2015
DOI: 10.1016/j.spl.2015.01.012
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Representation of self-similar Gaussian processes

Abstract: a b s t r a c tWe develop the canonical Volterra representation for a self-similar Gaussian process by using the Lamperti transformation of the corresponding stationary Gaussian process, where this latter one admits a canonical integral representation under the assumption of pure non-determinism. We apply the representation obtained to the equivalence in law for self-similar Gaussian processes.

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Cited by 10 publications
(9 citation statements)
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“…Then X is purely non-deterministic if H X 0+ is trivial. By [11] a purely non-deterministic Gaussian self-similar process admits the representation…”
Section: Self-similar Processesmentioning
confidence: 99%
“…Then X is purely non-deterministic if H X 0+ is trivial. By [11] a purely non-deterministic Gaussian self-similar process admits the representation…”
Section: Self-similar Processesmentioning
confidence: 99%
“…whereῩ is defined in (21) SinceῩ is the covariance function of a continuous Volterra process, a large deviation principle for 1] ) ε>0 actually holds from Theorem 2 with the inverse speed γ 2 ε and the good rate function given by (22). From Equation (18) and Remark 2 the same large deviation principle holds for the noncentered family…”
mentioning
confidence: 68%
“…Consider X(t) = t 0 κ(t, u)B(du) , t ≥ 0 with a Volterra kernel κ(t, u) = (t − u) α u −γ/2 . This process or similar processes have been recently studied by Yazigi (2015) [23]. By Theorem 2.1 in [23], the Volterra kernel κ can be written as…”
Section: Hölder Continuitymentioning
confidence: 95%
“…This process or similar processes have been recently studied by Yazigi (2015) [23]. By Theorem 2.1 in [23], the Volterra kernel κ can be written as…”
Section: Hölder Continuitymentioning
confidence: 95%