A NNALES DE L ’I. H. P., SECTION A
J.-P. A NTOINE F. B AGARELLO C. T RAPANI
Extension of representations in quasi
∗-algebras
Annales de l’I. H. P., section A, tome 69, n
o2 (1998), p. 241-264
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241
Extension of representations in quasi *-algebras
J.-P. ANTOINE
F. BAGARELLO
C. TRAPANI
Institut de Physique Theorique, Universite Catholique de Louvain
B-1348 Louvain-la-Neuve, Belgium Antoine @fyma.ucl.ac.be
Dipartimento di Matematica dell’ Universita di Palermo 1-90123 Palermo, Italy
Istituto di Fisica dell’ Università di Palermo 1-90123 Palermo, Italy
Trapani @unipa.it
Vol. 69, n° 2, 1998, Physique théorique
ABSTRACT. - Let
(2t,
be atopological quasi *-algebra,
which meansin
particular
thatSto
is atopological *-algebra,
dense in 2L Let x° be a*-representation
ofNo
in somepre-Hilbert
space D c H. Then wepresent
several ways ofextending ~r°, by closure,
to somelarger quasi *-algebra
contained in
2t,
eitherby
Hilbert spaceoperators,
orby sesquilinear
forms on D.
Explicit examples
arediscussed,
both abelian andnonabelian, including
the CCRalgebra.
©Elsevier,
ParisKey words: topological quasi *-algebras, closable *-representations, closable positive sesquilinear forms, CCR algebra.
RESUME. - Soit
(, o)
unequasi *-algèbre topologique,
cequi implique
en
particulier
que est une*-algèbre topologique,
dense dans St. Soit 7r" une*-representation
de dans un espaceprehilbertien
D c H.PACS : 02.10+w, 03.65.Fd, 11.30. j
Annales de l’lnstitut Henri Poincaré - Physique théorique - 0246-0211 1
Vol. 69/98/02/@ Elsevier, Paris
242 J.-P. ANTOINE, F. BAGARELLO AND C. TRAPANI
Dans ce contexte, nous
presentons plusieurs
manieres d’etendre parfermeture,
a unequasi *-algèbre plus grande
contenue dans2t,
soit par desoperateurs
dans un espace deHilbert,
soit par des formessesquilineaires
sur D. Plusieurs
exemples explicites
sontdiscutes,
tant abeliens que nonabeliens,
ycompris 1’ algebre
des relations de commutationcanoniques (CCR).
@Elsevier,
ParisMots clés : .’ topological quasi *-algebras, closable *-representations, closable positive sesquilinear forms, CCR algebra.
1. INTRODUCTION
One of the most familiar
techniques
in thedescription
of aquantum system
is toput
first thesystem
in a box A of finite volume V and then let V go toinfinity, possibly
with suitableboundary
conditions(for instance, periodic
b.c.).
Inquantum
fieldtheory,
this wouldcorrespond
to cut-offremovals
[ 1 ],
while in statisticalmechanics,
the relevantoperation
is thethermodynamical
limit[2].
A similar
approach
is common also in thealgebraic
version ofquantum
theory.
One considers first aC*-algebra 21A
of observables localized in A and then let A 2014~ oo. This works in most cases and leads to theconcept
ofquasi-local
observablealgebra. However,
there aresystems
for which thetechnique fails,
in the sense that thedynamics
does not converge ina C*-sense.
Typical
aresystems
withlong
rangecorrelations,
for instance theBCS-Bogoliubov
model of asuperconductor [3]-[5],
thedescription
ofthe CCR
algebra [4], [6]
and various latticespin systems,
called almostmean field models
[7], [8].
In these cases,however,
a solution may be foundby taking
for thealgebra
of the fullsystem
anO*-algebra,
thatis,
a*-algebra
of unboundedoperators
on a fixed invariant domain[9],
or evena
partial O*-algebra [ 10], [ 11 ] .
Thesimplest
case for the latter is that of aquasi *-algebra [4], [12],
and indeed several of thephysical systems
listed above lead to such a structure.First let us recall the basic definitions. Let 2t be a vector space and
2to
a*-algebra
contained in 2t. We say that 9t is aquasi *-algebra
withdistinguished *-algebra Q{o (or, simply,
over if(i)
theright
and leftmultiplications
of an element of 2tby
an element of2to
arealways
definedand
linear;
and(ii)
an involution *(which
extends the involution of isAnnales de l’lnstitut Henri Poincaré - Physique théorique
defined in 21 with the
property (AB~’~
=B * A*
whenever themultiplication
is defined. A
quasi *-algebra
is said to have a unit I if there existsan element I E
210
such that AI = I A =A,
VA E 2t. Unless statedotherwise,
all thequasi *-algebras
used in this paper are assumed to havea unit.
