VOL. 21 NO. (1998) 73-78
A CHANGE OF SCALE FORMULA FOR WIENER INTEGRALS OF CYLINDER FUNCTIONS ON ABSTRACT WIENER SPACE
YOUNG SIK KIM
GLOBAL ANALYSIS RESEARCH CENTER SEOUL NATIONAL UNIVERSITY
SEOUL
151-742,KOREA
(Received
April24,
1996 and in revisedformAugust 12, 1996)
ABSTRACT
The purpose of this paper is to establish the existenceofanalytic Wiener andFeynman
integrals foraclassofcertain cylinder functions whichisof the formF(x) f((h,,x)’,... (h,,,x)’),
x. B,
ontheabstractWiener space, and to establish therelationship betweenthe Wiener integral and the analytic
Feynman
integral forsuch cylinder functions on the abstract Wiener space.We
then establisha changeof scale formula for Wiener integrals of such cylinder functionson the abstract Wiener space.KEY WORDS AND PHRASES
Wienermeasure,analytic Wiener integral, analyticFeyn-
manintegral,changeof scaleformula.
1991
AMS SUBJECT CLASSIFICATION CODES
Primary28C20.1.
INTRODUCTION
In [4], Cameron
and Storvickexpressed the analytic Wiener andFeynman
integralsas the limitsof Wiener integrals for certain Banach algebra,S(L’[a,b])
of functionals. Using these results, they found a rather nice change of scale formula for Wiener integrals on a classical Wiener space[5]. In [13;14], Yoo, Yoon
and Skoug extended these results to an Yeh-Wiener space and toanabstract Wiener space.In [13], Skoug
andYoo
expressedtheanalyticWienerandFeynman
integralsasthelimitsof Wiener integrals, and thentheyestablished achange of scaleformula forWienerintegralson theFresnel class of the abstract Wiener space.In
this paper,we will show that the analytic Wiener andFeynman
integrals ofcertaincylinder functionsontheabstract Wiener spaceexist,andwewill establishthe relationship between the Wienerintegraland the analyticFeynman
integralfor suchcylinderfunctionsonthe abstract Wiener space. Usingtheseresults,
wewill establishachange of scale formula forWienerintegrals of suchcylinderfunctionsonthe abstract Wienerspace.Note
that the Fresnel classontheabstractWienerspaceconsistsof bounded functionsbut notallcylinderfunctionsareboundedingeneral.2.
DEFINITIONS AND PHRASES
Let H
bearealseparableinfinite dimensional Hilbert space withinnerproduct(., .>
andnormI" (V/’, "> Let I1" [10
beameasurablenormonH
withrespectto theGauss
measure#.Let B
denote thecompletion of
H
withrespecttoI1" II0. Let
denote the naturalinjection fromH
intoTypeset
by74 Y.S. KIM
B.
The adjoint operatori" of isone-to-one and mapsB"
continuously ontoadense subsetofH’,
whereH"
andB"
aretopologicaldualsofH
andB,
respectively.By
identifyingH
withH"
and
B"
withi’B’,wehaveatriplet(B’,H,B)
such thatB"
CH" H
CB
and(h,z) (h,x)
for all h in
B"
and zinH,
where(-,-)
denotesthe naturaldual pairing betweenB"
andB. By
awell known resultof
Gross [8;12],
#. -1 has auniquecountablyadditive extension v tothe Borel a-algebraB(B)
onB.
The triplet(B,H,v)
is calledan abstract Wiener space and v is calleda Wiener measure.We
denote the Wiener integralofa functionalF
byfs F(z)v(dx).
For
moredetailssee[8;12].
Let {e}=
denote acomplete orthonormal system inH
such thate’s
are inB’. For
eachh
H
and zB,
wedefineastochasticinnerproduct(-,-)~
betweenH
andB
asfollows:(h,z) ,hrn,, _. (h,%)(e,z),
if the limit exists,(2.1)
0, otherwise.
It
is well known[11]
that for every hH, (h,x)
exists for v-a.e, x inB
and it hasa Gaussian distribution with meanzeroandvarianceIhl -. Furthermore,
it iseasy to show that(h,x) (h,x)
forv-a.e, x inB
ifh EB, (h,x)
is essentiallyindependent of thecomplete orthonormal set used in itsdefinition,andfinallythat if{h,... h}
isanorthonormal setof elements inH,
then(h,x)~, (h,x)
areindependentGaussian functionals withmean zero andvariance one.Note
that if bothhand xareinH,
then(h,x) (h,x).
Throughoutthis paper, let
R
denote the n-dimensional Euclidean space and letC, C+,
andC
denote thecomplex numbers,thecomplex numberswith positive realpart,and thenon-zero complexnumbers with nonnegative realpart, respectively.DEFINITION
2.1Let (B, H,v)
be an abstract Wiener space.A
functionF
is calleda cylinderfunction
onB
if thereexists afinitesubset{g,-..
g}
ofH
such thatF(x) ((g,x)~, (g,x)~),
xB, (2.2)
where is a complex-valued Borel measurable functionon
R
k.It
is easy to show that there exists alinearlyindependent set{hi,-.. h}
ofH
suchthat every cylinder functionF
of the form(2.2)
isexpressedasF(x) f((h,x)~, (h,,x)~),
xB, (2.3)
where
f
isa complex-valued Borel measurable functiononR
". Thus we loseno generality in assuming that everycylinderfunctiononB
isof the form(2.3).
