1993
DOI: 10.1103/physrevlett.70.249
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Cited by 48 publications
(72 citation statements)
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“…In this situation, typicality can provide a fresh numerical perspective [9], Much less is known on transport dynamics apart from the mere existence of Drude weights. For spin transport at A = 1, steady-state bath scenarios [61,62] and classical simulations [63][64][65] suggest superdiffusive dynamics in the limit of high temperatures, while bosonization predicts diffusion at low but nonzero temperatures [66]. At A > 1, signatures of diffusion have been observed also at high temperatures in different approaches [47,61,62,65,67,68] (see Ref.…”
Section: Introductionmentioning
confidence: 99%
“…In this situation, typicality can provide a fresh numerical perspective [9], Much less is known on transport dynamics apart from the mere existence of Drude weights. For spin transport at A = 1, steady-state bath scenarios [61,62] and classical simulations [63][64][65] suggest superdiffusive dynamics in the limit of high temperatures, while bosonization predicts diffusion at low but nonzero temperatures [66]. At A > 1, signatures of diffusion have been observed also at high temperatures in different approaches [47,61,62,65,67,68] (see Ref.…”
Section: Introductionmentioning
confidence: 99%
“…In particular, it was found that the usual hydrodynamic assumptions break down in one dimension, so that the asymptotic behavior of the spin-spin correlation function deviates from the predictions of the classical diffusion theory ͑see Ref. 5 and references therein͒.…”
mentioning
confidence: 99%
“…We computed several logarithms of r to check the above scaling theory and found agreement with calculations of the critical exponents in the critical (massless) phase [14]. The most important result comes from the second order (two-loop) coefficient of x 3 log r that provides the temperature exponent of the slope a of Q(x) showing that it is equal to β, at least up to O(ǫ).…”
mentioning
confidence: 89%
“…They did not find any meaningful fixpoint, thus suggesting that there is no ATline around 6 dimensions. We feel, however, that their projected field theory, with all the masses other than that of the replicon taken to be infinite, is not sufficient to settle the question since even the crossover region including the known zero-field fixed-point [14] is impossible to reach in this model with only two cubic coupling constants. Taking into account all the eight cubic invariants of the permutation group we would have a large enough parameter space with eight ϕ 3 coupling constants and three masses.…”
mentioning
confidence: 99%
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