We are now ready to state the main result of rough paths theory: the continuity of solutions of differential equations with respect to the driving path.
Theorem: Let . Assume that
are
-Lipschitz vector fields in
. Let
such that
with .
Let be the solutions of the equations
There exists a constant depending only on
and
such that for
,
where is the control
The proof will take us some time and will be preceeded by several lemmas. We can however already give the following important corollaries:
Corollary: [Lyon’s continuity theorem] Let . Assume that
are
-Lipschitz vector fields in
. Let
such that
with .
Let be the solutions of the equations
There exists a constant depending only on
and
such that for
,
This continuity statement immediately suggests the following basic definition for solutions of differential equation driven by -rough paths.
Theorem: Let . Let
be a geometric
-rough path over the
-rough path
. Assume that
are
-Lipschitz vector fields in
with
. If
is a sequence that converges to
in
-variation, then the solution of the equation
converges in -variation to some
that does not depend on the choice of the approximating sequence
and that we call a solution of the rough differential equation:
The following propositions are easily obtained by a limiting argument:
Proposition:[Davie’s estimate for rough differential equations]
Let . Let
be a geometric
-rough path over the
-rough path
. Assume that
are
-Lipschitz vector fields in
. Let
be the solution of the rough differential equation
There exists a constant depending only on
and
such that for every
,
Proposition: Let . Let
be a geometric
-rough path over the
-rough path
. Assume that
are
-Lipschitz vector fields in
. Let
be the solution of the rough differential equation
There exists a constant depending only on
and
such that for every
,