Doléans-Dade exponential explained

In stochastic calculus, the Doléans-Dade exponential or stochastic exponential of a semimartingale X is the unique strong solution of the stochastic differential equation dY_t = Y_\,dX_t,\quad\quad Y_0=1,where

Y-

denotes the process of left limits, i.e.,

Yt-=\lims\uparrowYs

.

The concept is named after Catherine Doléans-Dade.[1] Stochastic exponential plays an important role in the formulation of Girsanov's theorem and arises naturally in all applications where relative changes are important since

X

measures the cumulative percentage change in

Y

.

Notation and terminology

Process

Y

obtained above is commonly denoted by

l{E}(X)

. The terminology "stochastic exponential" arises from the similarity of

l{E}(X)=Y

to the natural exponential of

X

: If X is absolutely continuous with respect to time, then Y solves, path-by-path, the differential equation

dYt/dt=YtdXt/dt

, whose solution is

Y=\exp(X-X0)

.

General formula and special cases

X

, one has \mathcal(X)_t = \exp\Bigl(X_t-X_0-\frac12[X]^c_t\Bigr)\prod_(1+\Delta X_s) \exp (-\Delta X_s),\qquad t\ge0,where

[X]c

is the continuous part of quadratic variation of

X

and the product extends over the (countably many) jumps of X up to time t.

X

is continuous, then \mathcal(X) = \exp\Bigl(X-X_0-\frac12[X]\Bigr).In particular, if

X

is a Brownian motion, then the Doléans-Dade exponential is a geometric Brownian motion.

X

is continuous and of finite variation, then \mathcal(X)=\exp(X-X_0).Here

X

need not be differentiable with respect to time; for example,

X

can be the Cantor function.

Properties

l{E}(X)

has jumped to zero, it is absorbed in zero. The first time it jumps to zero is precisely the first time when

\DeltaX=-1

.

\exp(Xt)

, which depends only of the value of

X

at time

t

, the stochastic exponential

l{E}(X)t

depends not only on

Xt

but on the whole history of

X

in the time interval

[0,t]

. For this reason one must write

l{E}(X)t

and not

l{E}(Xt)

.

X

. This has application in the theory of conformal martingales and in the calculation of characteristic functions.

Useful identities

Yor's formula: for any two semimartingales

U

and

V

one has \mathcal(U)\mathcal(V) = \mathcal(U+V+[U,V])

Applications

l{E}(X)

of a continuous local martingale

X

is a martingale are given by Kazamaki's condition, Novikov's condition, and Beneš's condition.

Derivation of the explicit formula for continuous semimartingales

For any continuous semimartingale X, take for granted that

Y

is continuous and strictly positive. Then applying Itō's formula with gives

\begin{align} log(Yt)-log(Y0)&=

t1
Yu
\int
0

dYu

t1
2
2Y
u
-\int
0

d[Y]u =Xt-X0-

1
2

[X]t. \end{align}

Exponentiating with

Y0=1

gives the solution

Yt=\expl(Xt-X

0-12[X]
tr),   

t\ge0.

This differs from what might be expected by comparison with the case where X has finite variation due to the existence of the quadratic variation term [X] in the solution.

See also

Notes and References

  1. Doléans-Dade. C.. 1970. Quelques applications de la formule de changement de variables pour les semimartingales. Zeitschrift für Wahrscheinlichkeitstheorie und Verwandte Gebiete . Probability Theory and Related Fields. fr. 16. 3. 181–194. 10.1007/BF00534595. 118181229 . 0044-3719. free.