1991
DOI: 10.1214/aop/1176990540
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Intersection Local Times for Infinite Systems of Brownian Motions and for the Brownian Density Process

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Cited by 23 publications
(19 citation statements)
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“…We remark that this theorem gives a rigorous meaning to the informal expression (43) in [36] ((B H 1 ) ) 2 . The relationship between the parameters follows from Proposition 2.1(b) and Theorem 3.2.…”
Section: Theorem 32 Let Y Be As In Lemma 31 Then the Real Processmentioning
confidence: 92%
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“…We remark that this theorem gives a rigorous meaning to the informal expression (43) in [36] ((B H 1 ) ) 2 . The relationship between the parameters follows from Proposition 2.1(b) and Theorem 3.2.…”
Section: Theorem 32 Let Y Be As In Lemma 31 Then the Real Processmentioning
confidence: 92%
“…A is a Borel set of R with finite Lebesgue measure |A|, B (1) and B (2) are independent, and E(B (1) …”
Section: The Rosenblatt Processmentioning
confidence: 99%
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“…For f, f[ as before, 4 E Sd, and The following result is from [12], and has antecedents in [9]: On the other hand, the branching Brownian motions that, in the infinite density limit, provide a particle picture for the super Brownian motion have a local time in only one dimension, an intersection local time up to three dimensions, and a renormalisable self-intersection local time only in dimensions one and two.…”
Section: (mentioning
confidence: 94%
“…2. Now we only recall that for a continuous centered Gaussian process X = (X t ) t∈ [0,1] in S (R d ), an intuitive definition of the SILT of X up to time t is given by the formal expression t 0 t 0 X s ⊗ X r , δ(x − y)ϕ(x) ds dr , (1.1) where ⊗ denotes the tensor product in S (R d ), δ is the Dirac distribution, ϕ ∈ S(R d ), and · , · is the duality on S (R 2d ) × S(R 2d ). We focus on the following primary questions:…”
Section: Introductionmentioning
confidence: 99%