A NNALES DE L ’I. H. P., SECTION B
A LEKSANDER W ERON
Second order stochastic processes and the dilation theory in Banach spaces
Annales de l’I. H. P., section B, tome 16, n
o1 (1980), p. 29-38
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Second order stochastic processes and the dilation theory in Banach spaces (*)
Aleksander WERON
Institute of Mathematics,
Wroclaw Technical University, Wybrzeze Wyspianskiego 27, 50-370 Wroclaw, Poland
Ann. Inst. Henri Poincaré,
Vol. XVI, n° 1, 1980, p. 29-38.
Section B : Calcul des Probabilités et Statistique.
SUMMARY. - The
study
of dilations of operator functions in non-Hilbert spaces has beeninspired by
theprobability theory
in Banach spaces. Our aim here is to show that there exists a close connection between the dilationtheory
and thetheory
of second order stochastic processes.1. INTRODUCTION
Simple
dilation theorems assert theembeddability
of a Hilbert space H into alarge
Hilbert spaceHi
so that agiven L(H)-valued
functionf
ona set T can be retrieved
by orthogonal projection
from asimpler L(H1)-
valued function
fl :
However
following [2] ]
we consider R-dilations of B-to-B* operator valuedfunctions,
where B is acomplex
Banach space and B* is its topo-logical
dual.By CL(B, B*)-denote
the space of all continuous anti-linear operators(*) Partially written during the author’s stay at I. N. S. A. Rennes and Southern Illinois
University, Carbondale, Illinois 62901.
Annales de l’Institut Henri Poincaré-Section B-Vol. XVI, 0020-2347/1980/29/$ 5,00/
© Gauthier-Villars.
29
30 A. WERON
from B into B* and
by CL(B, H) the
space of continuous linear operators from B into a Hilbert space H.By
Banach space valued second order stochastic process(B-process)
we mean a
family (Xt)teT
of elementsof CL(B, H),
cf.[1 ] or [19 ].
Its correla- tion function isgiven by
the formulaIt is known
[1 ] that
the spaceCL(B, H)
is aLoynes
space withCL(B, B*)-
valued inner
product [’,’ ].
ThusB-process
is atrajectory
in theLoynes
space
L(B, H).
In the case B is a Hilbert space such processes were detailed considerby
R.Payen [14 ].
When B is thetopological
dual of a Banachspace and H =
L~(Q)
we get thetheory
ofcylindrical
processes. The caseof 2-cylindrical martingales (H
is the space of realsquare-integrable
martin-gales)
was studiedby
M. Metivier[9] ] and by
M. Metivier and J. Pellau- mail[10].
Theimportant example
iscylindrical
Brownian motion which is a « white noise in time and in space ».Let us recall some useful facts on
B-processes.
(1.1)
PROPOSITION( [19 ]).
- Afunction
K : T x T --~CL(B, B*) is
thecorrelation
function of
aB-process iff
it ispositive definite :
for
eachN,
t 1 ... tN E T andb 1
...bN
E B. Moreoverif B-processes Xi
tand
Y~
have the common correlationfunction
then there exists aunitary
operator between the time domains U :Hx - Hy
such thatYt
=The above result may be
interpreted
as thefollowing Aronszajn-Kolmo-
gorov type theorem. For the Hilbert case see
( [ 14 ],
p.350).
Cf. also[8 ], 2.10.
(1. 3)
PROPOSITION. Forpositive definite
kernel K : T x T --~CL(B, B*)
there is a Hilbert space H and an operator valued
function
X : T -~CL(B, H)
such that
If
H is minimal i. e.,then Hand
X( . )
areunique
up tounitary equivalence.
Annales de I’Institut Henri Poincaré-Section B
THE DILATION THEORY IN BANACH SPACES 31
(1. 6)
PROPOSITION( [1 ], [13]). 2014 a) If B-process defined
over a group T isstationary, K(t, s)
=K’(t - s),
then there exists aunitary representation U of
T inHx
such thatXt
=UtXe.
b) If B-process defined
over a unitizedsemigroup
T ismultiplicatively correlated, K(t, s)
=s),
then there exists aself-adjoint
representa-tion
St of
T inHx
such thatX
=StX e.
2. DILATION THEOREMS
Let { and {
be two families of operators such thatKtECL(B, B*), Dt
ECL(H, H)
and R ECL(B, H).
