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A fundamental question in rough path theory is whether the expected signature of a geometric rough path completely determines the law of signature. One sufficient condition is that the expected signature has infinite radius of convergence, which is satisfied by various stochastic processes on a fixed time interval, including the Brownian motion. In contrast, for the Brownian motion stopped upon the first exit time from a bounded domain $Omega$, it is only known that the radius of convergence for the expected signature on sufficiently regular $Omega$ is strictly positive everywhere, and that the radius of convergence is finite at some point when $Omega$ is the $2$-dimensional unit disc ([1]). In this paper, we prove that on any bounded $C^{2,alpha}$-domain $Omega subset mathbb{R}^d$ with $2leq d leq 8$, the expected signature of the stopped Brownian motion has finite radius of convergence everywhere. A key ingredient of our proof is the introduction of a domain-averaging hyperbolic development (see Definition 4.1), which allows us to symmetrize the PDE system for the hyperbolic development of expected signature by averaging over rotated domains.
The Brownian motion $(U^N_t)_{tge 0}$ on the unitary group converges, as a process, to the free unitary Brownian motion $(u_t)_{tge 0}$ as $Ntoinfty$. In this paper, we prove that it converges strongly as a process: not only in distribution but also
Let ${U^N_t}_{tge 0}$ be a standard Brownian motion on $mathbb{U}(N)$. For fixed $Ninmathbb{N}$ and $t>0$, we give explicit bounds on the $L_1$-Wasserstein distance of the empirical spectral measure of $U^N_t$ to both the ensemble-averaged spectral m
In this paper we state and prove a central limit theorem for the finite-dimensional laws of the quadratic variations process of certain fractional Brownian sheets. The main tool of this article is a method developed by Nourdin and Nualart based on the Malliavin calculus.
We delve deeper into the compelling regularizing effect of the Brownian-time Brownian motion density, $KBtxy$, on the space-time-white-noise-driven stochastic integral equation we call BTBM SIE, which we recently introduced. In sharp contrast to seco
In this paper we prove that the spatially homogeneous Landau equation for Maxwellian molecules can be represented through the product of two elementary processes. The first one is the Brownian motion on the group of rotations. The second one is, cond