Chapter 3
Existence and Uniqueness of the
Solutions of SDE with
Two-Parameter Fractional
Brownian Motion
Next for K > 0 we define the closed sets
C[a,b],H(K) = {(P ? C[a,b],H :1(PI[a,b],H =
K}, and for (Pi ? C[ai,bi],ái,
(
CT,á1,á2,00(K, (P1, (P2) = x ?
CT,á1,á2,00 : x(a1, .) = (P1, x(., a2) = (P2,
Ix1T,á1,á2 = K,
sup
a1<t1<b1
|
kx(t1, .)I[a2,b2],á2 = K,
a2<sut2p<b2
|
}11x(., t2) 11 [a1 ,b1],á1 = K .
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By using the Hölder spaces of functions we obtain the
following local contraction property of an integral operator between such
spaces, which is useful in the next existence and uniqueness result.
Proposition 3.1. Let â1, â2 ? (1/2, 1] and
á1, á2 be such that âi > ái > 1 -
âi.Let g ? CR2,â1,â2 and b, ó : R ? Rbe
such that b is bounded and Lipschitz and ó ?
C2b(R) with ó" Lipschitz. Then for
every K > 0 and ai, bi ? R,ai < bi, i = 1, 2, there exists
å0 > 0 independent of ai, bi, such that for every (Pi ?
C[ai,ai+å0],ái(K) the operator
F :
C[a1,a1+å0]x[a2,a2+å0],á1,á2,00(2K, (P1,
(P2) ? C[a1,a1+å0]x[a2,a2+å0],á1,á2,00(2K, (P1,
(P2)
defined by
Existence and Uniqueness of the Solutions of SDE with
30 Two-Parameter Fractional Brownian Motion
Z s Z t Z s Z t
(F x)s,t = ?1(s) + ?2(t) + b(xu,v)dudv +
ó(xu,v)dg(u, v),
a1 a2 a1 a2
is a contraction.
Proof.(We refer to read [8] for more detail.) Clearly we have
~ ~ ~ ~
|
Z . Z .
a1 a2
|
~ ~
b(xu,v)dudv ~ = kb18(b1 -
a1)1-á1(b2 - a2)1-á2
~T,á1,á2,8
× [(b1 - a1)á1(b2 -
a2)á2 + 1] .
|
(3.1)
|
By using (2.18) it follows
~ Z.
~Z.
~~
a1a2
|
~ ó(xu,v)dg(u, v) ~=
(x)11T,á1,á2,811g11T,â1,â2
T,á1,á2,8
|
×(b1 - a1)â1?á1(b2 -
a2)â2?á2 [(b1 - a1)á1(b2 -
a2)á2 + 1] . (3.2)
Next
ó(x) ([s1, t1] × [s2, t2]) = (xt1,t2 - xt1,s2)
-(xs1,t2 - xs1,s2)
ó0 (ëxt1,t2 + (1 - ë)xt1,s2)
dë ó0 (ëxs1,t2+ (1 - ë)xs1,s2) dë
1
J
0 1
Z0
Z0 1 ó0 (ëxt1,t2 + (1 - ë)xt1,s2) dë
Then
ó(x) ([s1, t1] × [s2, t2]) = (xt1,t2 - xt1,s2 -
xs1,t2 + xs1,s2)
Z 1
+(xs1,t2 - xs1,s2) [ó0 (ëxt1,t2
+ (1 - ë)xt1,s2)
0
-ó' (ëxs1,t2 + (1 -
ë)xs1,s2)] dë.
(3.3)
Then (3.3) implies
{|ó(x) ([s1, t1] × [s2, t2])| =
1ó1181x1T,á1,á2 + Ió'IL1x(s1,
.)1[a2,b2],á2
)
Z 1 ~ dë
× ~ëkx(., t2)k[a1,b1],á1 + (1 -
ë)kx(., s2)k[a1,b1],á1
(t1-s1)á1(t2-s2)á1,
0
Existence and Uniqueness of the Solutions of SDE with
Two-Parameter Fractional Brownian Motion 31
and hence, if x ? CT,á1,á2,8(K, ?1, ?2), then
Ió(x)1T,á1,á2 = K
(1ó118 + kó0kL) .
(3.4)
From (3.2),(3.2) and (3.4) it follows that
Fx ? C[a1,b1]×[a2,b2],á1,á2,8
a
if x ? C[a1,b1]×[a2,b2],á1,á2,8nd also for
å1 > 0 enough small, Fx ?
C[a1,a1+å1]×[a2,a2+å1],á1,á2,8(2K, ?1, ?2) if
x ? C[a1,a1+å1]×[a2,a2+å1],á1,á2,8(2K, ?1,
?2).
Next we have
[ó(x) - ó(y)] ([s1, t1] × [s2, t2])
1
= (x - y)([s1,t1] × [s2, t2]) J ó0 (ëxt1,t2 + (1
- ë)yt1,t2) dë
+[(xs1,t2 -ys1,t2) -(xs1,s2 -ys1,s2)]
1
0
Z× [ó0 (ëxt1,t2 + (1 -
ë)yt1,t2) - ó0 (ëxs1,t2 + (1 - ë)ys1,t2)] dë
0 Z
1
+(xs1,s2 - ys1,s2) [ëx ([s1, t1] × [s2, t2]) + (1 -
ë)y ([s1, t1] × [s2, t2])]
Z 1 0
× ó00 (u(ëxt1,t2 + (1 - ë)yt1,t2) +
(1 - u) (ëxs1,t2 + (1 - ë)ys1,t2)) dudë
+(
Z
× [ó00 (u (ëxt1,t2 + (1 -
ë)yt1,t2) + (1 - u) (ëxs1,t2 + (1 - ë)ys1,t2))
0
-ó" (u (ëxt1,s2 + (1 -
ë)yt1,s2) + (1 - u) (ëxs1,s2 + (1 - ë)ys1,s2))] dudë.
