A NNALI DELLA
S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze
K OICHIRO I WATA
The inverse of a local operator preserves the Markov property
Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 4
esérie, tome 19, n
o2 (1992), p. 223-253
<http://www.numdam.org/item?id=ASNSP_1992_4_19_2_223_0>
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the
Markov Property
KOICHIRO IWATA
0. - Introduction
The present work was
originally
motivatedby
theanalysis
of adegenerate multicomponent
Gaussiangeneralized
random field which arises from thesimplest example
of quantum gauge fieldtheory,
i.e. theelectromagnetic
fieldLet
{X(~p); ~p
CCo’(E 4 -+
be ageneralized
random field with an index set D =Co (E4 --~ ]R4),
which is identified with the space of smooth differential 1-forms over the 4-dimensional Euclidean spaceE4
withcompact
supports, such thatwhere d is the exterior derivative
operator
and A is theLaplacian acting componentwise.
We note that the bilinear form(dp,
isdegenerate
and invariant under the
replacement by
wheref
ECÜ(E4). Speaking
inconnection with
physics,
describes theelectromagnetic
gaugepotential
field in Landau’s gauge
through
theanalytic
continuationprocedure
to theMinkowski space. Because of its
degeneracy
we can notapply
knowngeneral
results to discuss the Markov
property
of{X(~p)}. (See
e.g.[16], [30]
andalso
[11].
In[8], [15], [28]
and[29]
the relation betweenlocality
and Markovproperty
is discussed in the framework ofpotential theory).
On the other hand thefollowing
idea is known amongphysicists (see
e.g.[10], [20], [21]
and[42])
as restriction to transversal test forms. We setDt
=(p e P; 6p
=0},
where6 is the coderivative operator and consider its Hilbert space
completion M
withrespect
to(dp, (-A) -2 dp)L2.
Since this bilinear form isnon-degenerate
onDt,
N may be embedded in the space oftempered
currentsS’(E4 ---+ ]R4)
andPervenuto alla Redazione il 18 Febbraio 1991.
Now the
point
is that theoperator
8d is nolonger degenerate
on M. Thusapplying
Nelson’s arguments[23]
for theproof
of the Markov property of the free Euclideanfield,
one can show a Markovproperty
ofE Dt }
(note
thechange
of indexsets).
However the filtration subordinate to the lattergeneralized
random field has astrange
character which is causedby
the lack of C°°-module structure forDt.
Because of this we aim here to discuss the Markov property of ED }
and not that of{X (~p); ~p E Dt } .
Before
describing
how thequestion
above issolved,
we mention verybriefly
about the definition of Markovproperties.
We agree that asimple-minded
definition of Markov
property
for random fields E is thefollowing:
e D},
the u -fieldgenerated by e D},
E areconditionally independent
EaD}
for any open subset D withboundary
aD. However this definition excludes a lot ofinteresting examples.
In fact it is known that any translation
homogeneous
Gaussian Markov random field in the above sense must be asingle
Gaussian random variable if the dimension d is greater than 1(see
e.g.[17], [37]
and[38]).
McKean[22]
proposed
ageneral prescription by considering
thegerm u-fields.
His definition of Markov property,roughly speaking,
involves all normal derivatives of the random field at aD. Then one isnaturally
led to thequestion
howprecisely
oneshould know about the normal
derivatives,
forinstance,
whether it is sufficientto know the normal derivatives up to certain fixed order or not.
Wong
and Zakai[39]
introduced a notion of localizable random currents and gave ageometrical
formulation of normal derivatives of random currents. Moreover
they presented interesting examples
of Gaussian random currents with Markov property in their sense. Amont the recentdevelopments
weparticularly
mention the workby Albeverio, Hoegh-Krohn
andSurgailis [3]
oninteger
valued random fieldsarising
fromgrand
canonical Gibbsfields,
where the basic idea is that the Markov property must bepreserved
under localmanipulations
and is similar to ours. As for thesubject
related to Euclidean quantum fields we share in the benefits of the surveyby
Albeverio andZegarlinski [6].
