Exponentially weighted resolvent estimates for complex Ornstein-Uhlenbeck systems

preprint2015arXivOpen access

Abstract

In this paper we study differential operators of the form \begin{align*} \left[\mathcal{L}_\infty v \right](x) = A\triangle v(x) + \left\langle Sx,\nabla v(x) \right\rangle - Bv(x), \,x \in \mathbb{R}^d, \,d \geqslant 2, \end{align*} for matrices A,B∈CN,NA,B\in\mathbb{C}^{N,N}, where the eigenvalues of AA have positive real parts. The sum A△v(x)+⟨Sx,∇v(x)⟩A\triangle v(x) + \left\langle Sx, \nabla v(x) \right\rangle is known as the Ornstein-Uhlenbeck operator with an unbounded drift term defined by a skew-symmetric matrix S∈Rd,dS\in\mathbb{R}^{d,d}. Differential operators such as L∞\mathcal{L}_{\infty} arise as linearizations at rotating waves in time-dependent reaction diffusion systems. The results of this paper serve as foundation for proving exponential decay of such waves. Under the assumption that AA and BB can be diagonalized simultaneously we construct a heat kernel matrix H(x,ξ,t)H(x,ξ,t) of L∞\mathcal{L}_{\infty} that solves the evolution equation vt=L∞vv_t=\mathcal{L}_{\infty}v. In the following we study the Ornstein-Uhlenbeck semigroup \begin{align*} \left[ T(t)v\right](x) = \int_{\mathbb{R}^d} H(x,ξ,t) v(ξ) dξ,\,x \in \mathbb{R}^d,\, t>0, \end{align*} in exponentially weighted function spaces. This is used to derive resolvent estimates for L∞\mathcal{L}_{\infty} in exponentially weighted LpL^p-spaces Lθp(Rd,CN)L^p_θ (\mathbb{R}^d,\mathbb{C}^N), 1⩽p<∞1\leqslant p<\infty, as well as in exponentially weighted CbC_{\mathrm{b}}-spaces Cb,θ(Rd,CN)C_{\mathrm{b},θ}(\mathbb{R}^d,\mathbb{C}^N).

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