Finally,
thequasi *-algebra
is said to betopological
if2t carries a
locally
convextopology
T such that(a)
the involution is continuous and themultiplications
areseparately continuous;
and(b) 210
is dense in
Assume now that the set of observables of a
given physical system
is aquasi *-algebra
Then aproblem
arises. In the standardalgebraic formalism,
the concretedescription
of thesystem
is obtainedby selecting
a state 03C9 on the observablealgebra
2t andbuilding
thecorresponding representation by
the familiar GNS construction. Even if 2t isonly
aquasi *-algebra,
the GNS construction isavailable,
as forany
partial *-algebra [ 11 ], [12],
but the notion of state becomes moreinvolved and it is not
always
obvious to find concrete states. An alternativeapproach, possibly easier,
would be toproceed
in twosteps. ( 1 )
Start fromthe
subalgebra
select a state 03C9 over210
and build thecorresponding
GNS
representation (2)
Then extend7r~
to the fullquasi *-algebra
or at least to a
sufficiently large quasi *-algebra
C 21. The aim of this paper is toexplore
this extension process, and moregenerally,
the extension of agiven representation
7r° of within thequasi *-algebra
2t. Such anextension
naturally proceeds by taking limits,
but therepresentations 7r~
orx° are in
general
not continuous in thetopology
of2to. Instead,
wesuggest
to
perform
an extensionby closure,
whichrequires
that we introduce somenotion of
closability
of therepresentation.
We
emphasize
that thisprocedure
hasnothing
to do with the familiar notion of closure of a*-representation
7r, which is the extension 7f of 03C0 to thegraph topology completion
of the domain(in
whatfollows,
wemay as well assume that 7r° is a closed
*-representation
of~.°).
The samecomment
applies
to the extensiontheory developed
in[13],
which is of asimilar nature. In both cases, the extended set of operators is defined on a
larger domain,
but remains in one-to-onecorrespondence
with theoriginal
set. Here we want to obtain additional
operators.
Let us be more
precise.
Let 2t be atopological quasi *-algebra
over2~
and 7!-" be a
*-representation
of2~,
thatis,
a map from210
into the*-algebra
,C~ (1)),
where D is a densesubspace
in some Hilbert space?-~,
and,Ct ( D )
is the set of all
operators
A in H such that both A and itsadjoint A’~
map D into itself. Ingeneral, extending
7r°beyond 210
will force us to abandon the invariance of the domain D. Thatis,
for A E the extendedVol. 69, n° 2-1998.
244 J.-P. ANTOINE, F. BAGARELLO AND C. TRAPANI
representative
willbelong only
to,C~ (D, H),
which is defined asthe set
(actually
apartial O*-algebra)
of alloperators
X in H such thatD (X )
= D and D. Then one mayimpose
on 7r° to be closable in/~(P~),
andstudy
thecorresponding
extension of 7r"by
closure. Thiswill be done in Section 2. In
addition,
if 7r" is the GNSrepresentation 7r~
associated to some state 03C9 on there is another
possibility
ofextension, using sesquilinear
formtechniques.
We willstudy
this case too in Section2,
and in
particular
compare the results of the two methods.One can also go one
step
further.Putting
on D a suitable(graph) topology,
one builds therigged
Hilbert space D c H cD’,
where D’ isthe dual of D
[14],
and observes thatwhere
,C(D, D’)
denotes the space of all continuous linear maps from D intoD’.
Then one may alsorequire
that 7r" be closable in~(P, D’ )
andtry
to extend 7!-" within
,C(D, D’).
This forms thesubject
matter of Section 3.First we observe
that, given
a*-algebra 3~
and a*-representation
~r° :
2~ ~
for someprehilbert
space D cH,
it ispossible
tobuild a
topological quasi *-algebra (,
contained in,C (D, D’ )
anda
*-representation
7r of that extends 03C0o. Then we come back to thegeneral problem
ofextending
a*-representation
7r" of2to
within agiven quasi 2~o).
Since the elements of~C(I~ D’ )
may beinterpreted
as
sesquilinear
forms onD,
we will say that therepresentation
7r isan extension
by sesquilinear forms. Actually
thisproblem
wasalready
addressed in an earlier paper
[15],
but in a restricted way, in the sense thatonly
extensions to the wholequasi *-algebra
were considered.In both cases, extensions
by operators
and extensionsby sesquilinear forms,
concreteexamples
will bediscussed,
abelian ones(quasi *-algebras
of
functions)
as well as nonabelian ones(quasi *-algebras
ofoperators
ormatrices).
Of course, this paperrepresents only
a firststep
in thestudy
ofextension of
representations.