Concerning
notions of Markovproperty
there exists anotherimportant
onebesides the one in terms of
germ u-fields:
Given an openncovering {D+, D_ }
of
Ed,
one can ask whether ED+}
and ED_ }
areconditionally independent given
ED+ n D_ }
or not. Preiss andKotecky [27] pointed
out that if the above condition holds for any open
coverings {D+, D_ }
ofEd,
then
actually
the random field{Xt }
is Markov in McKean’s sense but not the other way around if one is concerned withgeneralized
random fields. Moreoverthey
clarified the difference between these two notions.Our method for the
analysis
of(o.1 )
is the factorization of the covariance bilinear form. This ispossible
when one embeds a differential form of order say r, r =0,1, ... , d,
as one of thehomogeneous components
of a section of thealternating algebra
bundlegenerated by
thecotangent
bundle. We note that if we can make theembedding
in such way that eachhomogeneous component
ismutually independent,
then the Markov property of totalsystem implies
thatof the
original
randomcurrent.
Then one can ask whether the extended randomcurrent is Markov or not. We consider the system determined
by
thefollowing elliptic
system:where X2
is,
forinstance,
a random currentderiving
from Gaussian whitenoises.
Then we can transfer the
degeneracy concerning
the deRahm-Hodge-Kodaira decomposition,
which is notlocal,
into that relative to the order of differentialforms,
which is local in contrast. Now thequestion
is whetherXl
inherits the Markov property of X2 relatedby (d + 6)Xi
=X2. Actually
ifX2
is Gaussiandistributed,
this set up works very well as Rozanov showed[31], [32].
This type ofproblems
with d + 6replaced by
localoperators
withanalytic symbols
werediscussed
extensively
in one-dimensionalsettings by
Doob[7],
Levinson and McKean[19],
and Okabe[24], [25].
On the other hand multidimensionalelliptic
cases were discussed
by Surgailis [34], [35]
andOsipov [26].
In 1979 Kusuoka[18]
gave acomprehensive
answer to thequestion by showing
that the inverse maps of invertible local linearoperators
preserve the Markovproperty
relativeto open
coverings (not
in the sense ofMcKean)
ingeneral
multidimensionalcases. However we find that the kernel of the linear
operator d
+ 6 is not smallenough
toapply
Kusuoka’s result indiscussing
our veryquestion.
Thus not asmall
part
of the present work isprecisely
devoted toremoving
the harmful effect of the nontrivial kernel of d + 6.Our formulation of the
problem
is as follows: LetIE1 and
be realvector bundles over a
paracompact
manifold M and L a linear differentialoperator mapping
C°°-sections of E2 to those ofJE1. r(IE1 )
stands for the space of all Coo -sections ofEi
andD1
for the space of all COO -sections of Ei with compact supports. We use theanalogous
notations for thecorresponding
spaces forE2. Suppose
we aregiven
twogeneralized
random fields{Xl (~); ~
EDl }
and E related
by
The heart of the argument is an
appropriate
choice of atolopogy
onÐ1
withrespect
to which is continuous inprobability.
LetN2
be a Frechet spaceconsisting
of smooth sections of E2satisfying
thefollowing postulates:
(0.3) N2
containsD2
and the inclusionD2
-N2
is dense.(0.4)
L :N2
-r(IEl )
isinjective
and there exists a linear map G :Ðl
-Jl2
such that thefollowing diagram
holds(0.5)
If(£n)
CÐl
andG£n -
0 inN2
thenX1(çn) ---+
0 inprobability.
(0.6) If p
EM2
satisfies supp p c D for some open subset D of M, then there exists a sequence(qn)
cD2
with supp qn c D such that y~ inM2.
Let
{D+, D_ }
be an opencovering
of M. We shall say that{D+, D_ }
is{L, H2}-admissible,
foreach E
EPi
withsupp E
c D+ there exists apartition
ofunity {x+, x_ }
subordinate to{D+, D_ }
such that EN2
and there existsa sequence
(gn)
cDl
withsupp gn
cD+
n D- such thatG~ 2013~ X-G~
in~2.
Under the above
setting
our main theorem in the present work asserts thefollowing.
THEOREM 0.7. Let
{L, H2 }-admissible
opencovering of
M.
If
supp q CD+}
and supp q CD_ }
areconditionally independent given
supp v CD, n D- 1,
then thecorresponding
relationalso
holds for {X1(ç)}.
