidence: 99%