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Rate of Growth of Local Times of Strongly Symmetric Markov Processes

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Seminar on Stochastic Processes, 1990

Part of the book series: Progress in Probability ((PRPR,volume 24))

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Abstract

Let S be a locally compact metric space with a countable base and let X = (Ω, f t , X t , P x), tR +,be a strongly symmetric standard Markov process with state space S. Let m be a σ-finite measure on S. What is actually meant by “strongly symmetric” is explained in [MR] but for our purposes it is enough to note that it is equivalent to X being a standard Markov process for which there exists a symmetric transition density function p t (x, y), (with respect to m). This implies that X has a symmetric 1-potential density

$${u^1}\left( {x,y} \right) = \int_0^\infty {{e^{ - t}}{p_t}\left( {x,y} \right)dt} $$
(1)

We assume that

$${u^1}\left( {x,y} \right) > \infty \forall x,y \in S$$
(2)

which implies that there exists a local time \(L = \left\{ {L_t^y,\left( {t,y} \right) \in {R^ + } \times S} \right\}\) for X which we normalize by setting

$${E^x}\left( {\int_0^\infty {{e^{ - t}}dL_t^y} } \right) = {u^1}\left( {x,y} \right)$$
(3)

It is easy to see, as is shown in [MR], that u 1(x, y) is positive definite on S × S. Therefore, we can define a mean zero Gaussian process G = {G(y), yS}, with covariance

$$E\left( {G\left( x \right)G\left( y \right)} \right) = {u^1}\left( {x,y} \right)\forall x,y \in S$$

The processes X and G, which we take to be independent, are related through the 1-potential density u 1(x, y) and are referred to as associated processes.

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References

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Marcus, M.B. (1991). Rate of Growth of Local Times of Strongly Symmetric Markov Processes. In: Çinlar, E., Fitzsimmons, P.J., Williams, R.J. (eds) Seminar on Stochastic Processes, 1990. Progress in Probability, vol 24. Birkhäuser, Boston, MA. https://doi.org/10.1007/978-1-4684-0562-0_12

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  • DOI: https://doi.org/10.1007/978-1-4684-0562-0_12

  • Publisher Name: Birkhäuser, Boston, MA

  • Print ISBN: 978-0-8176-3488-9

  • Online ISBN: 978-1-4684-0562-0

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