In order to discuss the system
(d + 6)Xi
=X2
with a Gaussian white noise XL, all we have to do is to put,where is the exterior
algebra generated by V.
Then we canverify
that allthe
postulates (0.3)-(0.6)
are satisfied and moreover any opencovering ID,, D_ }
of
Ed is
admissible relative to{d+6, )~21.
Thus we succeed inproving
the Markovproperty for the random current characterized
by (o.1 ).
We also discuss the so called
sharp
Markov property for a first orderelliptic system a X1
=X2
with a white noise X2. Let V be arepresentation
space of the Cliffordalgebra
overV,
then theoperator 0, usually
called the Dirac operator,acts on V-valued smooth functions on
Ed .
Moreover X 1 and X2 are definedas
generalized
random fields with a common index space D =Co (Ed
-~V).
We localize the
generalized
random fieldE D }
tohyperplanes
in thespirit
ofWong
and Zakai. Let be a sequence of mollifierstending
to6o
the Dirac mass at 0 E R. For each q ECÜ(JRd-1
-~Y )
the sequence0 ?y)}
of random variables converges in
probability
as8 1 o.
We shall denote the limitby (We identify
ahyperplane
inEd
with I and hence the tensorproduct js
is understood under thisidentification).
What we meanby
thesharp
Markov property and what we shall prove is thefollowing:
THEOREM
0.8. ~{Xi(~);
supp ~p c(-00,0)
x andsupp Sp c
(o, oo)
x areconditionally independent
(D~);
TJ E
Co (I~gd_ 1 --, V ) }.
On the other hand we shall
give
anexample showing
that thesplitting
6 -field may
spread
to the whole 6 -field contrary to what isintuitively suggested by
theterminology ’sharp
Markovproperty’.
Before
briefly describing
the contents, let us mention that these discussionscan be
applied
to prove the Markovproperty
of thegeneralized
random fieldinvestigated
in ourprevious
works[2] (collaborated
with S. Albeverio and R.Høegh-Krohn)
and[4] (with
S. Albeverio and T.Kolsrud).
Inparticular
the useof
adjective
’markovian’ whichappeared
in the title of[2]
isjustified by
thepresent work.
In Section 1 we mention two
mutually non-equivalent
notions of Markovproperty
andclarify
the differencefollowing
Preiss andKotecky.
In Section 2after some comments on Kusuoka’s result we shall prove our main theorem and illustrate how
(0.7)
isapplied. Finally
in Section 3 we examine thesharp
Markov
property
for the first orderelliptic
system.1. - Two
nonequivalent
notions of Markovproperty
To
begin
with we want toclarify
what we meanby
Markovproperties
ofgeneralized
random fields.Throughout
this paper(Q, 7, P)
denotes theunderlying probability
spacewhich we assume to be
complete.
N denotes the trivial sub u-field{A
E1; P(A)2
=P(A)}.
Let M be a paracompact C°°-differentiable manifold. We consider afamily
of random variables{X(~p); ~p
E indexedby
the space of all smooth functions on M withcompact
supports.(If
onelikes,
can be
replaced by
a certain spaceconsisting
of smooth sections ofsome vector bundle. Even the linear structure is
dispensable
except for Theorem(1.21)).
DEFINITION 1.1. If the
family {X(~p)}
is linear in thefollowing
sense, wecall it a
generalized
randomfield:
We
identify
and{X’(~p)}
ifX(p)
=X’(p)
a.s. forall p
ECü(M).
Given a
generalized
random field{X(Qp)},
the a -field F isnaturally
filtered.That
is,
we introduce afamily
of sub u-fields c M,open},
where’eachof
~
is defined as follows:We shall call the
family
of a -fields the canonicalfiltration
subordinate to thegeneralized
random field{X(~p)}.
In addition to the usualproperty,
satisfies thefollowing:
(1.2) if {Ua}
is an opencovering of
D, thenlD
=v1uu.
Of course this is due to the paracompactness of M and the
C°°(M)-module
structure of
C~ (M).
NOTATION 1.3. means that two sub Q -fields
.7,
and X- areconditionally independent given Jõ.
The u-field
Jõ
is often called asplitting
a -field forÃ
and 7- - We note thatLEMMA 1.4.
