Chaos expansions and local times
Abstract
Nualart, David; Vives, Josep
Full text
Publicacions
Ma emá iques,
Vol
36
(1992),
827-836
.
A
bs ac
CHAOS
EXPANSIONS
AND
LOCAL
TIMES
DAVID
NUALAII'I'
AND
JOSEP
VIVES
In
his
no e
we
p o e
ha
he
Local
Time
a
ze o
o
a
mul ipa a-
ne ic
Wiene
p ocess
belongs
o
he
Sobole space
Dk
-
z
-,,2
o
any
e
>
0
.
We
do
his
compu ing
i s
Wiene
chaos
expansion
.
We
see
also
ha
his
expansion
con e ges
almos
su ely
.
Finally,
us-
ing he
same
ecl nique
we
p o e
simila
esul s
o
a
eno malized
Local
Time
o
he
au o¡
n e sec ions
o
a
plana
B ownian
mo ion
.
0
.
In oduc ion
and
no a ions
In
his
no e
we
i s
ob ai,n
he
Wiene
chaos
decomposi ion
o
he
local
ime
a
ze o
o
a
mul ipa ame e
Wiene
p ocess
.
We
also
show
ha
he
Wiene
chaos
se ies
con e ges
almos
su ely,
and
he
local
ime
belongs
o
he
Sobole
space
Dk-!/2- ,2,
o
any
e
>
0,
whe e
k
;
is
he
numbe
o
pa ame e s
o
he
Wiene
p ocess
.
The
las
pa
o
he
pape
is
de o ed
o
show
he exis en e
o a
eno malized
local
ime
o
he
au oin e sec ions
o
a,
plana
B ownian
mo ion
(Va adhan
eno maliza-
ion),
by
ineans
o
he
Wiene
chaos
expansion
.
Le
(T,
5, p)
be a
a- ini o
a omless
measu e
space
.
We
will
deno e
by
H
he
Hilbe space
L
2
(T,
B, p)
which
is
assumed
o
he
sepa able
.
Le
W
=
h
E
H}
be
a
ze o-mean Gaussian
p ocess
wi h
co a iance
unc ion
E
[W
( )
W
(g)]
=
( ,
g)
H
de ined
en
so ne
p obabili y
space
(S2,
F,
P)
.
We
will
suppose
ha
.'F
is
he
Q- ield
gene a ed
by
{W
(h),
h
E
H}
.
I
is
well-known
ha
any
squa e-in eg able
unc ional
on
52
has
an
o hogonal
decomposi ion
o
he
o m
00
F=E[F]+E
I, ( , ),
n=l
whe e
~,
E
L2(T')
(symme ic
squa e
in eg able
ke nel),
and
I
deno es
he
mul iple
Wiene -I ó
s ochas ic
in eg al
.
828
D
.
NUA
AW ,
J
.
VIVES
In his
amewo k we can
conside
he
de i a i e
ope a o
D
which
ac s
on
mul iple
s ochas ic
in eg als
in
he
ollowing
o m,
o
n
>_ 1,
E
T
.
NVe
can
in oduce
he
Sobole
spaces
Dn,2
o
a
E
R,
as
i is
done
in
[11]
.
A
unc ional
F
E
L
2(Q)
wi h
he
de elopmen
(1)
belongs
o
Da,2
i
and
only
i
n>1
Se
D-,2
=
naERDa
,
2
and
D«-,2
=
n7<,D
7,2
o
all
a E
R
.
and
E[H,,(Y)]
=
0
i
n
is
odd
.
D
.
In
( a( i
1.
.
.;
n))
=
n
II,,-
1
( n( l,
. . .
.
,L-1,
))
n!(1
+
n)~
11
,L
II2
<
00
.
1
.
P elimina ies
Le
us
i s
ecall
he
S oock o mula
(c
.
[8])
ha
gi es
he
Wiene
chaos
decomposi ion
o
a
unc ional
F
belonging
o
D°°,2
:
L
J
1!
In
(E[Dn
F])
.
.-o
n
.
We
will
also
make
use
o
he
He mi e
polynomials
.
Fo
each
n
>_
0,
we
will
deno e
by
H,
(x),
he
n h
He mi e
polynomial
de ined
by
(3)
H,,
(x)
en2/2
d
7
e-~
2/2
)
n>
0
.
,!
dx
7
Le
p,(x)
be
he
cen e ed
Gaussian
ke nel
wi h
a ian e
E
>
0
.
The
ol-
lowing
equali y,
which
ollows
immedia ely
om
(3),
ela es
he
de i a-
i es
p
(
,
n)
(x)
wi h
he
He mi e
polynomials
:
p
(n)(
x
)
ñ
!