DEFINITION
2.2Let F
be a complex-valued measurable function onB
such that the integralJ(F; A) ./ F(A-1/2x)v(dx) (2.4)
exists forall real
A >
0. Ifthere existsafunctionJ*(F; z)
analyticonC+
such thatJ(F; A) J(F; A)
forall realA > 0,
thenwe defineJ*(F; z)
to be theanalytic Wiener integralofF
overB
withparameter z, andfor each zC+,
wewriteI"(F; z) J(F; z). (2.5)
Let
qbe a non-zeroreal number and letF
beafunctiononB
whose analytic Wienerintegral existsfor eachz inC+. If
the followinglimitexists, thenwecallitthe analyticFeynman
integral ofF
overB
withparameterq, andwewriteI1(F;q)=
limI(F;z), (2.6)
z---sq
where zapproaches-iqthrough
C+
and -1.DEFINITION
2.3Let (B, H, v)
beanabstract Wiener space.Let
nbeapositive integer, and let{h,-.. h}
beanorthonormal set of elements inH. For
1<
p< x,
let’(n; p)
denotetheclassof cylinder functions
F
withthe formasfollows:F() f((h,)~,..., (h,)~), e ,
where
f
]RC
isinLp(]R),
the spaceoffunctionswhose p-thpowersareLebesgue integrable onllanoLet ’(n; o)
denote theclass ofcylinder functionsF
with the formasfollows:F(x) f((hl,X)~, (h,.,,x)"),
xB, (2.8)
where jr
R
Cis inC0(R"),
the spaceofcontinuousfunctionsonR"
thatvanishatinfinity.We
will close this section by mentioning the following useful theorem which is called the WienerIntegrationFormula.THEOREM
2.4Let (B,H,v)
be an abstract Wiener space and let{h,---,h}
be an orthonormal setof elementsinH. Let F B
Cbeafunction definedbytheformulaF() ((h,,)~, (h,)~), ,
where
f :JR
C isaLebesgue measurable function. Then/zF(x)’(dx)=/Bf((h,x)","", (h, x)~) v(dx)
(-) f()-exp{-[l }d, (2.9)
where
(u,,.--, u) R", [[2 E3=I ’/"t32,
andd
du..,du,.,.In
the next section,wewilluseseveraltimesthefollowingwell-known integration formula:exp{-u + i}
duexp{- yg }, (2.10)
where is acomplex numberwith
Re > O,
b isarealnumber,
and -1.3.
THE MAIN RESULTS
We
willbeginthissectionby showingthatthe analytic Wiener integral ofF
exists for everyF _<p<_’(n; p)
andthat theanalyticFeynman
integralofF
existsforeveryF Y(n: 1).
THEOREM
3.1Let (B,H,v)
be anabstract Wienerspace and letF ’(n;p)
be giveny (.)
o:(.s),
wh< < .
The.:(i)
the analytic Wiener integrals ofF
exist, andfor every zC+,
z
.) /()exp{_Z
I""(F; z) (-) 5[[2} d, (3.1)
(ii)
for everynon-zeroreal numberq, and forF ’(n; 1),the
analyticFeynman
integral ofF
existsandisgiven
by
iq iq
i-l: } d- (3.2)
I’I(F; q) (-r) /() exp{-
and
d- du
du,.,.h
(,,..., ) e n , I1 := ,,
76 Y.S. KIM
PROOF. By
Theorem 2.4,we havethat for all realA >
0J(F; A) =/, F(A-1/2x)v(dx)
(-)- J’()exp{-l’l 2}
Let ’(F;) () f l()exp{-ll}d,
ze C+.
ThenJ’(F;A) J(F;A)
for all reelA>O.
e
iluorer’s
Theoremtosbott J’(F; z)
nanc
[unctono[ zn +.
Fksto[
I,
bythe DominatedConvergence Theorem,
ecnso
tbtJ’(; z) s
continuousonC+;
an
pproprte
dominating functions
obtainedalmostexactlyn
thefo1og gument.No et
be anyrectabesmpe
codcurveyng n +. e
nd only sbo thatJ’(F; z)
d 0.But
thiswill clearly follow from the CauchyIteal
Theorem if we canjustifymovg
the lineteal
alongr
inside the otherinteals
definingJ’(F;). Let sup{li
and
inf{Rez e ft.
IfF
belongs to(n; 1),
then the funetio()lI()l
dominates() II()lexp{-ll }
aditeable
onN . IfF
belongsto(;p) (1 <
p< ),
the
the function
()lI()lexp{-l }
dominates()lI()lexp{ -11 }
disiteeble
on
N
by H61der’s Inequality. IfF
belongsto(n; ),
then the fuctio() M p{-}
aomiates
() II()l exp{- }
adisinferable
onN,
whereM
aboundwithM
forallN .
