Linear Multifractional Stable Motion: wavelet estimation of H(⋅)H(\cdot) and $\al$ parameters

preprint2013arXivOpen access

Abstract

Linear Fractional Stable Motion (LFSM) of Hurst parameter HH and of stability parameter $\al$, is one of the most classical extensions of the well-known Gaussian Fractional Brownian Motion (FBM), to the setting of heavy-tailed stable distributions \cite{SamTaq,EmMa}. In order to overcome some limitations of its areas of application, coming from stationarity of its increments as well as constancy over time of its self-similarity exponent, Stoev and Taqqu introduced in \cite{stoev2004stochastic} an extension of LFSM, called Linear Multifractional Stable Motion (LMSM), in which the Hurst parameter becomes a function H(⋅)H(\cdot) depending on the time variable tt. Similarly to LFSM, the tail heaviness of the marginal distributions of LMSM is determined by $\al$; also, under some conditions, its self-similarity is governed by H(⋅)H(\cdot) and its path roughness is closely related to $H(\cdot)-1/\al$. Namely, it was shown in \cite{stoev2004stochastic} that H(t0)H(t_0) is the self-similarity exponent of LMSM at a time t0≠0t_0\neq 0; moreover, very recently, it was established in \cite{hamonier2012lmsm}, that the quantities $\min_{t\in I} H(t)-1/\al$, and $H(t_0)-1/\al$, are respectively the uniform Hölder exponent of LMSM on a compact interval II, and its local Hölder exponent at t0t_0. The main goal of our article, is to construct, using wavelet coefficients of LMSM, strongly consistent (i.e. almost surely convergent) statistical estimators of min⁡t∈IH(t)\min_{t\in I} H(t), H(t0)H(t_0), and $\al$; our estimation results, are obtained when $\al\in (1,2)$, and, H(⋅)H(\cdot) is a Hölder function smooth enough, with values in a compact subinterval [H‾,Hˉ][\underline{H},\bar{H}] of $(1/\al,1)$.

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