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Explosion by Killing and Maximum Principle in Symmetric Markov Processes

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arxiv 2406.15974 v1 pith:44BVUN4C submitted 2024-06-23 math.PR

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keywords zetakillingpartciteequivalentforminftylambda
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abstract

Keller and Lenz \cite{KL} define a concept of {\it stochastic completeness at infinity} (SCI) for a regular symmetric Dirichlet form $(\cE,\cF)$. We show that (SCI) can be characterized probabilistically by using the predictable part $\zeta^p$ of the life time $\zeta$ of the symmetric Markov process $X=({\bf P}_x,X_t)$ generated by $(\cE,\cF)$, that is, (SCI) is equivalent to $\bfP_x(\zeta=\zeta^p<\infty)=0$. We define a concept, {\it explosion by killing} (EK), by $\bfP_x(\zeta=\zeta^i<\infty)=1$. Here $\zeta^i$ is the totally inaccessible part of $\zeta$. We see that (EK) is equivalent to (SCI) and $\bfP_x(\zeta=\infty)=1$. Let $X^{\rm res}$ be the {\it resurrected process} generated by the {\it resurrected form}, a regular Dirichlet form constructed by removing the killing part from $(\cE, \cF)$. Extending work of Masamune and Schmidt (\cite{MS}), we show that (EK) is also equivalent to the ordinary conservation property of time changed process of $X^{\rm res}$ by $A^k_t$, where the $A^k_t$ is the positive continuous additive functional in the Revuz correspondence to the killing measure $k$ in the Beurling-Deny formula (Theorem \ref{ma-sh}). We consider the maximum principle for Schr\"odinger-type operator $\cL^\mu=\cL-\mu$. Here $\cL$ is the self-adjoint operator associated with $(\cE,\cF)$ %with non-local part and $\mu$ is a Green-tight Kato measure. Let $\lambda(\mu)$ be the principal eigenvalue of the trace of $(\cE,\cF)$ relative to $\mu$. We prove that if (EK) holds, then $\lambda(\mu)>1$ implies a Liouville property that every bounded solution to $\cL^\mu u=0$ is zero quasi-everywhere and that the {\it refined maximum principle} in the sense of Berestycki-Nirenberg-Varadhan \cite{BNV} holds for $\cL^\mu$ if and only if $\lambda(\mu)>1$ (Theorem \ref{RMP}).

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  1. Homeomorphism of the Revuz correspondence for finite energy integrals

    math.PR 2025-02 accept novelty 7.0 of 10

    For finite-energy smooth measures, the Revuz map is a homeomorphism between the measure space with the Dirichlet-form metric and the PCAF space with the L2(P_{m+κ+ν0}) local-uniform topology.

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