An integral functional driven by fractional Brownian motion

preprint2016arXivOpen access

Abstract

Let BHB^H be a fractional Brownian motion with Hurst index 0<H<10<H<1 and the weighted local time LH(⋅,t){\mathscr L}^H(\cdot,t). In this paper, we consider the integral functional CtH(a):=lim⁡ε↓0∫0t1{∣BsH−a∣>ε}1BsH−ads2H≡1πHLH(⋅,t)(a) {\mathcal C}^H_t(a):=\lim_{\varepsilon\downarrow 0}\int_0^t1_{\{|B^H_s-a|>\varepsilon\}}\frac1{B^H_s-a}ds^{2H}\equiv \frac1π{\mathscr H}{\mathscr L}^H(\cdot,t)(a) in L2(Ω)L^2(Ω) with a∈R,t≥0 a\in {\mathbb R}, t\geq 0 and H{\mathscr H} denoting the Hilbert transform. We show that CtH(a)=2((BtH−a)log⁡∣BtH−a∣−BtH+alog⁡∣a∣−∫0tlog⁡∣BsH−a∣δBsH) {\mathcal C}^H_t(a)=2\left((B^H_t-a)\log|B^H_t-a|-B^H_t+a\log|a| -\int_0^t\log|B^H_s-a|δB^H_s\right) for all a∈R,t≥0a\in {\mathbb R}, t\geq 0 which is the fractional version of Yamada's formula, where the integral is the Skorohod integral. Moreover, we introduce the following {\it occupation type formula}: ∫RCtH(a)g(a)da=2Hπ∫0t(Hg)(BsH)s2H−1ds \int_{\mathbb R}{\mathcal C}^H_t(a)g(a)da=2Hπ\int_0^t({\mathscr H}g)(B^H_s)s^{2H-1}ds for all continuous functions gg with compact support.

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