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Brownian excursion – Wikipedia – Enzyklopädie

Brownian excursion – Wikipedia

From Wikipedia, the free encyclopedia

Stochastic process

A realization of Brownian Excursion.

In probability theory a Brownian excursion process is a stochastic process that is closely related to a Wiener process (or Brownian motion). Realisations of Brownian excursion processes are essentially just realizations of a Wiener process selected to satisfy certain conditions. In particular, a Brownian excursion process is a Wiener process conditioned to be positive and to take the value 0 at time 1. Alternatively, it is a Brownian bridge process conditioned to be positive. BEPs are important because, among other reasons, they naturally arise as the limit process of a number of conditional functional central limit theorems.[1]

Definition[edit]

A Brownian excursion process,

e{displaystyle e}

, is a Wiener process (or Brownian motion) conditioned to be positive and to take the value 0 at time 1. Alternatively, it is a Brownian bridge process conditioned to be positive.

Another representation of a Brownian excursion

e{displaystyle e}

in terms of a Brownian motion process W (due to Paul Lévy and noted by Kiyosi Itô and Henry P. McKean, Jr.[2])
is in terms of the last time

τ{displaystyle tau _{-}}

that W hits zero before time 1 and the first time

τ+{displaystyle tau _{+}}

that Brownian motion

W{displaystyle W}

hits zero after time 1:[2]

Let

τm{displaystyle tau _{m}}

be the time that a
Brownian bridge process

W0{displaystyle W_{0}}

achieves its minimum on [0, 1]. Vervaat (1979) shows that

Properties[edit]

Vervaat’s representation of a Brownian excursion has several consequences for various functions of

e{displaystyle e}

. In particular:

(this can also be derived by explicit calculations[3][4]) and

The following result holds:[5]

and the following values for the second moment and variance can be calculated by the exact form of the distribution and density:[5]

Groeneboom (1989), Lemma 4.2 gives an expression for the Laplace transform of (the density) of

01e(t)dt{displaystyle int _{0}^{1}e(t),dt}

. A formula for a certain double transform of the distribution of this area integral is given by Louchard (1984).

Groeneboom (1983) and Pitman (1983) give decompositions of Brownian motion

W{displaystyle W}

in terms of i.i.d Brownian excursions and the least concave majorant (or greatest convex minorant) of

W{displaystyle W}

.

For an introduction to Itô’s general theory of Brownian excursions and the Itô Poisson process of excursions, see Revuz and Yor (1994), chapter XII.

Connections and applications[edit]

The Brownian excursion area

arises in connection with the enumeration of connected graphs, many other problems in combinatorial theory; see e.g.[6][7][8][9][10] and the limit distribution of the Betti numbers of certain varieties in cohomology theory.[11] Takacs (1991a) shows that

A+{displaystyle A_{+}}

has density

where

aj{displaystyle a_{j}}

are the zeros of the Airy function and

U{displaystyle U}

is the confluent hypergeometric function.
Janson and Louchard (2007) show that

and

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