1984
DOI: 10.1103/physrevb.30.6756
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Recurrence relations and time evolution in the three-dimensional Sawada model

Abstract: Time-dependent behavior of the three-dimensional Saeada model is obtained by a method of recurrence relations, Exactly calculated quantities are the time evolution of the density-fluctuation operator and its random force. As an application, their linear coefficients, the relaxation and memory functions, are used to obtain certain dynamic quantities, e.g. , the mobility.

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Cited by 20 publications
(9 citation statements)
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“…Applying the Laplace transform yields Π(z) = (2γ/π) arctan(ω s /z). It is interesting to note that this memory function is realized in electron gas models [27]. We now show that it is possible to find at least three time scales for this memory.…”
Section: Normal Diffusionmentioning
confidence: 99%
“…Applying the Laplace transform yields Π(z) = (2γ/π) arctan(ω s /z). It is interesting to note that this memory function is realized in electron gas models [27]. We now show that it is possible to find at least three time scales for this memory.…”
Section: Normal Diffusionmentioning
confidence: 99%
“…The basal autocorrelation a 0 is unknown a priori, however it is possible to determine it through the analytical theory of continued fractions due to Mori [16]. By taking the Laplace transform of 1 It is worth mentioning that the KSP (6) has already been used in several situations where β → ∞ (see, e.g., [6,7]). It is a standard linear response relation whose validity at T = 0 was established many years ago [2,17,18].…”
Section: The Recurrence Relations Methodsmentioning
confidence: 99%
“…The apparatus we are going to employ to solve the equation of motion of the density fluctuation is the well established RRM. This approach has already been successfully applied in the study of the nonrelativistic dense electron gas (2DEG), at the long wavelength and zero temperature limits, in one [5], two [6], three [7], and D dimensions [8]. Applications of the RRM to many-body systems, in general, are also available in the literature (see, e.g., reference [9]).…”
Section: Introductionmentioning
confidence: 99%
“…To order k, D, = u2n2/ (4n2 -l), nb 1, where u is defined in (C). Then, R(Z) = tan-' u/z and R(t) =jo(ut), where/, is the spherical Bessel function of order n. An interacting version of this model has been obtained [57].…”
Section: T=umentioning
confidence: 99%