Suppose 10
C 1-. Thenequivalent
to that= a.s.
for
all bounded7,-measurable functions f.
In this paper we are concerned with several notions of Markov
properties.
DEFINITION 1.5. We say that the filtration and hence is MI-Markov if for any open
convering {D+, D_ }
of M.REMARK 1.6. It is often
practical
to add some condition on opencoverings.
For
example
werequire
thatinf{ p(x, y);
x EMBD+,
y EMBD_ }
> 0, where p is a fixedcompatible
metric. This weaker form is called the 0-Markov property.In order to define the second notion of Markov
properties,
which issimply
called Markov property in much of the literature on the
subject,
we need tointroduce a
family
of sub u-fields indexedby
closed subsets of M. Let C bea closed subset. We consider the
following
sub u-field:DEFINITION 1.7. We say that the
filtration {FD}
is MII-Markov, if for any open subsets.As an illustration we consider a white noise. Let G be a
locally compact
Hausdorff group with a countable base. We assume that M is aG-homogeneous
space, i.e. G acts on M
transitively
from the left.DEFINITION 1.8.
By a
white noise on M we mean a system of random variables{W (A)}
indexedby relatively compact
Borel subsets of M which satisfies thefollowing postulates.
(i)
If aremutually disjoint,
then aremutually independent
and(ii)
If thenW(An) -
0 inprobability.
(iii)
The system{W (A)}
ishomogeneous
relative to theG-action, i.e.,
whence =
stands for theequivalence
in distribution.It is known that the distributions of such random variables
{W(A)}
mustbe
infinitely
divisibleprovided
M is uncountable.(See
e.g.[1].
Note that awhite noise over an uncountable space must be
non-atomic).
In fact there existsa
unique
continuousconditionally positive
definitefunction 1b
on R such thatwhere u
is the G-invariant Radon measure on M(unique
up tomultiplicative constants). y
is called theLevy
characteristic of the white noise. Inparticular
if
{ W (A) }
is mean 0 Gaussiandistributed, i.e., (
some c > 0,{W (A) }
is called a Gaussian white noise.2
The
following procedure
is standard. We set.M
:_ { f :
M - R; boundedmeasurable, vanishing
outside a compactset}.
It is easy to see that there exists a
unique family
of random variables{Y( f ); f E M}
such that(1.10 i) Y(cl/1 + c2 f2)
=C1Y(,fl) -~ C2Y(f2)
a.s. ci , c2 E R and E M.( 1.10 ii)
Iff n j 0,
thenY( fn) -
0 inprobability.
(1.10 iii)
a.s. for Arelatively
compact,where
1 A
is the indicator function of the set A. The random variableY(f)
iscalled the stochastic
integral
off
withrespect
to the white noise{W (A)}.
Itimmediately
follows thatWe define a
generalized
random field{X(~p)} by restricting
the index set toCü(M).
Thefamily (X(p))
shall be called a white noisegeneralized
randomfield (or simply
a whitenoise).
LEMMA 1.12. If D is an open subset of M, then
1D
= cPROOF. The
proof
is doneby showing
thatW(K)
is1D-measurable
foreach compact subset K of D..
By
virtue of this Lemma we see that the white noise(X(p))
is MI-Markovwith
respect
to any opencovering.
LEMMA 1.13.
~c
= A CC}
V Nfor
all closed subsets.PROOF. Let A be a
relatively
compact Borel subset. Thenby (1.12)
wehave - . -
where
C,
is theE-neighbourhood
of C with respect to acompatible
metric.Since
C( 1
C asc 10,
themartingale
convergence theoremimplies
thatThis shows that
n Fc,
c cC}
V N. On the other hand we seeby (1.12)
that the r.h.s. c Thus we get the desired relation..The Lemmas
(1.12)
and(1.13)
tell us that the canonical filtration subordinate to a white noise isparticulary good natured, i.e.,
We now return to the
general
situationagain.
PROPOSITION 1.14. Let be an MI-Markov
filtration.
ThenConversely,
has the property(1.2),
then( 1.15) implies
the MI-Markov property.The
following
version of themartingale
convergence theorem is used in theproof
of( 1.14) .
