Série Probabilités et applications
D. N UALART
M. S ANZ
Malliavin calculus for two-parameter processes
Annales scientifiques de l’Université de Clermont-Ferrand 2, tome 85, série Probabilités et applications, n
o3 (1985), p. 73-86
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MALLIAVIN CALCULUS FOR TWO-PARAMETER PROCESSES
D.
NUALART and
M.SANZ
Abstract. In this paper we
apply
the Malliavin Calculusto derive the existence of a
density
for the law of the solution of a stochastic differentialequation
with res-pect to a multidimensional two-parameter Wiener process.
AMS 1980
Subject
Classification:60H20,
60G30.0. Introduction. In this paper we prove the existence of a
density
for the
probability
law onRID
inducedby
the solution of the stochas- ticintegral equations.
2 1
z E
R2 ,
+ where W =(W 1,....Wd).
is a d-dimensional two-parameterz z z
Wiener process, x =
(x1 ,...,xm)~ R7,
andassuming
some conditionson the coefficients
Al
andBi.
If these coefficients aresmooth,
itj
is known
(cf.
Cairoli[2] , Hajek [4 ])
that(0.1)
has aunique
continuous
solution,
which has aparticular
Markov property. There exists a transitionsemigroup corresponding
to these Markov processes, but it acts on continuous functions over sets of the form{(x,t),
x~s}
U
{ (s,y) , y~ t }
and we cannot expect that theprobability
law ofXi
zsatisfy
a second orderpartial
differentialequation.
In the case of an
ordinary
stochastic differentialequation
withrespect to the Brownian
motion,
Malliavin hasdevelopped
in[6 ]proba-
bilistic
techniques
to show the existence and smoothness ofdensity
forthe solution of these
equations
underHormander’s
conditions. Alterna- tiveapproaches
to Malliavin’stheory
weregiven by Shigekawa 18 ],
Bis-mut
[1 ] and
Stroock[9 ].
It is not difficult to extend the Malliavin calculus to two-parameter Wiener functionals. However when weapply
thiscalculus to the solutions of
(0.1)
some technical difficulties appear, in relation with thefollowing
facts:i k
(a)
The innerproducts (in
the notation ofStroock)
arez z
(
not solutions of a similar system of
equations,
because the stochasticdifferentiation rules with respect to the two-parameter Wiener process involve the presence p of double
integrals
g over the set{(z,z’)~E
’R2
+ +, xR2
(b)
The system(0.1)
do notprovide
a flow of transformations ofRm.
Moreover if we consider a linear system ofequations,
the solutionis not
invertible,
ingeneral.
Here we have followed
Shigekawa’s presentation
of Malliavin Calcu-lus,
andusing
thistheory
we haveproved
the existence of adensity
forthe two-parameter Wiener functional
X z assuming
that the vector spacespanned by
the vector fieldsA1, ... ,A , Ai vAi,
ijij k. 1i, j d,
1 i,j,k d,...,
at thepoint
x(where
denotes the covarianti. j
derivative of A, in the direction of A.
),
isRm .
This property isj i.
strictly
weaker than the restrictedHormander’s conditions,
as we showin an
example. Actually
we haveproved (see [7 ])
that it alsoimplies
the smoothness of the
density.
1. Some results on Malliavin Calculus. The set of parameters will be T =
[ 0,1 ] 2 ,
with thepartial ordering
andonly
means that and
will denote the
rectangle {z
ET,
The
Lebesgue
measure of a Borelset
B C R2+
is denotedby lB l
.Our
probability
space is the canonical space associated to the d-dimensionaltwo-parameter
Wiener process. We also consider the filtration.{Fz ,
z ET} ,
where F isgenerated by
the func-tions c Q , s
z}
and the null sets of F. Thefamily
{ Fz
,z ET}
satisfies the usual conditions of[3 ].
>The
following
subsetof Q plays
animportant
role:H = there
i = 1,...,d,
> such thatdr ,
for any z E T and for anyi } .
H is a Hilbert space with the inner
product
A measurable function defined on is called a Wiener func- tional. A Wiener functional F: 0 --~ R is smooth if there exists
some n > 1 and a
C2-function
f onRn
such that(i)
f and its derivatives up to the second order have at most po-lynomial growth order,
Every
smooth functional isFrechet-differentiable,
and we haveWe also need the
operator
L defined on smooth functionals as fo- llows :where
For any
p > 1, Lp
will denote the space of Wiener functionals HF: Q ~ H such that
E( 11 P)
H If we fix w and a smoothfunctional
F , DF(w) :
H 20132013> R is a continuous linear map,and,
so, it may be considered as an element of H . In this sense we have DF ELp,
Hfor any p > 1 .
Let
1,
be the space of real valuedWiener functionals F such that there exists a sequence of smooth func- tionals
{F~,
k >1} satisfying:
in Lp1
is a
Cauchy
sequence inLH’ p2
and.
P3
is a
Cauchy
sequence inL .
For a Wiener functional F E we def ine DF = lim k
DFk
and LF = lim
LFk .