Hence
we canapplyubini’sTheoremto theteel fr J’(F; )
d and thenwehavefr J’(F;
d 0, becau the functio
() exp{- }
analyticonC+.
Thenwehave established(a.1).
Finallytheproofof(a.2)
immediate.In
order toobtain our mainresults, wend thefollowinglemma:LNMMMN
g.t (B, H,u)
be abstract Wiener space and let{h,,..., h}
be Definition 2.a.Let F e (n;p)
be given by(2.7)
or(2.8),
where 1 p.
Then forevery+,
the functional2 isWiener
inteable
onB.
PNOO. By
Theorem2.4,
wehave thatfor everyC+,
( )
[(h,, )1,}. F()()
"
1
zl } d
=()= .Y()"e{-
d
d du...du.
We
canshowthat the ltteal
h:afinite value byusing thesameargument intheproof
of Theorem 3.1. Thustheproof
ofthislemma complete.THEOREM
3.8Let (B,H,)
be anabract Wienerspace and let{h,,..-,h}
beDefinition2.3.
t F e Y(n;p)
begivenby(2.7)
or(2.8),
where 1<
p< .
Then foreveryz
e E+,
the analyticWienertel I:(F; z)
ofF
isexpreed follows:z:(F; z) z xp{ ( z)
[(a,, )]}. ()(). (.)
PROOF. By Lemma 3.2,
the right hand sideof(3.3)
hasafinite value. Using Theorem2.4,
weobtainthat
exp{ (1 z)
-[(h, x)~]} F(x)u(dx)
2
exp{ (1-z)
]
[(h,,l l.I((,,) (h )(
I()’exp{-ll }
and
d du...du. Therefore,
we have where u(u,,.-. ,u,)
6R", Il E,=u,,
establhedtheequality
(3.3)
by(3.1)in
Theorem3.1Now
weshallexpress theanalyticFeynman inteal I"t(F; q)
ofF (n; 1)
the litofaquence ofWiener
inteals
ontheatract
Wiener space.THEOREM
3.4Let (B,H,v)
beanabstract Wienerspace and let{h,... ,h,}
be inDefinition 2.3.
t F
6(n; 1)
be givenby(2.7).
If{z}=
is aquenceof complexnumbers fromC+
such thatz
approhes -iq throughC+,
where q is a non-zero real number and-1,thenthe
analic Feynman inteal I"(F; q)
ofF
isexpressed follows:i,(F;q) 2(z)
9exp{ (1 z) [(h, x)]’} F(x)u(dx) (3.4) PROOF. By
Theorem2.4,
we canshow that(z) exp{ [(h,, x)]’} F(x) U()
=1
Zk Zk
() f().exp{-Tll }d,
and
d du...du.
Using the argument where u(u,,.-. ,u,)
6R
",1[= =,u,
similar tothat theproofofTheorem
3.1,
weconcludethatlim
<z)/ exp{ 1- z)[(h,,
2=1z).]} F(z)()
2i()e I().exp{-ll }d
-iq iq
where the last equality follows from
(3.2)
in Theorem 3.1 Thus theproof
ofthistheorem is complete.Now
we canobtainachange
of scaleformula for Wiener integralson(n; p)
which follows from Theorem 3.3and Definition2.2.THEOREM
3.5Let (B, H,)
beanabstract Wiener space.Let
p>
0 begiven and let{hi,--., h,,}
beasin Definition2.3. Then foreveryF
6’(n;p),
/s F(px) u(dx) p-" fe exp{ (p
2pl) [(h,,x)"12} F(x) ,(dx), (3.5)
78 Y.S. KIM where 1
PROOF.
First,we canshow that for all real z>
0,I(F;z) =/B F(z-1/2x)v(dx)
by Definition2.2. Using Theorem 3.3 and taking z
p-2
in the aboveequality, we have the desiredresult.EXAMPLE Let (B,H,v)
beanabstract WienerSpace
and n beapositive integer and let{hi,... ,h}
beanorthonormal setof elements ofH.
DefineF B C
byF() f((h,,)~,..., (h., ) ~) exp[--a ((h,, x)~) 21
3-’1
(3.6)
wherea isacomplex numberwith
Re(a) >
0.It
iseasy toseethatF
Ef31<<o’(n p)
sinceRe(a) > 0,
andsoF
satisfiesthehypothesis ofall the theorems in this paper.But
becauseofthespecial form ofF(see(3.6))
we caneasily evaluate the integralsonthe right-hand sideofequations(3.1)
and(3.2). Thus,
fornon-zero real q and z EC+,
it followsthatI(F" z) (--g) "
and thatIl(F q)
limqI(F z) (__=z)
2--qr
ACKNOWLEDGEMENT
Workonthis paperwaspartlysupportedby GlobalAnalysis ResearchCenter,
SeoulNational University,Korea.
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