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Brownian meander : ウィキペディア英語版
Brownian meander

In the mathematical theory of probability, Brownian meander W^+ = \ is a continuous non-homogeneous Markov process defined as follows:
Let W = \ be a standard one-dimensional Brownian motion, and \tau := \sup \ , i.e the last time before ''t'' = 1 when W visits \. Then
:W^+_t := \frac |, \quad t \in ().
The transition density p(s,x,t,y) \, dy := P(W^+_t \in dy \mid W^+_s = x) of Brownian meander is described as follows:
For 0 < s < t \leq 1 and x, y > 0, and writing
: \phi_t(x):= \frac} \quad \text \quad \Phi_t(x,y):= \int^y_x\phi_t(w) \, dw,
we have
:
\begin
p(s,x,t,y) \, dy &:= P(W^+_t \in dy \mid W^+_s = x) \\
&= \bigl( \phi_(y-x) - \phi_(y+x) \bigl) \frac \, dy
\end

and
:
p(0,0,t,y) \, dy := P(W^+_t \in dy ) = 2\sqrt \frac\phi_t(y)\Phi_(0,y) \, dy.

In particular,
: P(W^+_1 \in dy ) = y \exp \ \, dy, \quad y > 0,
i.e W^+_1 has the Rayleigh distribution with parameter 1, the same distribution as \sqrt is an exponential random variable with parameter 1.
== References ==

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抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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