2007
DOI: 10.1007/s10955-007-9304-2
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On the Zero Mass Limit of Tagged Particle Diffusion in the 1-d Rayleigh-Gas

Abstract: We consider the M → 0 limit for tagged particle diffusion in a 1-dimensional Rayleigh-gas, studied originaly by Sinai and Soloveichik [14], respectively by Szász and Tóth [19]. In this limit we derive a new type of model for tagged paricle diffusion, with Calogero-Moser-Sutherland (i.e. inverse quadratic) interaction potential between the two central particles. Computer simulations on this new model reproduce exactly the numerical value of the limiting variance obtained by Boldrighini, Frigio and Tognetti in … Show more

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Cited by 2 publications
(16 citation statements)
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“…Thus α = 0 in (1.13). Therefore by (1.13), q * (a)[1] = lim α→0 2 − α {(2a + α) − (2a − α) } = a −1 .Thus, by the second formula of (1.13), we obtain w * (a)[1] by x a [1] = a 2 , so 3 is proved. Now apply (1.54), also at (r, y, z) = 1.…”
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confidence: 86%
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“…Thus α = 0 in (1.13). Therefore by (1.13), q * (a)[1] = lim α→0 2 − α {(2a + α) − (2a − α) } = a −1 .Thus, by the second formula of (1.13), we obtain w * (a)[1] by x a [1] = a 2 , so 3 is proved. Now apply (1.54), also at (r, y, z) = 1.…”
mentioning
confidence: 86%
“…Since any downward lattice path from n to 0 must first reach the level m = 1, we have an initial factor g n,1 in a product formula for g n,0 . Any section of a lattice path for g n,1 , which must end in DD, is followed by a sequence of steps of the form (U D) U U , or by a terminal sequence (U D) D. To handle transitions that do not start U U or DD we introduce: [1] is as well. In our discussion of g n,0 , if f ≥ 3, then k a = k(a, a) accounts for a generating factor for an upward preamble (U D) from level m = 1, succeeding DD and preceding U U ; in this case…”
Section: Proofs Of the Building Blocksmentioning
confidence: 99%
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