The intermediate arc-sine law
It is well-known that the sojourn time of Brownian motion B(t), t>0, namely Γ(B)= meas(s⩽1 : B(s)>0), obeys the arc-sine law, while, subject to the condition B(1)=0, is uniformly distributed. We present here the distribution of Γ( B) under the condition B( u)=0, for u⩾1. This is called the int...
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| Published in | Statistics & probability letters Vol. 49; no. 2; pp. 119 - 125 |
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| Main Authors | , |
| Format | Journal Article |
| Language | English |
| Published |
Elsevier B.V
15.08.2000
Elsevier |
| Series | Statistics & Probability Letters |
| Subjects | |
| Online Access | Get full text |
| ISSN | 0167-7152 1879-2103 |
| DOI | 10.1016/S0167-7152(00)00038-9 |
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| Summary: | It is well-known that the sojourn time of Brownian motion
B(t),
t>0,
namely
Γ(B)=
meas(s⩽1
:
B(s)>0),
obeys the arc-sine law, while, subject to the condition
B(1)=0, is uniformly distributed. We present here the distribution of
Γ(
B) under the condition
B(
u)=0, for
u⩾1. This is called the intermediate arc-sine law and it is shown that it converges to the classical one as
u→∞ and becomes the uniform law as
u=1. We also show that the first instant where the maximum of Brownian motion is attained follows the intermediate arc-sine law when the condition
B(u)=0,
u⩾1,
is assumed. It is pointed out that such “intermediate” arc-sine laws are connected with generalized Kac empirical processes. |
|---|---|
| ISSN: | 0167-7152 1879-2103 |
| DOI: | 10.1016/S0167-7152(00)00038-9 |