(3.5)
0 Z 1 xs1,s2 - ys1,s2) [ë(xt1,s2 - xs1,s2) + (1 -
ë)(yt1,s2 - ys1,s2)] 0 1
If x, y ?
C[a1,a1+å1]×[a2,a2+å1],á1,á2,8(K, ?1, ?2), then
(3.5) yields
kó(x) -ó(y)1T,á1,á2 = C (K,
kól8, MótkL, kóitkL)
Mx - ylT,á1,á2. (3.6)
From (3.1), (3.2) and (3.6) it follows that there exists å2
> 0 enough small, independent of ai, bi, such that
11F
x-Fyl[a1,a1+å2]×[a2,a2+å2],á1,á2,8 =
dlx-yl[a1,a1+å2]×[a2,a2+å2],á1,á2,8, (3.7)
for some 0 < d < 1, and hence, denoting å0 =
min(å1, å2), we obtain that
Existence and Uniqueness of the Solutions of SDE with
32 Two-Parameter Fractional Brownian Motion
F :
C[a1,a1+å0]x[a2,a2+å0],á1,á2,00(2K, ?1, ?2) ?
C[a1,a1+å0]x[a2,a2+å0],á1,á2,00(2K, ?1, ?2)
is a contraction. 111
An existence and uniqueness result for ordinary differential
equations with Hölder continuous forcing is obtained in [11]. The global
solution is constructed, first in small time interval, when the contraction
principle can be applied, by using estimates in terms of Hölder norms. For
the two-parameter case we have the following result.
Theorem 3.1. Let â1, â2 ? (1/2, 1] and á1,
á2 be such that âi > ái > 1- âi. Let g ?
CR2,â1,â2 and b, ó : R ? R be such that b is
bounded and Lipschitz and ó ? C2 b (R) with ó"
Lipschitz. Then for every a1 < b1, a2 < b2 and ?i ?
C[ai,bi],ái with ?1(a1) = ?2(a2), the equation
t
x st=?1(s) ? 2(t) - ?1 (a1) + f i
b(xu,v)dudv
l a
2
(3.8)
+ Is ft
ja1 ó(xu,v)dg(u,v), (s, t) ? T,
has a unique solution in CT,á1,á2,00.
Proof. Let K > 0 be such that ?i ? C[ai,bi],ái(K). Then
from Proposition 3.1 we obtain the existence of the solution x of (3.8) on the
rectangle
[a1, a1 + å0] × [a2, a2 + å0], å0
independent of ai, bi (but dependent on K). If a1 + å0 < b1,
let n0 be the biggest integer such that n0å < b1. Then x ?
CT,á1,á2,00(2K) and inductively we obtain the existence of the
solution on
[a1 + å0, a1 + 2å0] × [a2, a2 + å0], ...,
[a1 + n0å0, b1] × [a2, a2 + å0], and then on
[a1, a1 + å0] × [a2 + å0, a2 + 2å0], ...,
[a1 + n0å0, b1] × [a2 + å0, a2 + 2å0],
and continuing again by induction we obtain the existence on T
. Let now x1, x2 be two solutions of (3.8). In particular, there is K > 0
such that x1, x2 ? CT,á1,á2,00(K). From (3.7) we deduce the
existence of å0 > 0 (which does not depend on ai, bi) and 0 < d
< 1 such that
1x1 - x21[a1,a1+å0]x[a2,a2+å0] = d1x1 -
x21[a1,a1+å0]x[a2,a2+å0],
and therefore x1 = x2 on [a1, a1 + å0] × [a2, a2 +
å0].Inductively (see the existence part) we obtain that x1 = x2 on T.
111
Existence and Uniqueness of the Solutions of SDE with
Two-Parameter Fractional Brownian Motion 33
Theorem 3.2. Let (BHt )tE[0,1]2 be a
two-parameter fractional Brownian motion with Hi ? (1/2,1) and let
ái,âi > 0 be such that 1/2 < âi < Hi,
âi > ái > 1-âi, i = 1, 2. Let b,
ó : R ? R be such that b is bounded and Lipschitz and ó ?
C2b (R) with ó" Lipschitz and let be
the processes {?i(t)}tE[0,1] such that almost surely ?1(0) = ?2(0) and
?i ? C[0,1],á,. Then with probability one the stochastic
equation
s t
Xs,t = ?1(s) + ?2(t) - ?1 (0) + b(Xu,v)dudv
f
0 0 (3.9)
+ 1s ft
0 ft (s,t)? [0,1]2,
has a unique solution {Xu,v}(u,v)E[0,1]2 with the
paths in C[0,1]2,á1,á2,00.
Proof. From the Kolmogorov criterion (see [2, 7]) it follows that
BH has â-Hölder paths, i.e., there exists a random
variable C such that for all ù ? Ù
2
(BH ([t, s])) (ù) ~~ = C(ù)
|
II
j=1
|
(sj - tj)â' . (3.10)
|
s pt
Therefore almost surely we have by Theorem 2.1.1 and (3.10) that
the Stieltjes integral
10 0 f (u, v)dBuH,v
is well defined for f ? C[0,1]2,á1,á2.
Now the result is a consequence of Theorem 3.1 applied pointwise.
Existence and Uniqueness of the Solutions of SDE with 34
Two-Parameter Fractional Brownian Motion
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