2015
DOI: 10.1088/1742-5468/2015/05/p05020
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Kurtosis of height fluctuations in (1 + 1) dimensional KPZ dynamics

Abstract: Abstract. We study the fourth order normalized cumulant of height fluctuations governed by 1 + 1 dimensional Kardar-Parisi-Zhang (KPZ) equation for a growing surface. Following a diagrammatic renormalization scheme, we evaluate the kurtosis Q from the connected diagrams leading to the value Q = 0.1523 in the large-scale long-time limit.

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Cited by 7 publications
(19 citation statements)
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“…Since the dynamics is governed by a white noise following a Gaussian distribution, the lowest order approximation appeares to be influenced rather strongly by the Gaussian noise. A similar trend was observed in the one-loop perturbative calculation for kurtosis, namely, Q = 0.1523 [42] which is lower than the Baik-Rains value 0.2892. However the value for skewness via the perturbative scheme, namely, S = 0.3237 [41] is slightly lower than the Baik-Rains value 0.3594.…”
Section: Discussionsupporting
confidence: 83%
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“…Since the dynamics is governed by a white noise following a Gaussian distribution, the lowest order approximation appeares to be influenced rather strongly by the Gaussian noise. A similar trend was observed in the one-loop perturbative calculation for kurtosis, namely, Q = 0.1523 [42] which is lower than the Baik-Rains value 0.2892. However the value for skewness via the perturbative scheme, namely, S = 0.3237 [41] is slightly lower than the Baik-Rains value 0.3594.…”
Section: Discussionsupporting
confidence: 83%
“…We shall find a renormalized equivalent of this bare quantity by means of a renormalization scheme employed earlier for the calculation of skewness and kurtosis [41,42]. We perform the internal frequency integration in Eq.…”
Section: The Fifth Cumulantmentioning
confidence: 99%
“…A similar scheme was employed earlier for the calculation of skewness [40] and kurtosis [41] in the case of non-conserved interface growth governed by the (1 + 1)-dimensional KPZ equation. The amputated parts of the connected loop diagrams, namely, l 2 , l etc., for the second and third moments as shown in Figs.…”
Section: Discussionmentioning
confidence: 99%
“…Subsequently, we calculate the skewness of height fluctuations of the VLDS equation. A similar scheme was employed earlier for the calculation of skewness [40] and kurtosis [41] in the case of non-conserved interface growth governed by the (1 + 1)dimensional KPZ equation. The amputated parts of the connected loop diagrams, namely, l 2 , l…”
Section: Discussionmentioning
confidence: 99%
“…where k n = − n−1 j=1 k j , ω n = − n−1 j=1 ω j . The function L n is perturbatively computed to one loop order [43][44][45][46] as L n = (2D)δ n,2 + L n,1 ,…”
Section: Cumulantsmentioning
confidence: 99%