We study the fluctuations of the outer domain of Hastings–Levitov clusters in the small particle limit. These are shown to be given by a continuous Gaussian process F taking values in the space of holomorphic functions on |z|>1 , of which we provide an explicit construction. The boundary values W of F are shown to perform an Ornstein–Uhlenbeck process on the space of distributions on the unit circle T, which can be described as the solution to the stochastic fractional heat equation ∂/∂W(t,ϑ)=-(-Δ)1/2W(t,ϑ)+√2ξ(t,ϑ),where Δ denotes the Laplace operator acting on the spatial component, and ξ(t, ϑ) is a space-time white noise. As a consequence we find that, when the cluster is left to grow indefinitely, the boundary process W converges to a log-correlated fractional Gaussian field, which can be realised as (-Δ) -1/4W, for W complex white noise on T.
Fluctuation results for Hastings–Levitov planar growth / Silvestri, V.. - In: PROBABILITY THEORY AND RELATED FIELDS. - ISSN 0178-8051. - 167:1-2(2017), pp. 417-460. [10.1007/s00440-015-0688-7]
Fluctuation results for Hastings–Levitov planar growth
Silvestri V.
2017
Abstract
We study the fluctuations of the outer domain of Hastings–Levitov clusters in the small particle limit. These are shown to be given by a continuous Gaussian process F taking values in the space of holomorphic functions on |z|>1 , of which we provide an explicit construction. The boundary values W of F are shown to perform an Ornstein–Uhlenbeck process on the space of distributions on the unit circle T, which can be described as the solution to the stochastic fractional heat equation ∂/∂W(t,ϑ)=-(-Δ)1/2W(t,ϑ)+√2ξ(t,ϑ),where Δ denotes the Laplace operator acting on the spatial component, and ξ(t, ϑ) is a space-time white noise. As a consequence we find that, when the cluster is left to grow indefinitely, the boundary process W converges to a log-correlated fractional Gaussian field, which can be realised as (-Δ) -1/4W, for W complex white noise on T.File | Dimensione | Formato | |
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