Local time (mathematics) explained
In the mathematical theory of stochastic processes, local time is a stochastic process associated with semimartingale processes such as Brownian motion, that characterizes the amount of time a particle has spent at a given level. Local time appears in various stochastic integration formulas, such as Tanaka's formula, if the integrand is not sufficiently smooth. It is also studied in statistical mechanics in the context of random fields.
Formal definition
For a continuous real-valued semimartingale
, the local time of
at the point
is the stochastic process which is informally defined by
where
is the
Dirac delta function and
is the
quadratic variation. It is a notion invented by
Paul Lévy. The basic idea is that
is an (appropriately rescaled and time-parametrized) measure of how much time
has spent at
up to time
. More rigorously, it may be written as the almost sure limit
Lx(t)=\lim\varepsilon\downarrow
1 | |
| \{x-\varepsilon<Bs<x+\varepsilon\ |
} \, d[B]_s,
which may be shown to always exist. Note that in the special case of Brownian motion (or more generally a real-valued diffusion of the form
where
is a Brownian motion), the term
simply reduces to
, which explains why it is called the local time of
at
. For a discrete state-space process
, the local time can be expressed more simply as
[1]
}(X_s) \, ds.
Tanaka's formula
Tanaka's formula also provides a definition of local time for an arbitrary continuous semimartingale
on
[2] Lx(t)=|Xt-x|-|X0-x|-
\left(1(0,infty)(Xs-x)-1(-infty,(Xs-x)\right)dXs, t\geq0.
A more general form was proven independently by Meyer
[3] and Wang;
[4] the formula extends Itô's lemma for twice differentiable functions to a more general class of functions. If
is absolutely continuous with derivative
which is of bounded variation, then
F(Xt)=F(X0)+
F'-(Xs)dXs+
Lx(t)dF'-(x),
where
is the left derivative.
If
is a Brownian motion, then for any
the field of local times
has a modification which is a.s. Hölder continuous in
with exponent
, uniformly for bounded
and
.
[5] In general,
has a modification that is a.s. continuous in
and
càdlàg in
.
Tanaka's formula provides the explicit Doob–Meyer decomposition for the one-dimensional reflecting Brownian motion,
.
Ray–Knight theorems
The field of local times
associated to a stochastic process on a space
is a well studied topic in the area of random fields. Ray–Knight type theorems relate the field
Lt to an associated
Gaussian process.
In general Ray–Knight type theorems of the first kind consider the field Lt at a hitting time of the underlying process, whilst theorems of the second kind are in terms of a stopping time at which the field of local times first exceeds a given value.
First Ray–Knight theorem
Let (Bt)t ≥ 0 be a one-dimensional Brownian motion started from B0 = a > 0, and (Wt)t≥0 be a standard two-dimensional Brownian motion started from W0 = 0 ∈ R2. Define the stopping time at which B first hits the origin,
T=inf\{t\geq0\colonBt=0\}
. Ray
[6] and Knight
[7] (independently) showed thatwhere (
Lt)
t ≥ 0 is the field of local times of (
Bt)
t ≥ 0, and equality is in distribution on
C[0, ''a'']. The process |
Wx|
2 is known as the squared
Bessel process.
Second Ray–Knight theorem
Let (Bt)t ≥ 0 be a standard one-dimensional Brownian motion B0 = 0 ∈ R, and let (Lt)t ≥ 0 be the associated field of local times. Let Ta be the first time at which the local time at zero exceeds a > 0
Ta=inf\{t\geq0\colon
>a\}.
Let (
Wt)
t ≥ 0 be an independent one-dimensional Brownian motion started from
W0 = 0, then
[8] Equivalently, the process
(which is a process in the spatial variable
) is equal in distribution to the square of a 0-dimensional
Bessel process started at
, and as such is Markovian.
Generalized Ray–Knight theorems
Results of Ray–Knight type for more general stochastic processes have been intensively studied, and analogue statements of both and are known for strongly symmetric Markov processes.
See also
References
- K. L. Chung and R. J. Williams, Introduction to Stochastic Integration, 2nd edition, 1990, Birkhäuser, .
- M. Marcus and J. Rosen, Markov Processes, Gaussian Processes, and Local Times, 1st edition, 2006, Cambridge University Press
- P. Mörters and Y. Peres, Brownian Motion, 1st edition, 2010, Cambridge University Press, .
Notes and References
- Book: Ioannis . Karatzas . Steven . Shreve . 1991 . Brownian Motion and Stochastic Calculus . Springer .
- Book: Kallenberg . Foundations of Modern Probability . limited . New York . Springer . 1997 . 428–449 . 0387949577 .
- Book: Meyer, Paul-Andre . Un cours sur les intégrales stochastiques . Séminaire de probabilités 1967–1980 . . 1771 . 174–329 . 2002 . 1976 . 10.1007/978-3-540-45530-1_11 . 978-3-540-42813-8 .
- Wang . Generalized Itô's formula and additive functionals of Brownian motion . Zeitschrift für Wahrscheinlichkeitstheorie und verwandte Gebiete . 41 . 2. 153–159 . 1977 . 10.1007/bf00538419. 123101077 . free .
- Book: Kallenberg . Foundations of Modern Probability . limited . New York . Springer . 1997 . 370 . 0387949577 .
- D. . Ray . Sojourn times of a diffusion process . . 7 . 4 . 615–630 . 1963 . 10.1215/ijm/1255645099. 0156383 . 0118.13403 . free .
- F. B. . Knight . Random walks and a sojourn density process of Brownian motion . . 109 . 1 . 56–86 . 1963 . 1993647 . 10.2307/1993647. free .
- Book: Marcus . Rosen . Markov Processes, Gaussian Processes and Local Times . limited . New York . Cambridge University Press . 2006 . 53–56 . 0521863007 .