Thefamily {
is called an R-dilation of{
ifKt
=R *DtR
for every index t .See
[Il ] and [20 ].
The first dilation theorem for a B-to-B* valued functionwas
published by
N. N. Vakhania(1968) (*)
when he studied covariance operators forprobability
measures in Banach spaces.Namely,
heproved
the
following
« lemma on factorization » ; for eachpositive
operator A ECL(B, B*)
there exist a Hilbert space H and an operator R ECL(B, H)
such that A = R*R. If H is minimal then the factorization is
unique
up tounitary equivalence.
This result shows that eachpositive
operator A ECL(B, B*)
has a R-dilation to theidentity
operator in a Hilbert space H :In the case of B-to-B* operators the
analogues
of results of Bochner and Naimark onpositive
definite functions andpositive
measures were obtainedby
the methods ofstationary
stochastic processes(detailed
referencesin
[20 ]).
Thetypical
result is thefollowing analogue
of Naimark’s dilation theorem.(2.1)
EXAMPLE. Let F be apositive CL(B, B*)-valued
measure on theJ-algebra
of all borelian subsets of a LCA groupG,
which is the dualgroup of LCA group T. Let K be its Fourier transform
where ( t, g ~
is a value of a character g on t. SinceKo(s, t)
=K(s - t)
is
positive
definite thenby (1.1)
and(1.6)
it is the correlation function (*) The theorem occurs, however, in an unpublished 1957 report by G. B. PEDRICK, cf. ([7], p. 415-416).Vol. XVI, n° 1-1980. 2
32 A. WERON
of a
stationary B-process Xt.
Thus there exists a Hilbert space H =Hx
and a
unitary representation U~
such thatwhere
E( . )
is aspectral
measure ofUg
obtained from the Stone’s theorem.By
theuniqueness
of the Fourier transform we haveSince
Hx-the
time domain of the processXt
is minimal in the senseof
(1.5)
thusby Prop.
1. 3. H =Hx,
R =Xe
andE( ~ )
areunique
up tounitary equivalence.
So thetriple (H, R, E( ~ ))
is a minimal andunique
R-dilation of
F( . ).
Thus we haveproved
ananalogue
of Naimark’s dilation theorem.The reason for which this result was
proved by
a method of stochasticstationary
processes followsimmediately
if weinterpretate
theProp.
1.1and
Prop.
1.6 in thelanguage
of dilationtheory. Namely,
the correlation functionK(t)
of astationary
B-valued processXt
has a minimal andunique
R-dilation
(Hx, Xe, Ut).
(2.2)
REMARK. - The existence of the above closerelationship
betweenthe dilation
theory
andstationary
B-valued processes isimplicit
in papers of S. A.Cobanjan (1970),
A. I. Ponomarenko(1972)
and the writer(1975).
(See
detailed references in[20 ].)
Thesystematic
studies of these ideas inmore
general setting
ofsemigroups,
thetheory
of so called propagators(stationary
process has theunitary propagator)
and its connection with Kernel theorem(Prop. 1.3)
has been doneby
P.Masani,
cf.[8 ].
Howeverhe has used the definition of dilation in which R is a linear
isometry
on aHilbert space B into H and
consequently
consider dilationsonly
for Hilbertcase. It is extended
by
ourapproach
which may be alsoapplied
tolocally
convex spaces. Since the
complete analogue
ofProp.
1.3 does not holdin all
locally
convex spaces, therefore one may deduce dilation theoremsonly
for those spaces which are characterizedby
Kerneltheorems,
see[3 ].
In
[2] we proved
a B-to-B*analogue
ofgeneral
B.Sz-Nagy’s
dilationtheorem
by using
thecomplicated
construction which is like theoriginal
one for the Hilbert case. Now we
give
a shortproof
of the stronger result which is in aspirit
of the aboveexample.
For non-unital case see[12].
Let S be a
*-semigroup
i. e., S is a unitalsemigroup
with a function* : S -~ S such that for each s, t E S
Annales de I’Institut Henri Poincaré- Section B
THE DILATION THEORY IN BANACH SPACES 33
A function K : S -~
CL(B, B*)
ispositive-definite
if a functionK1(s, t)
=K(t*s)
defined on S x S satisfies(1.2).
Anoperator
valued functionD(. ) :
S -~CL(H)
is called a*-representation
ifIf
K( . )
is the formwhere R E
CL(B, H)
thenD( ~ )
is an R-dilation ofK( ).