LEMMA 1. 16. Let H be a Hilbert space and P be a set
of orthogonal projectors
in H.Suppose
P is directed in thefollowing
sense:for
anypair
Pi, P2 E P there existsP3
E P withP3
P, andP3
P2. Thengiven
x E Hthere is a sequence C P such that
Pnx -; Qx,
whereQ
is theorthogonal
projector
onton Image
P.PEP
PROOF OF 1.14. Let
f+, f-
andfo
be bounded -,.7c- -
andmeasurable functions
respectively.
If D is an open setcontaining C+
n C-, then{D
UC+,
D UC_}
is an opencovering
and(D
UC+)
n(D
UC-)
= D. Thereforewe see that
by using
the MI-Markov property.Applying ( 1.16)
we havewhich shows
( 1.15 ) .
Next we prove the converse statement. Given an open
covering {D+, D_ }
of
M,
choose another opencovering {D+,o, D_,o}
so thatD+,o
cD+
and
D_,o
c D-. We consider two families :=D+,o
U and:=
D-,o
U where A is the collection of all open subsets A withA c D+ n D-.
Clearly
it follows thatD+,A
cD+, D-,A
c D- for A E~t,
and covers D+,
{D_,A }
covers D- coversD+ n D_ .
Therefore,
thanks to the property(1.2),
weget
Let
f
be a boundedFD-
-measurablefunction, then,
if A :D B, we seeby ( 1.15)
that
Hence
by (1.16)
and(1.17)
we obtain ] a.s..According
to
(1.4)
thisimplies
the MI-Markov property.REMARK 1.18.
Concerning
thetopology
of M, it is theT4-separation
axiom that we
actually exploited
in theproof
of the converse relation. This remark alsoapplies
to thefollowing
Theorem(1.23).
This
proposition
has thefollowing
immediatecorollary.
THEOREM 1.19.
Every
MI-Markovfiltration
possesses the MII-Markov property as well.REMARK 1.20. In
general
the MI-Markovproperty
isstrictly
stronger than the MII-Markovproperty.
As anexample
we consider a translationhomogeneous
Gaussian
generalized
random field onEd
withindependent
values at everypoint (cf. [9]).
It is of course MII-Markov. However it is known that the MI-Markovproperty
is validsolely
for the white noise among such a class(see
e.g.[18]
and
[27]).
In the
following
discussion we want tosingle
out the difference between the MI- and MII-Markovproperties.
The next Theorem and(1.22)
are due toPreiss and
Kotecky [27].
THEOREM 1.21. Let be an MI-Markov
generalized
randomfield.
Then
it follows
thatPROOF.
(i)
The relation~D+
CFMBD-
VFD,ND-
must beproved. Let p
be an element of with supp p C D+. Given an open set D D
MBD-,
choose ~o+ E so that supp ~p+ c D n D+ and supp
(~p - p+)
cD+
n D-(using
apartition
ofunity).
Then we haveBecause
of
the MI-Markov property,Therefore
eRtx(’P)E
is.tD-
measurable ifM(D- , i.e.,
it is
:1MBD- -measurable.
On the other hand we can find a
family
ofprobability
measureson R such that
Consider the
following
sets:Then
SZn
EfD+nD-
andQn > Q
as n - oo. We now fix n andsuppose It 1.
Then we see that n
Hence the l.h.s. is V
fD+nD- -measurable.
Sincemust be V
fD+nD- -measurable.
(ii)
Letf and g
be bounded:Tc- -
and:TMBC-
-measurable functionsrespectively. According
to(1.14)
we haveSince V
by
thealready proved
relation(i),
we get:Tc+
c:Tc+nc_.
Thiscompletes
theproof. ·
REMARK 1.22. In the
previous
Remark(1.20)
we mentioned anexample
ofMII-Markov
generalized
random fields without MI-Markov property.Actually
theProposition (1.21) suggests
an alternative way to show the failure of MI-Markovproperty by proving
the existence of opencoverings {D+,D-}
of which donot
satisfy
the condition(i)
in(1.21) (see [27]).
An outline of the argument is as follows: We consider a mean 0 translationhomogeneous
Gaussiangeneralized
random field with
independent
values at everypoint.
