2009/01/08 by Xia Chen, Wenbo Li, Chen, Xia +5
Mathematics · #FOS: Mathematics #Probability (math.PR) #math.PR
paper · pdf · doi:10.48550/arxiv.0901.1102
arxiv created 2009/01/08 · arxiv updated 2009/12/01
Let \Lxt ; (x,t)∈ R1× R1+\ denote the local time of Brownian motion and αt:=∫-∞∞ (Lxt)2 dx . Let η=N(0,1) be independent of αt. For each fixed t ∫-∞∞ (Lx+ht- Lxt)2 dx- 4ht\over h3/2 \stackrelL→(64 \over 3)1/2√αt η, as h\rar 0. Equivalently ∫-∞∞ (Lx+1t- Lxt)2 dx- 4t\over t3/4 \stackrelL→(64 \over 3 )1/2√α1 η, as t\rar∞.