Regularity of Invariant Measures on Finite and Infinite Dimensional Spaces and Applications

Regularity of Invariant Measures on Finite and Infinite Dimensional Spaces and Applications
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DOI:
10.1006/jfan.1995.1123
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发表时间:
1995-10
影响因子:
1.7
通讯作者:
V. Bogachev;M. Röckner
V. Bogachev;M. Röckner
中科院分区:
数学1区
文献类型:
--
作者:
V. Bogachev;M. Röckner

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摘要在有限维和无限维状态空间E上,对于L = Δ + B·∇型算子,我们证明了测度μ求解方程L *μ = 0的正则性(即光滑性)的新结果。特别地,我们解决了I. Shigekawa在Δ = Δ H是gross - laplace, (E, H, γ)是抽象Wiener空间,B = - id E + v(其中v取Cameron-Martin空间H中的值)的一个猜想。利用高斯对数sobolev不等式,我们证明了μ在高斯测度γ下总是绝对连续的,并且密度的平方根在l2 (γ)中的1阶Malliavin检验函数空间中。进一步讨论了在无限维随机微分方程中的应用,并证明了L *μ = 0的一些新的存在性结果。这些包括关于“逆问题”的结果,即,我们给出了确保B是一个测度的(向量)对数导数的条件。我们还证明了μ对称的充分必要条件(即L在l2 (μ)上对称)。最后,本工作的很大一部分致力于研究L的对称测度的唯一性。我们通过相关(经典)狄利克雷形式的不可约性来描述具有唯一性的情况。
Abstract In this paper we prove new results on the regularity (i.e., smoothness) of measures μ solving the equation L *μ = 0 for operators of type L = Δ + B · ∇ on finite and infinite dimensional state spaces E . In particular, we settle a conjecture of I. Shigekawa in the situation where Δ = Δ H is the Gross-Laplacian, ( E , H , γ) is an abstract Wiener space and B = −id E + v where v takes values in the Cameron-Martin space H . Using Gross′ logarithmic Sobolev-inequality in an essential way we show that μ is always absolutely continuous w.r.t. the Gaussian measure γ and that the square root of the density is in the Malliavin test function space of order 1 in L 2 (γ). Furthermore, we discuss applications to infinite dimensional stochastic differential equations and prove some new existence results for L *μ = 0. These include results on the "inverse problem", i.e., we give conditions ensuring that B is the (vector) logarithmic derivative of a measure. We also prove necessary and sufficient conditions for μ to be symmetrizing (i.e., L is symmetric on L 2 (μ)). Finally, a substantial part of this work is devoted to the uniqueness of symmetrizing measures for L . We characterize the cases, where we have uniqueness, by the irreducibility of the associated (classical) Dirichlet forms.