(2 . 3)
THEOREM.- a)
Let aCL(B, B*)
valued kernelK( ~ )
on a unitized*-semigroup
S bepositive definite.
Then thefollowing
areequivalent : ( 1 )
There exists afunction
oe : S --~ such thatfor
each s, t E Sand bEB(2) K( ~ )
has an R-dilationD( ~ )
which is aninvolutory representation of
S.(3)
There exists afunction
6 : S --~ and a number c > 0 thatfor
each s, t E S
where Q is
submultiplicative ; 6(st)
_b)
Theminimality
condition H = determines HandD( ~ )
up to
unitary equivalence.
tEsc)
The minimal space H isseparable i, f’f K(t)B
is aseparable
sub-space
of
B*. rEsProof
Since K ispositive definite,
thereforeby Prop. 1.3,
there isa Hilbert space H and an
operator-valued
function X : S -~CL(B, H)
such that
Now
by [7,
th.4.13] ] (1)
isequivalent
to the fact that there is a semi-group { D(s), s
ES }
onCL(H, H)
such that for each s, t E SHence
We have thus shown that
(1) implies (2). Next,
we show that(2) implies (3).
Indeed,
Vol. XVI, n° 1-1980.
34 A. WERON
Hence with c
= ( ~ R ~ ~ 2
and6(s) _ ( ~ (
we have(3)
sinceFinally
from( [18 ],
cf. also[17] and [8 ])
we know that(3)
isequivalent
to
(1).
Thiscomplete
theproof
of theequivalences.
As for the
minimality
conditionb),
suppose that for i =1,
2,Di
areinvolutory representations
ofS,
where
Ri
ECL(B, H;)
and =K(s).
LetXls)
=Di(s)Ri.
ThenHence,
cf.(1.1),
there is aunitary
operator U onH 1
ontoH2
such thatX2(s)
=UX1(s),
for each s E S. ThusThis shows that
D2(s)U
=UD 1 (s)
onRi(B),
and hence on itsclosure,
i. e., on
Hi.
Thiscompletes
theproof
of partb).
The part
c)
follows from thefact,
that3. APPLICATIONS TO STOCHASTIC PROCESSES
In this section we want to deduce some theorems for
B-processes by using
dilationapproach.
The first result followsimmediately
from Th. 2 . 3a).
(3 .1)
COROLLARY. -If B-process defined
over a*-semigroup
T is*-stationary; K(t, s)
=K’(s*t),
then there exists aninvoluntary
represen- tationDt of
T inHx
such thatX
=DtX e iff
thecorrelation function K’( . ) satisfies
the condition(1)
or(3) from
Th. 2.3.Next we would like to show that the
uniqueness
of minimaldilations,
Th. 2.3
b), suggested
a new way forobtaining isomorphism
theorems forstationary B-processes.
We start from thefollowing example
which illus-trates the idea in the case B = C.
Annales de l’lnstitut Henri Poincaré-Section B
35
THE DILATION THEORY IN BANACH SPACES
(3.2)
EXAMPLE. - The correlation functionK(.)
of a continuousstationary complex
valued processXr
over an LCA group T is acomplex
valued
positive
definite function on T. Since each group is a*-semigroup (t* = - t)
and in this case each functiontrivially
satisfies the condition(1)
from Th.
2 . 3,
thusK(’)
has the minimalunitary
dilation(Hx, Xe, U~).
On the other hand
K(’)
is continuous andby
the Bochner theorem there exists anonnegative
scalar measure F on the Borel6-algebra
of thedual group G such that K is its
Fourier-Stieltjes
transform. Consider the spaceL2(F)
of squareintegrable complex
functions on G and theunitary
group
Vt given by
the formulaIt is easy to observe that the
triplet (L2(F), M, Vt),
where M : C -L2(F) -multiplication by f (g)
--_1,
is another minimal dilation ofK( . ).
By
theuniqueness
property in Th. 2.3 there exists aunitary
operator W :L2(F) -~ Hx
such that WM =Xe
andWVt
=UtW.
Let’s note that Wis realized as a stochastic
integral
Thus we have obtained a new
proof
of the celebratedisomorphism
theoremfor
stationary
processes, see[15 ].
The above construction may not be
directly
extended to the Banachspaces because a space
L2(F)
forCL(B, B*)-valued
measure F is not definedas far. For a case B is a Hilbert space see
[6].