* is a Banach space with the normk i ~ J
we will say that a sequence of smooth functionals
1}
is anapproximating
sequence for F if lim( ifF - F k 11p+ IIDF - DF k 11p+
k K. P ~ P
continuously
differentiable function such that u and its first and second derivatives have at mostpolynomial growth
order. If we set F =then and the
following
differentiation rules hold:The next result is the main theorem in
Shigekawa’s
paper[8 ] adap-
ted to the Wiener process with two parameters, and with a
slight
diffe-rence
consisting
in the use of the spaceH(1,2;1).
Theproof given by Shigekawa
can be extended to these new conditions without anychange.
Theorem 1.1. Let F = be an
R -valued
two-parame-ter Wiener functional. We assume that F satisfies the
following
con-ditions :
Then,
theprobability
law of F isabsolutely
continuous with respect to theLebesgue
measure.In the next section we will
employ
this result to show the existen-ce of a
density
for the law inducedby
the solution of a stochastic diffe- rential system.2.
Application
to stochastic differentialequations.
Considermappings
A:
Rm
xRn
---~R. -n I2I Rd an d
B:P,7
xR n
20132013~f
s u ch that(i)
All their components have bounded and continuous first order derivatives.(ii)
x -A(x, Q)
and x ---~B (x, 0)
areslowly increasing
a
S
functions,
that isk(l
+x, )
and +I xl )
for some
positive integers
aand S
andpositive
constant k .Lemma
2.1.. Let a =
2 z ET}
be a continuous andadapted
n-di-mensional stochastic process such that for each
p_> 2,
E{sup oJ
z
E: T
Consider a continuous and
adapted
m-dimensional processz
such that E
{sup j X PI
00 for everyp > 2 ,
and fix v E T .z ET ~
’
Then,
there is aunique
continuous andadapted
n-dimensional process Y =satisfying
the stochastic differential systemand the
following
property holds:The solution of
~?.1) (with
anarbitrary
initialpoint v)
can beapproximated by polygonal paths,
as it is stated in the next lemma.k 2013k -k
For any k ->- 1 we consider the
set k
ofpoints (i2 ,j2 )
I, or u=vuz with
k k k
v
E k
or with vC- S k
oru=z .
Define~k (z) =
supu E k
uz and and
yk(z) (z) -
= inf inf{
uE k u>z .Lemma 2.2.
Let a = T}
andak = I ak(z) ,
z ET } ,
,k > 1 be continuous and
adapted
n-dimensional processessatisfying
for each
p > 2,
and let X be as in thepreceding
lemma. Consider theprocess defined
by (2.1).
Consider also theprocess
given by
where is a sequence of continuous and
adapted
m-dimensional stochastic processes such that for eachp > 2,
This result is a
generalization
to the two-parameter case of lemma V . 2 .1 from[5] .
..Lemma 2.3. Let X = z
(x1, ..., Xm)
z ’ zz E T be
the process which sa-tisfies
where A:
Rm
and B:Rm >R7
have bounded and continuous deriva- tives up to the second order. ,, Then i fori=l,... m ,
’ ’ ’Proof. For any n > I consider the process
X2013 =
de---- y n>1 p
z
(X
z ’ ’ z
fined
by
the recursive systemThe random variables z z E T are smooth functionals. We are
going
to prove that , n >
1}
is anapproximating
sequence forXi .
z g
z
First, by
lemma 2.2 we haveand u - sup ~
Fix an
element w E Q . Differentiating
termby
term we obtainwhere E i
du , and ei
is the. 11
From now on we will omit the
depen-
dence on w .
Denote
by
the derivative ofDX n,i
in the sensez ~ z
Then,
and for r E R we havez
For a fixed r let us consider the processes so-
lution of
Applying
lemma 2.2 to the processesIn consequence, is a
Cauchy
sequence in for any p >1,
and the derivative satisfiesfor
any h E H .
It remains to prove that is a
Cauchy
sequence inApplying
the differentiation rules wehave
where,
Consider now the stochastic differential system
with
It can be checked that
any
p ~ 1, therefore, 1 } Cauchy
sequencez
in
L , by
lemma 2.2applied
to the processesTheorem 2.4. Let X =
(X’,...,km)
be the solution of the stochas-201320132013201320132013201320132013
z z z
tic differential system
(0.1),
whereAi
andB i
have bounded and conti- jnuous derivatives of any order. Assume further that the
following
proper- ty holds:(P)
The vector spacespanned by
the vector fieldsA ,...,A ,
" 31at the
point
x has fullrank.
Then for any
point (s, t)
withst 1 0,
the law of the random vec- torXst
admits adensity
function.Proof .
We have to check conditions(i) , (ii)
and(iii)
of theorem 1.1.The first condition follows from lemma 2.3. Let
Uz (r)
be the processintroduced
in theproof
of lemma2.3,
which satisfies(2.2) ,
and callS’.. ::; ij
DXI ,
z z>H
H °Then,
f rom(2.3)
we have*
where ,
for any r, the process{ c 1(r, z) , z > r}
is defined as the so-lution of the stochastic differential system
By
Burkholder andHolder inequalities
and Gronwall’s lemma it is ea-sy to obtain the
following
estimate:-/,I
Therefore, by
means ofKolmogorov’s continuity criterium,
a version of{ Et’r,z),
rz }
can be choosen with almostsurely
continuouspaths.