Then its covariance bilinear form determines aunique
differential operator P. Provided P is not a constant,one can show that if D is a
non-empty
bounded open set with smoothboundary,
then there exists a non-trivial solution
f
forP f
= 0 onRdB8D
with finite norm( f , f )
oo. This willimply
that VTheorem
(1.21)
and Remark(1.22)
tell us that the difference between the MI-Markov property and the MII-Markov property lies in thevalidity
ofcondition
(i)
in(1.21).
In fact we can prove thefollowing
theorem.THEOREM 1.23. Let
IYDI be an
MII-Markovfiltration
with the property(1.2).
Then thefollowing implies
the MI-Markov property:Before
going
into theproof
we mention asimple
fact.LEMMA 1.24. 7- and
70
be subu-fields of
~.If
then(1+
V.70)-L(F-
VTo)1 To.
PROOF OF
(1.23).
Given an opencovering {D+, D_ },
choose an open subsetDo
withMBD-
cDo
cDo
cD+.
We consider afamily {DA
:=Do
UAIAEA,
where A is the collection of all open subsets A with A c D+ n D-. Since
(MBDA)
U(DA n D-)
=D_ BaDA,
we seeby
theassumption
and the property(1.2)
that for each ALet
fl, f 2
andf 3
be bounded andFaDA -measurable
functionsrespectively.
Thenby
the MII-Markov property and(1.24)
we haveTherefore
is .1D+nD- -measurable,
iff
is.1D-
-measurable. On the other hand a similar argument to(1.17)
shows that.1D+
=V(.1DA
V.1aDA). Thus, according
to( 1.16},
] isFD+nD- -measurable.
Thiscompletes
theproof:
REMARK 1.25. The canonical filtration subordinate to a random field satisfies the condition in
(1.23)
and hence the MI- and MII-Markov propertyare
equivalent
for randomfields.
Finally
we discuss thequestion
whether the MI-Markovproperty
isequivalent
for twogeneralized
random fields with the same finite dimensional distributions or not. We shallgive
an affirmative answer under some mildcontinuity assumption.
We agree that isequipped
with the Schwartztopology, i.e.,
thestrongest locally
convextopology
which makes all natural mapsCü(D) ---+ Cü(M) continuous,
where D runsthrough
acovering consisting
of
relatively
compact open subsets and thetopology
on eachCü(D)
is inducedby
the compact opentopology
onC°°(M). (This topology
isindependent
ofthe choice of open
coverings).
Theresulting
Hausdorfftopological
vector space shall be denoteby P(M).
MoreoverD’(M)
stands for thetopological
dual spaceof P(M) and (’, ’)
for the canonicalpairing
in the dualpair (P’(M), D (M) ~ .
DEFINITION 1.26. We say that a
generalized
random field isstochastically
continuous, if Spimplies
inprobability.
We dare to omit the word
sequentially,
since it turns out that this weaker form is sufficient in mostinteresting
cases.(See
e.g.[13]
on relatedsubjects).
Suppose
M is second countable. Then the Schwartztopology
is a strict inductive limit of nuclear Frechettopologies.
Thereforegiven
astochastically
continuousgeneralized
randomfield,
thanks to Minlos’theorem,
we obtain a consistent system ofprobability
measures on duals of nuclear Frechet spaces.According
to
Kolmogorov
the obtained countableprojective
limit is a-additive.However,
even if we do not assume the second
countability
for M, theprojective
limitis 6-additive..
To prove this we recall that each connected component of a paracompact manifold is second countable. SinceD’(N),
where Nruns
through
all connectedcomponents
of M, thea-additivity
follows(cf. [41]).
In the
following
discussion we assume that M is second countable till thisassumption
is canceled. What isfavorable,
when M is secondcountable,
is that thetopological u-field
forD’(M) equipped
with the weak *topology
is standard Borel and moreover all Borel
probability
measures are Radon. Inparticular
we have thefollowing
LEMMA 1.27.
If a generalized random field
on(Q, .1,P)
isstochastically
continuous, then there exists aD’(M)-valued
random variableX on (Q,.1, P)
such thatX(p) = (X, p)
a.s.for each p
ECü(M).
We express the canonical filtration of
stochastically
continuousgeneralized
random fields in terms of
P’(M)-valued
random variables.NOTATIONS 1.28. 7rD :
P’(M) - D’(D)
denotes the canonical restriction map for each open subset.Let
{X (~p) }
andX
be as in(1.27).
