Abstract:Various paths properties of a stochastic process are obtained under mild conditions which allow for the integrability of the characteristic function of its increments and for the dependence among them. The main assumption is closely related to the notion of local asymptotic self-similarity. New results are obtained for the class of multifractional random processes .
“…A well-known example is multifractional Brownian motion, where the Hurst exponent h of fractional Brownian motion is replaced by a functional parameter h(t), permitting the Hölder exponent to vary in a prescribed way, see [2,3,5,12] and references therein. Close to time t, the process behaves like index-h(t) fractional Brownian motion, but, nevertheless, this local form may vary considerably with time.…”
We use characteristic functions to construct α-multistable measures and integrals, where the measures behave locally like stable measures, but with the stability index α(x) varying with x. This enables us to construct α-multistable processes on R, that is processes whose scaling limit at time t is an α(t)-stable process. We present several examples of such multistable processes and examine their localisability.
“…A well-known example is multifractional Brownian motion, where the Hurst exponent h of fractional Brownian motion is replaced by a functional parameter h(t), permitting the Hölder exponent to vary in a prescribed way, see [2,3,5,12] and references therein. Close to time t, the process behaves like index-h(t) fractional Brownian motion, but, nevertheless, this local form may vary considerably with time.…”
We use characteristic functions to construct α-multistable measures and integrals, where the measures behave locally like stable measures, but with the stability index α(x) varying with x. This enables us to construct α-multistable processes on R, that is processes whose scaling limit at time t is an α(t)-stable process. We present several examples of such multistable processes and examine their localisability.
“…The Hausdorff dimension of the level sets of B (H) (t) is, almost surely, bounded from below by 1−H; see Theorems 4 and 5 in Chapter 18 of [8] (actually, equality holds here, but we will need only the lower bound). The same arguments show that, for an independent Brownian motion B(t), the Hausdorff dimension of any level sets of B(t) − B (H) (t) is also bounded from below by 1 − H almost surely (see also Proposition 5.1 and Section 7.2 in [2]). Moreover, it is well known that, for a standard one-dimensional Brownian motion and any x ∈ R, any set of Hausdorff dimension strictly greater than 1/2 is intersected by the level set {t : B(t) = x} with positive probability.…”
Section: Proof Of Theoremmentioning
confidence: 76%
“…• if a n = 3, let f a 1 ,...,a n (0) = f a 1 ,...,a n−1 (2), f a 1 ,...,a n (1) = f a 1 ,...,a n−1 (1).…”
Section: Definition 21mentioning
confidence: 99%
“…. , a n is not 0-reverse, let f a 1 ,...,a n (0) = f a 1 ,...,a m (0); • if a n = 3, let f a 1 ,...,a n (0) = f a 1 ,...,a n−1 (2) and -if a 1 , . .…”
Section: Algorithm 2 (Alternate Generalized Hilbert) Define F ∅ By (mentioning
“…Ayache, Cohen and Lévy-Véhel [3] and Herbin [19] studied the covariance structure of mfBm with harmonisable representations. We refer to [14,29] for further information. We refer to [14,29] for further information.…”
By using a wavelet method we prove that the harmonisable-type N -parameter multifractional Brownian motion (mfBm) is a locally nondeterministic Gaussian random field. This nice property then allows us to establish joint continuity of the local times of an (N, d)-mfBm and to obtain some new results concerning its sample path behavior.Résumé. Au moyen d'une méthode d'ondelettes nous montrons que le mouvement Brownien multifractionnaire de type harmonisable à N indices (mfBm) est un champ Gaussien localement non-déterministe. Grâce à cette propriété nous établissons ensuite la bicontinuité des temps locaux d'un (N, d)-mfBm et cela nous permet d'obtenir de nouveaux résultats concernant son comportement trajectoriel.MSC: 60G15; 60G17; 28A80
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