THEOREM (Itˆo’s formula in n-dimensions). Suppose that dX = Fdt + GdW,as
above. Let u : R
n
×[0,T] be continuous, with continuous partial derivatives
∂u
∂t
,
∂u
∂x
i
,
∂
2
u
∂x
i
∂x
j
,
(i, j =1,...,n). Then
(5)
d(u(X(t),t))=
∂u
∂t
dt +
n
i=1
∂u
∂x
i
dX
i
+
1
2
n
i,j=1
∂
2
u
∂x
i
∂x
j
m
l=1
G
il
G
jl
dt,
where the argument of the partial derivatives of u is (X(t),t).
An outline of the proof follows some preliminary results:
LEMMA (Another simple stochastic differential). Let W (·) and
¯
W (·) be indepen-
dent 1-dimensional Brownian motions. Then
d(W
¯
W )=Wd
¯
W +
¯
WdW.
Compare this to the case W =
¯
W . There is no correction term “dt” here, since W,
¯
W
are independent.
Proof. 1. To begin, set X(t):=
W (t)+
¯
W (t)
√
2
.
We claim that X(·) is a 1-dimensional Brownian motion. To see this, note firstly that
X(0) = 0 a.s. and X(·) has independent increments. Next observe that since X is the
sum of two independent, N(0,
t
2
) random variables, X(t)isN(0,t). A similar observation
shows that X(t) − X(s)isN(0,t− s) for t ≥ s. This establishes the claim.
2. From the 1-dimensional Itˆo calculus, we know
d(X
2
)=2XdX + dt,
d(W
2
)=2WdW + dt,
d(
¯
W
2
)=2
¯
Wd
¯
W + dt.
Thus
d(W
¯
W )=d
X
2
−
1
2
W
2
−
1
2
¯
W
2
=2XdX + dt −
1
2
(2WdW + dt)
−
1
2
(2
¯
Wd
¯
W + dt)
=(W +
¯
W )(dW + d
¯
W ) − WdW −
¯
Wd
¯
W
= Wd
¯
W +
¯
WdW.
We will also need the following modification of the product rule:
78