Thenconcerning
the canonical filtrationwe have the
following
LEMMA 1.29.
~ = ~ ~~D
oX} for
all open subsets.PROOF. Since the Borel structure for
(D’(D),
weak*)
is standard andP(D)
isseparable,
we obtain an into Borelisomorphism P~(D) 2013~ by collecting
acountable
family
of maps w -(w, ~~.
Therefore it follows thatThis
completes
theproof..
We now prove the
following
theorem withoutassuming
that M is secondcountable.
THEOREM 1.30. Let be a
stochastically
continuousgeneralized
random
field
with the MI-Markov property.If (Y(p))
is ageneralized
randomfield
with the same characteristicfunctional
as then is MI-Markov.
PROOF. We denote the canonical filtration subordinate to
{X(~p)} by
and that subordinate to
{Y(~p)} by
Note that if N is an openand closed subset of M and
I U,, U- I
is an opencovering
of N, thenSuppose
N is second countable in addition.Then,
dueto the existence of conditional
probability
kernels on standard Borel spaces,we deduce from
(1.29)
that Thatis,
if{D+,D_}
is an opencovering
of M, then Since eachcomponent
of M is secondcountable,
we seeby (1.2)
and(1.16)
that is MI-Markov..2. - Linear maps
preserving
the Markovproperty
The main purpose in the
present
work is to discuss thequestion
whenthe inverse map of a local
operator
preserves Markovproperties.
The situationis as follows: Let M and
E2 ---+
M be vector bundles. We use the notationreEl)
for thetotality
of COO-sections ofE1 and Di
for thetotality
of C°°-sections of
El
with compact supports. The same rule isapplied
toE2.
Suppose
ageneralized
random field indexedby ÐI
and a local linear map L :r(E2) ---+ reEl)
aregiven.
Consider anothergeneralized
random field:= indexed
by D2.
Since L islocal,
we may wellexpect
thatsome local structures of is deduced from that of That
is,
weset up the
question
whether inherits the Markovproperty
of(X2(q))
or not.
Kusuoka
[18]
discussed the case when both of thegeneralized
randomfields are realized
by
random variablestaking
values insubspaces El respectively E2
of the Schwartz distributions and there exists abijective
map L’ :Ei -
E2, which is dual to L. He stressed theimportance
oftopologies
onEl
andE2
which make L’homeomorphic
and arecompatible
with the sheaf structure of the Schwartz distributions. From ourpoint
of view his result reads as follows:Let
Ei
be a Hausdorfftopological
vector space with a continuousmonomorphism ti : ~Z
for i =1, 2,
and let L’ :El -~ E2
be ahomeomorphic
linear
isomorphism. Suppose
L islocal,
i.e. ker7ri
o t, c ker7r 2
o 12 o L’ forany open subset D of M.
We say that an open
covering {D+, D_ }
of M is admissible relative to{ G 1 : E1 ~--~ ~l , G2 : E2 ~--~ J~2 ~,
iffand the canonical
projection
is continuous.
THEOREM 2.3. Let
X2 be
anE2-valued
random variableinducing
aRadon
probability
measure.If
thegeneralized
randomfield { ~G2X2,
Sp ED21
is MI-Markov with respect to an admissible open
covering,
then so isREMARKS 2.4.
(i) By using
apartition
ofunity
subordinate to the opencovering {D+, D_ },
one sees that ker 1rD+EÐ ker 7rD = ker 1rD+nD-.Therefore,
if thepartition
ofunity
iscompatible
with ti :El
2013~then
we willget (2.1).
Onthe other
hand,
if thetopology
forE2 is,
forexample, Frechet,
thenby
virtueof the closed
graph
theorem theprojection (2.2)
isautomatically
continuous.(ii)
It isprobable
that thelinearity
isdispensable
for thepreservation
ofthe Markov
property
inspite
of the technicaldifficulty
without it.Let S’ be the space of
tempered
distributions onEd
and t, : S’ ~ ~’ be the naturalinjection.
Then it is not difficult to see that opencoverings {D+, D_ }
of
Ed
with EEdBD+, y
E > 0 are admissible relativeto
it, S’ -, P’,
t : : S’ -~’ } .