E-n/2
pe(x)
H,,
(-)
'
n>
1
.
Lemma
1
.1
.
Le
Y
be
a
andom
a iable
wi h
dis ibu ion
N(0,
o-2)
.
Then
2
!
(0-2
-
1)
.
.
2-
m!
P oo
.
.
I
ollows easily
om
he
explici
o mula
o
He mi e
polynomials
:
[n/21
k
n-2k
n
k
!
(n
-
2k)
!
2k
'
k=o
and
he
momen s
o
a
Gaussian
andonl
a iable,
E[Y2,]
_í
2
2
~
.
Lemma
1 .2
.
Le ,
{FE}E>o
be
a a,mily o
squa e
in eg able
andoni
a iables
wi h
he
expansions
Assum,e
ha
i)
.,
con e ges
in
L
2
(T`),
when
E
10,
o
so ne
lLnc ion
,
E
L2(T'L)
.
,~=o
E
11
~s
Slip
{n!
112}
<
W
.
Tl~,e1
hc
allLily
F
E
con e ges
in
L
2
(Q)
o
F
=
°°
o
I'n
( z)
.
P o0
.
I
is
animmedia e
consequence
o
he
Lebesgue
do nina ed
con e gen e
heo e n
.
Le
So
be
he
Di ac
del a
unc ion
a
ze o
.
NVe can
conside
6o(W(h))
as
a,
dis ibu ion
on
he
Wiene
space
in
he
sense
o
Wa anabe
(c
.
[11])
.
Using
he
in eg a ion
by
pa s
o mula
on
he
Wiene
space
one can
show
ha
p,(W(h))
con e ges
in
B-1,2
o
bo(6V(h,))
(see
[5])
.
We
will
i s
compu e
he
Wiene
chaos
expansion
o
p
(W(h)),
and
om
i
we
will
deduce
he expansion
o
6o(W(h))
.
By
o mulas
(2)
and
(3)
we
ha e
p,
( 1
+'(h))
=
CI-IAOS
GNPANSIONS
AND
LOCAL
TIMES
829
2
.
Chaos
expansion
o
b
o
(W(h))
W
(n!1E
. 2E
~pE(IV(h))Hn
.
(
w
)
)]
I~
.(h®,~)
n=0
00
_l
E
p('n)(W(h))]
I,l(h®'y)
1L!
,L=o
The
expec a ion
appea ing
in
he
abo e
o mula
anislies
i
n
is
odd
because
pE
and
H,,
a e
e en
unc ions
.
On
he
o he
hand,
using
Lemma
1
.1
o
n=
2-ni
we
ob ain
x
H2, L
(-)
PEMPIJhll2(x)dx
E
_
(
21
(11h11
2
+E))-'/2
J
x
E
)
p_-111111
2 1
(E+1111
.11
1
)(x)dx
_
(2~(11h~~
2
+E))
1
~2
V2711,!
2
,
11
ni!
(~I
,Ia
-E
h
(1
2
+
E)
830
D
.
NUALART,J
.
VIVES
Finally,
om
(6)
and
(7),
we
ge
he
ollowing
expansion
(10)
e>0
.
(
-1)m
I2m(h
®2m
)
pe(W(h))
_
1
:
-+1/2
?n-o
27
2m
m
!
(11
h
112
+
E)
Le ing
E
end
o ze o
we deduce
he
Wiene
chaos
expansion
o
bo(W(h))
:
00
(9)
bo(W(h))
=o
(
-1
)
m
I
2m
(h®2 n)
27
2
m
m,!
II
h
II
2-+1
This
se ies
does
no
con e ge
in
L
2
(9),
because
11
bo(W(h))
112
=
m=0
(2m)
!
_
00
.
22m
(m!)2
27 il
hij
2
-
;
by
he
S iling
o mula
.
Obse e
ha
om
(9)
and
(10)
we
ob ain
i)
bo(W(h))E
D-1/2-,2
ii)
bo(W(h))0
D
-1
/
2
'
2
and
he
se ies
(9)
con e ges
in
he
no m
o
he
space
D-1/2-6,2,
o
any
Rema k
.
Mo e
gene ally
we
can ob ain
he
chaos
expansion
o
b,
;
(W
(h»
when
x
7~
0
6
.
(W
(h))
=
-p
11
lZ
II
()
x
I
n
(h
®n
)
2x
H
~h~~~
~~h~~ z
n!
.
n=o
3
.
Wiene
chaos
expansion
o
he
local
ime
o
a
mul ipa ame ic
Wiene
p ocess
In
his
sec ion
we
will
assume
ha
T
is [0,
1]
k
,
wi h
k
>_
1
.