For each
n>
I let be the process definedrecursively
For each
n>
1 letJ
be the process definedrecursively
The random
variables ( n ->- 11
are smooth functionalsJ
and
by
aslight
modification of lemma 2.3 one can see thatthey
form anapproximating
sequence for and that thisapproximation
is uni-j
form in r. The same conclusion is true for the random variables
{Ai (X ), n >1 r }
and A (X). j r1
Therefore,
afterhaving
noticed thataw
-- -
is a sequence of smooth functionals we deduce that n >
1 }
is anapproximating
sequencei.j
for S.. and so, condition
(ii)
of theorem 1.1 holds.ij .
Set
C
o = andC. kj
*A ~
Cj-ll . By
property(P)
there exists apositive integer j
0
such
j-1 Jo
that the linear span of U
C.
at thepoint
x has dimension m.j=o
JFor each
Q
denoteby
Ka (w)
the linear span of(A.(X .((w)
K x tk> ), > ,
Xl x ’0 , *0, k=i , k=l,...,d} ,
... , di
, and andK +(w)
= nK a(w) .
. We0
W>
>s
u
°> .
vepoint
out thefollowing
facts:(a) Kq(W)
increases with 0.(b) By
the Blumenthal zero-one
law,
K+(w)
does’ntdepend
on w a.s.(c)
Letp = inf
{J ,
dim Kc; > dim
K 0 +} .
. p is astrictly positive stopping
ti-o 0+
me with
respect
to the filtration0 Si ,
andp (w)
=
K0+(w)
..Assume that condition
(iii)
of theorem 1.1 is notsatisfied,
thatmeans
P{ W ,
infXTS(W)X
=01
>0 ,
where S =(S
, andconsequently
Then, using (2.4)
we haveBy (b)
and(c)
thisimplies
that thereexists X, IXI
= 1 such thatP{ X ortogonal to K (LO) *cr
>0 ,
in consequence = 0 for all
k=l,...,d.
Applying Itô’s
formula in the first coordinate(
see[10] ),
wehave ..
have .
A1 -
For any
t) , os}
is a continuous semimar-tingale, which
isequal
to zero on a set ofpositive probability,
in con-sequence on this set
In
particular,
Repeating
the same argument as before to the continuous semimar-tingale
for all A E
C ;
2 andrecursively,
which is
contradictory
with thehypothesis ~P).
0In the one parameter case, the existence of a
density
for the so-lution of a stochastic differential
equation
can beproved
underHorman-
Suppose B, Al,...,Ad
bounded derivatives of any order
greater
than orequal
to one. Thenthe
following assumption
suffices for the existence of adensity:
(H)
The vector spacespanned by
1 d 2 1i, j
i j
w d, [A., [A., A]],
1i,j, kd ...,
at thepoint
x isRID.
i
Actually,a
moregeneral condition, using
the Lie brackets formed with the vector field B as generators would be suf f icient.Cond i t ion ~P~ is
weakerthan (H) and,
inf ac t ,
theor em 2 . 4 can b eapplied
to afamily
of situations that did not appear in the one para- meter case.Consider,
forinstance,
thefollowing example.
Assume1 2 1
that
m=2,
d=l1 A2 1 = xl
and x =(0.0).
Then condition(H)
doesnot
hold
s and the one parameter solution t t t0 s s
1 1
2 _
2 12 _
t t t
0 s s
2
2 t t]
satisfies2X2 = (x1)2-
t.However
in the two-pa-t
t
rameter case, theorem 2.4 can be
used, and,
forst 1 0,
thejoint
dis-tribution of the random variables
X1
st =w1 ,
st stfR Rst z Wi dWI
z has a .density
onR2. Remark
that here the stochastic differentiation rules(cf.
claim that-
st]
, and~2
is not a function ofX1 .
st - - - st ~ f
References.
[1]. Bismut,
J.M.(1981). Martingales,
the Malliavin Calculus andhy- poellipticity
undergeneral Hörmander’s
conditions. Z. Wahrsch.verw.
Gebiete,
pp 469-505.[2]. Cairoli,
R.(1972).
Sur uneéquation
différentiellestochastique.
CRAS
274,
pp 1739-1742.[3 ]. Cairoli,
R. andWalsh,
J.B.(1975).
Stochasticintegrals
in theplane.
Acta Math.134,
pp 111-183.[4]. Hajek,
B.(1982).
Stochasticequations
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type and atwo-parameter Stratonovich calculus. Ann.
Probability 10,
pp. 451-463.
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N. andWatanabe,
S.(1981).
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P.(1978).
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M.(1984).
Malliavin Calculus for two-parameter Wiener functionals.
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I.(1980).
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M.(1978).
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Matematiques
Universitat de Barcelona
Gran