The Hurst exponent and variance are two quantities that often characterize real-life, high-frequency observations. Such real-life signals are generally measured under noise environments. We develop a multiscale statistical method for simultaneous estimation of a time-changingHurst exponent H(t) and a variance parameter.. in amultifractional Brownian motion model in the presence of white noise. Themethod is based on the asymptotic behavior of the local variation of its sample pathswhich applies to coarse scales of the sample paths. This work provides stable and simultaneous estimators of both parameters when independent white noise is present. We also discuss the accuracy of the simultaneous estimators compared with a few selected methods an...
This thesis deals with statistical problems related to two parametric models : the fractional Browni...
International audienceWe estimate the Hurst parameter H of a fractional Brownian motion from discret...
We consider the models Yi,n = ∫ i/n 0 σ(s)dWs + τ(i/n)i,n, and Ỹi,n = σ(i/n)Wi/n + τ(i/n)i,n, i = 1...
This paper addresses the problem of estimating the Hurst exponent of the fractional Brownian motion ...
Abstract: High frequency based estimation methods for a pure-jump subordinated Brownian motion expos...
Multifractional Brownian motion is a type of stochastic process with time-varying regularity. The ma...
AbstractIn this paper, a class of Gaussian processes, having locally the same fractal properties as ...
AbstractThe generalized multifractional Brownian motion (GMBM) is a continuous Gaussian process that...
Conference PaperThe multifractal spectrum characterizes the scaling and singularity structures of si...
We consider a model based on the fractional Brownian motion under the influence of noise. We impleme...
We estimate the Hurst parameter H of a fractional Brownian motion from discrete noisy data observed ...
The multifractal spectrum characterizes the scaling and singularity structures of signals and proves...
In this paper, we propose a method using continuous wavelets to study the multivariate fractio...
In this paper, we build an estimator of the Hurst exponent of a fractional Lévy motion based on its ...
Some real-world phenomena in geo-science, micro-economy, and turbulence, to name a few, can be effec...
This thesis deals with statistical problems related to two parametric models : the fractional Browni...
International audienceWe estimate the Hurst parameter H of a fractional Brownian motion from discret...
We consider the models Yi,n = ∫ i/n 0 σ(s)dWs + τ(i/n)i,n, and Ỹi,n = σ(i/n)Wi/n + τ(i/n)i,n, i = 1...
This paper addresses the problem of estimating the Hurst exponent of the fractional Brownian motion ...
Abstract: High frequency based estimation methods for a pure-jump subordinated Brownian motion expos...
Multifractional Brownian motion is a type of stochastic process with time-varying regularity. The ma...
AbstractIn this paper, a class of Gaussian processes, having locally the same fractal properties as ...
AbstractThe generalized multifractional Brownian motion (GMBM) is a continuous Gaussian process that...
Conference PaperThe multifractal spectrum characterizes the scaling and singularity structures of si...
We consider a model based on the fractional Brownian motion under the influence of noise. We impleme...
We estimate the Hurst parameter H of a fractional Brownian motion from discrete noisy data observed ...
The multifractal spectrum characterizes the scaling and singularity structures of signals and proves...
In this paper, we propose a method using continuous wavelets to study the multivariate fractio...
In this paper, we build an estimator of the Hurst exponent of a fractional Lévy motion based on its ...
Some real-world phenomena in geo-science, micro-economy, and turbulence, to name a few, can be effec...
This thesis deals with statistical problems related to two parametric models : the fractional Browni...
International audienceWe estimate the Hurst parameter H of a fractional Brownian motion from discret...
We consider the models Yi,n = ∫ i/n 0 σ(s)dWs + τ(i/n)i,n, and Ỹi,n = σ(i/n)Wi/n + τ(i/n)i,n, i = 1...