But anotherinteresting approach
ispossible.
Let F beCL(B, B*)
valuedpositive
measure suchthat there exists a
nonnegative
(7-finite measure J.1 that foreach x,
y E B(F( . )x)( y)
isabsolutely
continuous w. r. t. ,u. Thenby [5 ]
there exists aHilbert space K and an operator
Q
ECL(B, L2(,u : K))
such thatThus
F(’)
has thefollowing
dilation inL 2(11; K):
where
Eo(’)
is thespectral
measure inL2(~u : K)
defined as an operator ofmultiplication by
the indicator This dilation is minimalby
the defini-tion in the
subspace
Vol. XVI, n° 1-1980.
36 A. WERON
On the other hand the measure F defined
by
thestationary B-process
has
by (? .1 )
the minimalspectral
dilation(Hx, Xe, E( . )).
Thusby
theuniqueness
property there exists aunitary
operator W : L such thatWXe
=Q
andWE(-)
=Eo( . )W. Consequently
we obtainThus we have
proved
thefollowing
(3 . 3)
THEOREM(cf. (4 ]).
LetXt be a
continuousstationary B-process
over an LCA group such that F related to
Xt
as in{2.1)
has a weakspectral density.
Then the time domainHx
and thespectral
domainL(F) of
the processare
unitary equivalent.
Finally
we shall present someapplication
of dilationapproach
to2-integrable martingales
which were studied in[9] and [10].
Let T =
[o,.1_ ], (Q, ~, P)-basic probability
space and ~~ be the space of all squareintegrable
realmartingales Xt
which areright
continuous and with left hand limits andXo
= 0. Ifmartingales Xt
andYt
such thatP
[sup Xt - Yt| ] ] =
0 areindistinguishable
inU,
then U is a Hilbert space with natural L2 innerproduct.
Following [9, 10] ]
we say that X is2-cylindrical martingale
on B* ifX E
CL(B*,
Animportant
role in thetheory
of such processesplays
such called
quadratic
Doleans’ measure M of X which is defined on the7-algebra ~
ofpredictable
subsets of T x Q.Let m be defined
by
the formulawhere A = F x
] s, t] ]
ispredictable rectangle
and h Q gbelongs
to thetensor
product B*
Q B*. The extension of[m(A) ] (h
Qg)
defines a mapp-ing
M from * into the dual space(B* Q 1 B*)*.
Thismapping
M is calledquadratic
Doleans’ measure(see [10 ]).
(3 .4)
THEOREM. Let M be thequadratic
Doleans’ measureof
a2-cylin-
drical
martingale. If
is aseparable subspace of
B** thenAE~
there exists a
nonnegative
real valued measure ,u on P such thatfor
eachx, y E B*
[M( . ) J(x
Qy)
isabsolutely
continuous w. r. t. ,u.Proof
Note that x Q y can be identified with a bilinear continuousAnnales de I’Institut Henri Poincaré-Section B
THE DILATION THEORY IN BANACH SPACES 37
form on B* x B* or a continuous linear form on B* @ B*
through
theformula
Thus there exists a continuous extension of this linear
mapping
intoan
isometry
from(B* 0i 1 B*)*
ontoCL(B*, B**)
which to a boundedbilinear
form f
on B* x B*correspond
the bounded lineaioperator
F e
CL(B*, B**)
such thatSince
by
the definitionquadratic
Doleans’ measure ispositive
valuedthen we may use the dilation
theorem,
cf.[20 ]. Consequently
there existsa Hilbert space
H,
an operator R ECL(B*, H)
and aspectral
measureE( . )
on
(y-algebra
ofpredictable
sets such thatMoreover
by
the partc)
ofTh.2.3,
H isseparable
becauseB~ M(A)B*
is
separable.
Note that H ={E(A)RB* }.
~- Aei?
Let
where
(e,,)
is a CONS in H. Thus ~~ isnonnegative
real valued measure on(T
x Q,~)
and for eachE(. )en ~ ~ 2 « y.
Hence for eachh, gE
H(E(. )lT, g) «
~ltoo. Therefore for h =
E( . )Rx and g
=E( . )Ry, where x, y
E B* we obtaincompleting
theproof.
ACKNOWLEDGMENT
The author is
grateful
to the referee for hissuggestions.
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(Manuscrit reçu le 19 octobre 1979) The first version was send in July 1978
Annales de l’Institut Henri Poincaré-Section B