7.3 Itˆo Equations in Belopolskaya-Daletskii Form 157
dξ(t) = exp
ξ(t)
(a(t, ξ(t))dt + A(t, ξ(t)))dw(t) (7.23)
is well-defined where w(t) is a Wiener process in R
k
(see Example 7.4) and exp
is the exponential mapping of a connection on M . Introduce a Riemannian
metric on M (for example, the first fundamental form generated by the inner
product in R
k
). If M is a compact manifold, the connection and metric are
compatible in the sense of Definition 7.35. The existence of a strong solution
for all t ∈ [0, ∞) is proved as above.
We conclude this section with a description of a class of stochastic differ-
ential equations on infinite-dimensional Hilbert manifolds that will be used
below. This class is a particular case of the equations on infinite-dimensional
manifolds considered in [23] (see also [35, 66], where equations in Stratonovich
form are considered).
Let M be a Hilbert manifold, H be a connection on M and G(·, ·)be
a strong Riemannian metric on M (the term “strong” means that G(·, ·)
determines the topology of the model space in tangent spaces to M;the
description of Riemannian metrics and connections on infinite-dimensional
manifolds can be found, e.g., in [172], see also Chapter 10 for the particular
case of groups of diffeomorphisms). Notice that in this case Definition 7.9 of
a uniform Riemannian atlas and Definition 7.35 of compatible metrics and
connections remain valid.
Let α(t, m) be a vector field and A(t, m) be a field of linear operators
A(t, m):R
n
→ T
m
M where m ∈ M, t ∈ [0,l]andR
n
is the Euclidean space
in which a Wiener process w(t) takes values. As in the finite-dimensional
case the pair (α, A) is called an Itˆo vector field and for this field (and for the
exponential mapping exp of the connection H) equation (7.18) is well-defined.
For convenience of reference we formulate an existence of solution theorem
for (7.18) in this case as a separate statement.
Theorem 7.41 Let the above mentioned objects G, H, α(t, m) and A(t, m)
be given on a Hilbert manifold M and let the conditions of Theorem 7.36 be
satisfied for them. Then for every m
0
∈ M there exists a strong and strongly
unique solution ξ(t) of equation (7.18) with initial condition ξ(0) = m
0
,well-
defined for all t ∈ [0,l].
Note that Theorem 7.41 is valid for every finite-dimensional Euclidean
space R
n
. As for Theorem 7.36, the proof of Theorem 7.41 is reduced to
Theorem 7.20. Recall (see Remark 7.21) that the proof of Theorem 7.20 is
analogous to that of Theorem 2.2 in [23] (proved in the infinite-dimensional
case). The modification mentioned in Remark 7.21 is also valid here.