For a continuous real-valued semimartingale ${\displaystyle (B_{s})_{s\geq 0}}$ , the local time of ${\displaystyle B}$  at the point ${\displaystyle x}$  is the stochastic process which is informally defined by

${\displaystyle L^{x}(t)=\int _{0}^{t}\delta (x-B_{s})\,d[B]_{s},}$ 

where ${\displaystyle \delta }$  is the Dirac delta function and ${\displaystyle [B]}$  is the quadratic variation. It is a notion invented by Paul Lévy. The basic idea is that ${\displaystyle L^{x}(t)}$  is an (appropriately rescaled and time-parametrized) measure of how much time ${\displaystyle B_{s}}$  has spent at ${\displaystyle x}$  up to time ${\displaystyle t}$ . More rigorously, it may be written as the almost sure limit

${\displaystyle L^{x}(t)=\lim _{\varepsilon \downarrow 0}{\frac {1}{2\varepsilon }}\int _{0}^{t}1_{\{x-\varepsilon <B_{s}<x+\varepsilon \}}\,d[B]_{s},}$ 

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 ${\displaystyle dB=b(t,B)\,dt+dW}$  where ${\displaystyle W}$  is a Brownian motion), the term ${\displaystyle d[B]_{s}}$  simply reduces to ${\displaystyle ds}$ , which explains why it is called the local time of ${\displaystyle B}$  at ${\displaystyle x}$ . For a discrete state-space process ${\displaystyle (X_{s})_{s\geq 0}}$ , the local time can be expressed more simply as^[1]

${\displaystyle L^{x}(t)=\int _{0}^{t}1_{\{x\}}(X_{s})\,ds.}$ 

Tanaka's formula also provides a definition of local time for an arbitrary continuous semimartingale ${\displaystyle (X_{s})_{s\geq 0}}$  on ${\displaystyle \mathbb {R} :}$ ^[2]

${\displaystyle L^{x}(t)=|X_{t}-x|-|X_{0}-x|-\int _{0}^{t}\left(1_{(0,\infty )}(X_{s}-x)-1_{(-\infty ,0]}(X_{s}-x)\right)\,dX_{s},\qquad t\geq 0.}$ 

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 ${\displaystyle F:\mathbb {R} \rightarrow \mathbb {R} }$  is absolutely continuous with derivative ${\displaystyle F',}$  which is of bounded variation, then

${\displaystyle F(X_{t})=F(X_{0})+\int _{0}^{t}F'_{-}(X_{s})\,dX_{s}+{\frac {1}{2}}\int _{-\infty }^{\infty }L^{x}(t)\,dF'_{-}(x),}$ 

where ${\displaystyle F'_{-}}$  is the left derivative.

If ${\displaystyle X}$  is a Brownian motion, then for any ${\displaystyle \alpha \in (0,1/2)}$  the field of local times ${\displaystyle L=(L^{x}(t))_{x\in \mathbb {R} ,t\geq 0}}$  has a modification which is a.s. Hölder continuous in ${\displaystyle x}$  with exponent ${\displaystyle \alpha }$ , uniformly for bounded ${\displaystyle x}$  and ${\displaystyle t}$ .^[5] In general, ${\displaystyle L}$  has a modification that is a.s. continuous in ${\displaystyle t}$  and càdlàg in ${\displaystyle x}$ .

Tanaka's formula provides the explicit Doob–Meyer decomposition for the one-dimensional reflecting Brownian motion, ${\displaystyle (|B_{s}|)_{s\geq 0}}$ .

The field of local times ${\displaystyle L_{t}=(L_{t}^{x})_{x\in E}}$  associated to a stochastic process on a space ${\displaystyle E}$  is a well studied topic in the area of random fields. Ray–Knight type theorems relate the field L_t to an associated Gaussian process.

In general Ray–Knight type theorems of the first kind consider the field L_t 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 edit

Let (B_t)_{t ≥ 0} be a one-dimensional Brownian motion started from B₀ = a > 0, and (W_t)_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, ${\displaystyle T=\inf\{t\geq 0\colon B_{t}=0\}}$ . Ray^[6] and Knight^[7] (independently) showed that

${\displaystyle \left\{L^{x}(T)\colon x\in [0,a]\right\}{\stackrel {\mathcal {D}}{=}}\left\{|W_{x}|^{2}\colon x\in [0,a]\right\}\,}$

(1)

where (L_t)_{t ≥ 0} is the field of local times of (B_t)_{t ≥ 0}, and equality is in distribution on C[0, a]. The process |W_x|² is known as the squared Bessel process.

Second Ray–Knight theorem edit

Let (B_t)_{t ≥ 0} be a standard one-dimensional Brownian motion B₀ = 0 ∈ R, and let (L_t)_{t ≥ 0} be the associated field of local times. Let T_a be the first time at which the local time at zero exceeds a > 0

${\displaystyle T_{a}=\inf\{t\geq 0\colon L_{t}^{0}>a\}.}$ 

Let (W_t)_{t ≥ 0} be an independent one-dimensional Brownian motion started from W₀ = 0, then^[8]

${\displaystyle \left\{L_{T_{a}}^{x}+W_{x}^{2}\colon x\geq 0\right\}{\stackrel {\mathcal {D}}{=}}\left\{(W_{x}+{\sqrt {a}})^{2}\colon x\geq 0\right\}.\,}$

(2)

Equivalently, the process ${\displaystyle (L_{T_{a}}^{x})_{x\geq 0}}$  (which is a process in the spatial variable ${\displaystyle x}$ ) is equal in distribution to the square of a 0-dimensional Bessel process started at ${\displaystyle a}$ , and as such is Markovian.

Generalized Ray–Knight theorems edit

Results of Ray–Knight type for more general stochastic processes have been intensively studied, and analogue statements of both (1) and (2) are known for strongly symmetric Markov processes.

• Tanaka's formula
• Brownian motion
• Random field

• K. L. Chung and R. J. Williams, Introduction to Stochastic Integration, 2nd edition, 1990, Birkhäuser, ISBN 978-0-8176-3386-8.
• M. Marcus and J. Rosen, Markov Processes, Gaussian Processes, and Local Times, 1st edition, 2006, Cambridge University Press ISBN 978-0-521-86300-1
• P. Mörters and Y. Peres, Brownian Motion, 1st edition, 2010, Cambridge University Press, ISBN 978-0-521-76018-8.