Brownian meander explained
In the mathematical theory of probability, Brownian meander
is a continuous non-homogeneous Markov process defined as follows:
Let
be a standard one-dimensional
Brownian motion, and
\tau:=\sup\{t\in[0,1]:Wt=0\}
, i.e. the last time before
t = 1 when
visits
. Then the Brownian meander is defined by the following:
} | W_ |, \quad t \in [0,1].
In words, let
be the last time before 1 that a standard Brownian motion visits
. (
almost surely.) We snip off and discard the trajectory of Brownian motion before
, and scale the remaining part so that it spans a time interval of length 1. The scaling factor for the spatial axis must be square root of the scaling factor for the time axis. The process resulting from this snip-and-scale procedure is a Brownian meander. As the name suggests, it is a piece of Brownian motion that spends all its time away from its starting point
.
p(s,x,t,y)dy:=
\indy\mid
=x)
of Brownian meander is described as follows:
For
and
, and writing
} \quad \text \quad \Phi_t(x,y):= \int^y_x\varphi_t(w) \, dw,
we have
\begin{align}
p(s,x,t,y)dy:={}&
\indy\mid
=x)\\
={}&l(\varphit-s(y-x)-\varphit-s(y+x)l)
dy
\end{align}
and
p(0,0,t,y)dy:=
\indy)=2\sqrt{2\pi}
\varphit(y)\Phi1-t(0,y)dy.
In particular,
\indy)=y\exp\{-y2/2\}dy, y>0,
i.e.
has the
Rayleigh distribution with parameter 1, the same distribution as
}, where
is an
exponential random variable with parameter 1.
References
- Durett, Richard . Iglehart, Donald . Miller, Douglas . 1977. Weak convergence to Brownian meander and Brownian excursion . The Annals of Probability . 5 . 1. 117–129 . 10.1214/aop/1176995895. free .
- Book: Revuz, Daniel . Yor, Marc . Continuous Martingales and Brownian Motion . 2nd . 3-540-57622-3 . Springer-Verlag . New York . 1999.