Then
W
={W
(
),
E
T}
will
be
he
s anda d
Wiene
p ocess
on
T
.
We
will
deno e
by
[0, ]
he ec angle
[0,
1] x
.
.
.
x
[0,
k],
whe e
=
( ,,
..
. ,
k)
.
We
will
also
se
1
1
=
1
-...-
k
.
The
local
ime
o
W
can
be
o mally
de ined
as
(11)
L(
;
x)
=
&,
(14
7
s
)
d
.s
;
E
T,
x
E
R
.
!o~l
Al hough
o
any
ixed s,
b~(61
s)
is
no
an
o dina y
andom
a iable
bu
a
dis ibu ion
on
he
Wiene
space,
i
ums
ou
ha
he
in eg al
in (11)
has
a
smoo hing
e ec ,
and L(
,x)
is
a
well-de ined
andom
a iable
o
any
ixed
poin
_,
,
no
on
he
axes
.
We
will es ic
ou
analysis
o
he
case
x
=
0,
and
we
will
se
L( )
=
L( ,
0)
.
We
know
ha
L( )
=
o
.a]
So(14~
s
)
ds
can
be
ob ained
as
he
L
2
-limi o
(12)
LE( )
=
pe(ws
)
d, .s
o, l
when
e
ends
Lo
0
(see,
o
ins an e,
[2])
.
In
he
nex
heo em
we
will
compu e
he
Wiene
chaos
expansion
o
L(
)
.
Theo em
3
.1
.
We
ha e
ha
L( )
belongs
o
he
space
®
k--,2
,
o
any
poin
no
2
o a
he
a es,
and
i
holds
ha
L( )
=
P oo
..
(
-
1
.
),
n
2k
m
ó
27
2m a!(1-712)
CHAOS
EXPANSIONE
AND
LOCAL
TIMES
831
Mo eo e ,
L( )
does
no
belong
o
®~`-2
,2
.
00
(13)
L
E
( )
=
M=0
z
1,i
2, z,i
i=1
We
will
i s
compu e
he
Wiene
chaos
expansion
o
L
E
( ) applying
he
esul s o
he
p e ious
sec ion
.
F om
(8)
and
(11)
we
ob ain
I2z z
1®2m
(
-
1) n
o
s]
2~
2
m
.
ío
ds
.
,al
(I
s
I
+
.
),,+1/2
Then
he se ies
Z
:,°0
1
X
n
con e ges
a
.s
.
(14)
CHAOS
EXPANSIONS
ANll
LOCAL
TIMES
As
a
consequence
o
his
heo em,
i
F
is
a
squa e
in eg able
andom
a iable
wi h
he
de elopmen
(I
.),
and
L
=
n=o
hen
he
Wiene
chaos
expansion
(1)
con e ges
a
.s
.
In
pa icula
he
condi ion
(14)
is
sa is ied
i
F
belongs
o
he
Sobole
space
®e,2
o
any
e
>
0
.
Consequen ly, applying
Theo em
3
.1,
and
he
abo e
c i e ion
(14),
we
deduce
he
almos
su e
con e gen e
o
he
Wiene
chaos
expansion
o
he
local
ime
o
he
mul ipa a ne e
Wiene
p ocess
.
4
.
Reno malized
local
ime
o
he
au oin e sec ions
o
a
plana
B ownian
mo ion
Conside
now
W
=
{
(W¿,
W,
2 ),
E
[0,1]
}
a
s anda d
plana
B ow-
nian
mo ion
.
Le
us
w i e
[X]
=
X
-
.E
(X)
o
any
in eg able
andom
a iable
X
.
I
is
known
om
[6]
ha
(15)
L
E
_
[pE
(W -
Ws
)
pE
(W¿-
1V
.,2)]
ds d
o
<4< <1
con e ges
in
L2(Q)
;
as
E
ends
o
ze o
.
The
pu pose
o
his
sec ion
is
o
gi e
a
new
p oo
o his ac
by
means
o
he
esul s
ob ained
on
Sec ion
2
.
Theo em
4
.1
.
The
amily
o
andom
a iables
L
E
con e ges
as
E
ends
o
ze o,
in
®1/2-6,
2
,
o
any
6
>
0
.
In
pa icula ,
his
implies
he
con e gen e
in
L2(Q)
.
P oo
.-
Se
¿I
=
(s,
]
.
Applying
he
esul s
o
Sec ion
2,
we
ha e
(16)
I2e
1ó2e
1
2p
(
1021,
,
`
`'
ds
d ,
27
2
,
1
P,
!
p
!
