2016
DOI: 10.1088/1742-5468/2016/01/013203
|View full text |Cite
|
Sign up to set email alerts
|

Hyperskewness of (1  +  1)-dimensional KPZ height fluctuations

Abstract: Abstract. We evaluate the fifth order normalized cumulant, known as hyperskewness, of height fluctuations dictated by the (1 + 1)-dimensional KPZ equation for the stochastic growth of a surface on a flat geometry in the stationary state. We follow a diagrammatic approach and invoke a renormalization scheme to calculate the fifth cumulant given by a connected loop diagram. This, together with the result for the second cumulant, leads to the hyperskewness value S = 0.0835.

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

1
6
0

Year Published

2017
2017
2020
2020

Publication Types

Select...
3
2

Relationship

1
4

Authors

Journals

citations
Cited by 5 publications
(7 citation statements)
references
References 53 publications
1
6
0
Order By: Relevance
“…The Gaussian behavior obtained for Eq. ( 3) coincides with analytical DRG results which follow successful analyses of field statistics for the KPZ [45][46][47] and nonlinear-Molecular Beam Epitaxy (MBE) [48] equations, and for the scalar Burgers equation with non-conserved noise [49]. The method performs a partial RG transformation in which the equation is coarse-grained [50], while omitting the rescaling step [27,36].…”
supporting
confidence: 74%
“…The Gaussian behavior obtained for Eq. ( 3) coincides with analytical DRG results which follow successful analyses of field statistics for the KPZ [45][46][47] and nonlinear-Molecular Beam Epitaxy (MBE) [48] equations, and for the scalar Burgers equation with non-conserved noise [49]. The method performs a partial RG transformation in which the equation is coarse-grained [50], while omitting the rescaling step [27,36].…”
supporting
confidence: 74%
“…This scheme of calculation finds out the renormalized quantities directly from various loop diagrams for the second and third order cumulants of velocity derivative. This type of scheme has previously been used for the calculation of statistical cumulants in KPZ [35,36,37] and VLDS [38] surface growth dynamics. Employing diagrammatic approach, we have seen that there are two contributing Feynman diagrams [ Fig.…”
Section: Discussionmentioning
confidence: 99%
“…This scheme is different from the above RG schemes as it finds a relation between the renormalized Feynman diagrams involving the renormalized viscosity. Recently this procedure was found to be successful in determining the experimentally observed statistical characteristics in Kardar-Parisi-Zhang (KPZ) [35,36,37] and Villain-Lai-Das Sarma (VLDS) [38] surface growth dynamics. This scheme enables us to calculate the second-and third-order cumulants of velocity derivative and the resulting value for skewness is obtained as S = −0.647.…”
Section: Introductionmentioning
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%
“…While λ and D do not renormalize and are thus scaleindependent, the coarse-grained linear coefficient ν(k) depends on wave vector as ν(k) ≃ (6Dλ 2 /π) 1/3 |k| −1 (see Appendix A 1 for details). We exploit this fact to estimate by DRG the cumulants of the statistical distribution of φ, following the methodology successfully employed for the KPZ [43][44][45] and NLMBE [46] equations. Thus, the n-th cumulant reads…”
Section: A Drg Evaluation Of Cumulantsmentioning
confidence: 99%