This means that if L’ is a differentialoperator
mapping S’
into S’bijectively
and X2 is an S’-valued random variable which induces a 0-Markovgeneralized
randomfield,
thenL’-IX2
induces a 0-Markovgeneralized
random field as well.REMARK 2.5.
Concerning
the conservation of the MII-Markovproperty
we mention thefollowing example.
Let{X2(~p)}
be a mean 0 Gaussiangeneralized
random field with covariance functional
We recall that such a
generalized
random field(X2(p))
is MII-Markov but notMI-Markov
(see
Remark(1.20)).
Because of stochasticcontinuity,
there existsa
unique
S’-valued random variable such that(X2, y~~
=X2(p)
a.s. for ~p E ~.We define another S’-valued random variable
Xl by Xl - (2 - LB)-n X2,
wheren is an
integer
greater than(d
+3)/4.
Then we haveWe can
easily
see that if n >(d
+3)/4,
thenfor some
positive
constant C.By
vertue of this estimate and the Gaussianproperty
ofXi,
we canapply multiparameter
versions ofKolmogorov’s
criterion(see
e.g.[36])
and hence we mayregard
the S’-valued random variableXl
asa continuous random field.
According
to[16],
the random fieldXl
is not MII-Markov,
for itsspectral density
is not thereciprocal
of an entire function ofminimal
exponential type. (Note
that the MI- and MII-Markovproperties
areequivalent
as far as continuous random fields are concerned. See Remark(1.25)).
Thus
(2 - 0)-n, n
>(d
+3)/4,
does notnecessarily
preserve the MII-Markovproperty,
while it preserves the MI-Markovproperty.
Somewhat
unsatisfactory
is that it is not so clear whether we canapply (2.3)
to L = A or not, since A- Imaps S
= d > 3, into atruely larger
space.
Actually
S is not dense in0-1 S ,
which isequipped
with thetopology
transferred
by
0-1 I fromS,
and therefore the natural map t2 : E2 =(LB-1 S)’
--~ Diis no
longer injective.
Thus our effort is devoted toseeking
an answer whichcovers the case L = A or which is flexible for nontrivial kernels of L’.
Our discussion starts from the suitable choice of a
subspace N2
ofr(E2)
which satisfies the
following postulates.
ASSUMPTION 2.6.
(i) N2
containsD2
and isequipped
with a Frechettopology
such thatD2
is dense.(ii)
L mapsM2
intor(Ei ) injectively.
There exists a linear map G :Pi
--+N2
such thatGLq = ?7 for q
ED2
andLG~ = ~ for ~
EPi.
Let
~l
denote theimage
ofN2
under L. Since L :N2
-~r(Ei )
isinjective,
L induces a Frechet
topology
on Then itimmediately
follows that~l1
containsDl (= LG D1)
and the inclusionDl
~~1
1 is also denseAlthough
we do notspecify
thetopology
such that the dual L’ behaves well in the sense of Theorem(2.3),
nevertheless the kernel of L’ cannot be toolarge
orthe
image
of L must belarge.
Thefollowing
is thecorresponding assumption.
ASSUMPTION 2.7. is
stochastically
continuous withrespect
to theH1-topology.
We note that
(2.7) implies
the stochasticcontinuity
of(X2(q))
with respectto the
M2-topology. By
a standardprocedure
we will get aunique family
ofrandom variables cp E such that the
followings
hold:The
family M, I
shall be called the stochastic continuous extention of~Xl(~)}.
The sameprocedure
alsoapplies
to{X2(7?)}.
We use theanalogous
notation for the stochastic continuous extension of
Clearly
it follows thatIn order to describe the canonical filtration
subordinate
to(X2(q)),
interms of the random variables
~f2}
we shall assume thatASSUMPTION 2.10. If supp cp c D for some p e
)12
and some open subset D of M, then there exists a sequence CD2
such that supp ~n c D andin
~2.
Then we
immediately
obtain thefollowing description.
We still need one notion to state our theorem.
DEFINITION 2.12. An open
covering {D+,D-}
of M is{L,
if for
each ~
EPl
withsupp ~
CD+
there exists apartition
ofsubordinate to