Jo<s<e<1
(~
0
+
E)n+1
2+P=
.
n!(logn)
Z
11 ,
2
112
<
oe,
833
whe e
I2g
and
I2
P
deno e,
espec i ely,
he
mul iple
s ochas ic
in eg als
wi h
espec
o
he
B ownian
mo ions
GV
I
and
W
2
.
When
n
a ios
he
834
D
.
NUALART,
J
.
VIVES
e ms
appea ing
in
he
abo e
sum
a e
o hogonal
.
The
squa e
o
he
L
2
-no m
o
he
n h
e co
is
gi en
by
(17)
<
L
Obse e
ha
(2,,)2
22n
C+p
n
(e
!)2
(p
!)
2
E[I2e(lo)I2e(lo'),
~[
1
Z
p(
l
o)
I2
p()]
ds
d
du
d
;
[(,A~+E)
(IA*I+e)]n+l
whe e
0*
=
(u
;
]
.
We
can
es ima e
his
e m by
(2n)
!
:(
n
!
)2
(2e)
!(2p)
_
!(lo
;
1,J
.)
2n
(2~)222n(n!)2
P+p=n
e!p!
<
(2n)!
(I
I
0*
I)n+I
-_
(2n)
!
(2
7
)222n
(
n
!)2
On
he
o he
hand
we
claim
ha
¡
(18)
//
1
(s
;
]
1
(u,
]
1
2n
ds
d
du
d
<
J
'<
(
-
S
)n+I
(
V
-
U
)n+1
,
1
.
2
(19)
2
u<s<V<
(7L)
(TL
p
~
///
) p
e
(2n)
Jus<L
e+p=n
2e
<
`ei
<
(n
+
1)
max
(2ze
n)
O<Q<n
In
o de
o
show
(18)
we
will
decompose
he
in eg al
by
conside ing
he
di e en
posi ions
o
s,
,
u and
.
We
ha e
ha
he
le
hand
side
o
(18)
is
equal
o
(
-
(
_
s)n+1
S
)2n
ds
d
du
d
(
-
u)TL+1
+2
J
eL<s< <
Q
n
Q
*
I2n
(I
0
11
0*
I)
n+l
(e)
2
(2e)
<n+1
.
(
-
u)n+1
The
second
summand
in
(19)
can
be
es ima ed
as
ollows
2
(
_
~
-
s)n
du
ds
d
=
1
<
1
.
n
<s<
(
-
u)n+
i
n
(n
+
1)
n2
d
.s
d
du d
d
.s
d
du
d
.
ds d
du d
.
Fo
he
i s
e co,
we
ha e
<
CHAOS
EXPANSIONE
AND
LOCAL
TIMES
835
2
1
(
-
s)'
2
1
(
-
s)'
ds d
d
n
(
+I
ds
d ,
di)
-
~
+
I
~
< <
-
S)
n
< <
(
-8
)
-
1
2
~
(
-
$)2"
ds d
+
2
~
(
-
s
)n
ds d
n
(n
+
1)
n
2
S<
(1
-
.s)
,,
n
n
2
,
s<
n
_
1
2
(
V
-
n
[l_
(,
-
s)n
n
(n
+
1)
+
n
]
2
s
<
n
(1
-
s)n
1 1
2
n
(n
+
1)
+
? 2
<_
n2'
which
comple es
he
p oo
o (18)
.
The e o e
he
squa e
o
he
L
2
no nl
o
each
e co o
(16)
can
be
es ima ed
by
(2n)
!
3(?z,
+
1)
(27
)222n
(
n
!)2
Re e en es
n
2
d
.s
d
which
is
equi alen
o a
cons an
imes
i7,
-3
/2
.
Then
Le nma
1
.2
allows
o
comple e
he
p oo
o
he
heo em
.
1
.
N
.
BOULEAU
ANDF
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"Di -ichle
o as
and
analysis
on
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Wal e
de
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1991
.
2
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D
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GEMAN
AND
3
.
HOROWITZ,
Occupa ion
densi ies,
Annals
o
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8
(1980),
1-67
.
3
.
J
.
F
.
LE
GALL,
"Su
le
emps
local
d'in e sec ion
du
mou emen
b ownien
plan
e la
mé hode
de
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de
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ime
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7
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Da id
Nuala
:
Josep
Vi es
:
Facul a
de
Ma emá iques
Depa amen
de
Ma emá iques
Uni e si a
de
Ba celona
Uni e si a
Au óno na
de Ba celona
G an
Via,
585
08193
Bella e a
(Ba celona)
08007
Ba celona
SPAIN
SPAIN
Rebu
el
2
de
Ma i
de
1992