SearcharxivSearch

arXiv subjects

Davide A. Bignamini

Publications and source records attributed to Davide A. Bignamini.

10 recordsLinked to original sources

Asymptotic Behaviour for Isotropic Pearson Random Walks

In the Pearson random walk the direction of the i-th step is a random variable uniformly distributed on the d-dimensional sphere, and its length is a non-negative random variable. In a general framework, we are going to study the asymptotic behaviour of the Pearson random walks when the dimension d goes to infinity. Further, we investigate the same convergence result in a more general framework, where both the number and the lengths of the steps depend on the dimension. The results in the present paper can be applied to approximate the distribution of some classical Pearson random walk, for example, in the Dirichlet case.

math.PR

Stochastic dissipative systems in Banach spaces driven by Lévy noise

In this paper, we are interested in the well-posedness of stochastic reaction diffusion equations like \begin{equation} \begin{cases} dX(t)(ξ)=\big(Δ_ξX(t)(ξ)-p(X(t)(ξ))\big)dt+RdW(t)+dL(t) , \quad t\in [0,T];\\ X(0)=x\in L^2(\mathcal{O}) \end{cases} \end{equation} where $\mathcal{O}$ is a bounded open domain of $\mathbb{R}^d$ with regular boundary, $d\in\mathbb{N}$, $p:\mathbb{R}\rightarrow\mathbb{R}$ is a polynomial of odd degree with positive leading coefficient, $R$ is a linear bounded operator on $L^2(\mathcal{O})$, $\{W(t)\}_{t\geq 0}$ is a $L^2(\mathcal{O})$-cylindrical Wiener process, $\{L(t)\}_{t\geq 0}$ is a pure-jump Lévy process on $L^2(\mathcal{O})$. We complement the equation with suitable boundary conditions on $\partial \mathcal{O}.$ Some papers in literature analize existence and uniqueness of mild solutions for every $x\in L^p(\mathcal{O})$, for some suitable $p\geq 2$. The results of this paper allow to study reaction diffusion equations also on the space of continuous function $C(\overline{O})$. This seems to be new in the Lévy case (it is already done in the Wiener case).\\ We also discuss and review the previous cited works with the aim of unifying the different frameworks. We underline that when $R=0$ for every $x\in C(\overline{O})$ (or $x\in L^p(\mathcal{O})$) the mild solution to the equation has a càdlàg modifications in $C(\overline{O})$ (or $\in L^p(\mathcal{O})$), even if $\{L(t)\}_{t \geq 0}$ is not a Lévy process taking values in $C(\overline{O})$ (or $\in L^p(\mathcal{O})$). This phenomenon for the linear problem (i.e., $F\equiv 0$ in the SPDE) has been investigated in other papers.

math.PR

Stochastic and deterministic non-autonomous reaction-diffusion equations

In this paper we prove the well-posedness of non-autonomous deterministic and stochastic reaction-diffusion equations with a polynomial reaction term. Concerning the stochastic problem, we also prove a new result on the space-time regularity of the non-autonomous stochastic convolution.

math.PR

Pathwise uniqueness for stochastic heat and damped equations with Hölder continuous drift

In this paper, we prove pathwise uniqueness for stochastic differential equations in infinite dimension. Under our assumptions, we are able to consider the stochastic heat equation up to dimension $3$, the stochastic damped wave equation in dimension $1$ and the stochastic Euler-Bernoulli damped beam equation up to dimension $3$. We do not require that the so-called {\it structure condition} holds true.

math.PR

$L^p$-$L^q$ estimates for transition semigroups associated to dissipative stochastic systems

In a separable Hilbert space, we study supercontractivity and ultracontractivity properties for a transition semigroups associated with a stochastic partial differential equations. This is done in terms of exponential integrability of Lipschitz functions and some logarithmic Sobolev-type inequalities with respect to invariant measures. The abstract characterization results concerning the improving of summability can be applied to transition semigroups associated to a stochastic reaction-diffusion equations.

math.PR

Log-Sobolev inequalities and hypercontractivity for Ornstein-Uhlenbeck evolution operators in infinite dimensions

In an infinite dimensional separable Hilbert space $X$, we study the realizations of Ornstein-Uhlenbeck evolution operators $\pst$ in the spaces $L^p(X,\g_t)$, $\{\g_t\}_{t\in\R}$ being the unique evolution system of measures for $\pst$ in $\R$. We prove hyperconctractivity results, relying on suitable Log-Sobolev estimates. Among the examples we consider the transition evolution operator of a non autonomous stochastic parabolic PDE.

math.AP

Schauder regularity results in separable Hilbert spaces

We prove Schauder type estimates for solutions of stationary and evolution equations driven by weak generators of transition semigroups associated to a semilinear stochastic partial differential equations with values in a separable Hilbert space.

math.AP

$L^2$-theory for transitions semigroups associated to dissipative systems

Let $\mathcal{X}$ be a real separable Hilbert space. Let $C$ be a linear, bounded and positive operator on $\mathcal{X}$ and let $A$ be the infinitesimal generator of a strongly continuous semigroup on $\mathcal{X}$. Let $\{W(t)\}_{t\geq 0}$ be a $\mathcal{X}$-valued cylindrical Wiener process on a filtered (normal) probability space $(Ω,\mathcal{F},\{\mathcal{F}_t\}_{t\geq 0},\mathbb{P})$. Let $F:D(F)\subseteq\mathcal{X}\rightarrow\mathcal{X}$ be a smooth enough function. Under suitable conditions on $A$, $C$ and $F$ the following semilinear stochastic partial differential equation \begin{gather*} \begin{cases} dX(t,x)=\big(AX(t,x)+F(X(t,x))\big)dt+ \sqrt{C}dW(t), & t>0;\\ X(0,x)=x\in \mathcal{X}, \end{cases} \end{gather*} has a unique generalized mild solution $\{X(t,x)\}_{t\geq 0}$. We consider the transition semigroup defined by \begin{align*} P(t)φ(x):=\mathbb{E}[φ(X(t,x))], \qquad φ\in B_b(\mathcal{X}),\ t\geq 0,\ x\in \mathcal{X}. \end{align*} If $\mathcal{O}$ is an open set of $\mathcal{X}$, we consider the stopped semigroup defined by \begin{equation*} P^{\mathcal{O}}(t)φ(x):=\mathbb{E}\left[φ(X(t,x))\mathbb{I}_{\{ω\inΩ\; :\;τ_x(ω)> t\}}\right],\quad φ\in B_b(\mathcal{O}),\; x\in\mathcal{O},\; t>0 \end{equation*} where $τ_x$ is the stopping time defined by \begin{equation*} τ_x=\inf\{ s> 0\; : \; X(s,x)\in \mathcal{O}^c \}. \end{equation*} We will study the infinitesimal generators of $P(t)$ and $P^{\mathcal{O}}(t)$ in $L^2(\mathcal{X},ν)$ and $L^2(\mathcal{O},ν)$ respectively, where $ν$ is the unique invariant measure of $P(t)$. We will focus on investigating how these two semigroups are related to the operator formally defined by \begin{equation*} Nφ(x):=\frac{1}{2}\mbox{Tr}[C\nabla^2φ(x)]+\langle Ax+F(x), \nablaφ(x) \rangle. \end{equation*}

math.PR