2009
DOI: 10.1088/1742-5468/2009/07/p07012
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Winding of planar Gaussian processes

Abstract: We consider a smooth, rotationally invariant, centered gaussian process in the plane, with arbitrary correlation matrix C tt . We study the winding angle φt around its center. We obtain a closed formula for the variance of the winding angle as a function of the matrix C tt . For most stationary processes C tt = C(t − t ) the winding angle exhibits diffusion at large time with. Correlations of exp(inφt) with integer n, the distribution of the angular velocityφt, and the variance of the algebraic area are also o… Show more

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Cited by 5 publications
(11 citation statements)
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“…provided that this infinite integral is finite. This coincides with predictions in a physics paper of Le Doussal, Etzioni and Horovitz [6]. They also noticed the following simplification in this case: denoting θ(x) = arcsin r(x) (θ is well-defined, since r is now real-valued), we have…”
Section: Denoting R(x) = R ′supporting
confidence: 89%
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“…provided that this infinite integral is finite. This coincides with predictions in a physics paper of Le Doussal, Etzioni and Horovitz [6]. They also noticed the following simplification in this case: denoting θ(x) = arcsin r(x) (θ is well-defined, since r is now real-valued), we have…”
Section: Denoting R(x) = R ′supporting
confidence: 89%
“…However, perhaps surprisingly, the winding of Gaussian stationary processes appears to be a topic that has been largely ignored. Prior to this work, we know only of a paper by Le-Doussal, Etzioni and Horovitz [6] which provides predictions and intriguing examples regarding the nature of the fluctuations of the winding. Their interest was inspired by their research on the winding of particles in random environments [9].…”
Section: Introductionmentioning
confidence: 99%
“…Recently Le Doussal [68] used the replica Bethe ansatz to obtain an exact representation for the distribution of the one-point, two-time height difference h (0, t) − h (0, 0) for the KPZ interface for a combined initial condition which is flat at x < 0 and stationary at x > 0. This problem can be generalized by considering the distribution P (H, L) of the two-point, two-time height difference H = h (L, t)−h (0, 0) with the same combined initial condition.…”
Section: Summary and Discussionmentioning
confidence: 99%
“…It is therefore the optimal history for the combined initial condition of Ref. [68] at L ≥ 0. As a result, the λH 1 tail of P (H, L) for the combined initial condition is given by Eqs.…”
Section: Summary and Discussionmentioning
confidence: 99%
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