Our aim here isonly
toidentify
theproblem properly
and tosuggest
somepossible
solutions. Further work is in progress.2. EXTENSIONS BY HILBERT SPACE OPERATORS 2.1. Closable
*-representations
in,Ct (D, H)
Let
(2t[r~ 2to)
be atopological quasi *-algebra
and 7ro a*-representation
of
210
on the domainD(~°)
:= D. This means that E/~(D),
VA EAnnales de l’Institut Henri Poincaré - Physique théorique
Since
Gt(D)
c it make sense to ask thequestion
as towhether admits an extension to a
subspace
of 2ltaking
values inGt (D; H).
As
usual,
we consider£f (D, H)
as endowed with thestrong*-topology
ts*
definedby
thefamily
of seminormsWe remind that is
ts~ -complete.
For X E we set
7r(X)
=Clearly,
7r is well-defined and extendsSince the
involution f
ists* -continuous,
Ximplies
thatX*
E Therefore2tT(7r)
is a *-invariant vectorsubspace
of2t,
but it need not be a
quasi *-algebra
overIndeed,
even if X E2lt (7r)
and B E
2to.
this does notimply
that X B E However:PROPOSITION 2.2. - Let be a
ts*
-closable*-representation of
in D.Assume moreover that 7r 0 is a bounded
*-representation.
Then( 7r)
is aquasi *-algebra
over~Lo.
Proof -
Let X E and B E We will show that X B eSince X E there exists a net C such that
Xa -~ X
andis
ts* -convergent
in,Ct (D, H).
ThereforeXaB #
X B andTherefore is
ts* -convergent
and so X B E 0Vol. 69,n° 2-1998.
246 J.-P. ANTOINE, F. BAGARELLO AND C. TRAPANI
2.2. Extension of
GNS-representations
Let
(2t[r],
be atopological quasi *-algebra
and w a state on Asis well known
[16], ~
defines a(closed) *-representation
of on adomain
D(~w~.
We will nowtry
to extend7r~
to elements of There are two ways ofdoing that,
which we will discuss below.The usual
GNS-representation 7r~
isbuilt-up
in thefollowing
way. Onebegins by considering
the setwhich turns out to be a left ideal of Then the
quotient
space~ 1= (whose
elements will be denoted asA~(X),
X Eis a
pre-Hilbert
space with scalarproduct
The
representation 7r~
is then definedby
One
readily
checks that03C0o03C9(A*) = 03C0o03C9(A)~,
V A Eo
and so03C0o03C9(A)
E~t(~). Furthermore, A~(7)
is acyclic
vector for7r~. Finally
thisrepresentation
can be continued to a closedrepresentation
in a standardfashion,
but we are not interested here to thisprocedure.
If is
ts -closable,
then we canproceed
as before and we obtain anextension of
7r~
to asubspace
of 2LHowever,
there is anotherpossible
way ofextending
outside ofnamely by closing
thepositive sesquilinear
formHo
definedby
~.The
equation
defines indeed a
positive sesquilinear
form on210
x We now assumethat
00
is closable in 2t in the sense we shall define in a while. Let be a net in210
and X E 2L We say thatXa
is03A9o-convergent
to X ifDEFINITION 2.3. - We say that
flo
is closableif 03A9o(X03B1,X03B1)
converges to0
for
any net that is03A9o-convergent
to 0.If
S2o
isclosable,
we defineAnnales de l’lnstitut Henri Poincaré - Physique théorique
Remark. - The above definitions are
slight
modifications of the usual definition of closablesesquilinear
form on a Hilbert space[17].
Let
r~ := Do
x It iseasily
seen that [1 andr~ satisfy
thefollowing
conditions:
Let us now define the set
It is clear that is a
quasi *-algebra
over2~.
The form H may beregarded
as an
everywhere defined o-weight
in the sense of[ 18],
Definition 3.1 with the obvious choicer 0 ==
x In fact thefollowing
conditions hold:Indeed, (i)
and(ii)
are more or lessobvious; (iii)
follows from asimple limiting
argument and(iv)
is due to the fact that H is apositive sesquilinear
form on
2(0
x and thus satisfies theCauchy-Schwarz inequality
Conditions
(i)-(iii)
are characteristicof ips (invariant positive sesquilinear)
forms on
partial *-algebras [ 10], [11]. (The complete
definition ofips
formon a
partial *-algebra actually
includes an additionalcondition,
but inVol. 69, n ° 2-1998.
248 J.-P. ANTOINE, F. BAGARELLO AND C. TRAPANI
this case it follows
immediately
from(iii).) Nevertheless,
thetheory
of *-representations developed
there can beapplied only
if an additionaldensity
condition is fulfilled. This is
actually
the case, as we shall see in a while.One
begins
withconsidering
the setand then takes the
quotient
:== whose elements are denoted as E Let be thecompletion
ofLet B E
Q(o}.
Then is dense inIndeed,
Do. Therefore, by
the constructionitself,
ifÀo (A)
E thereexists a net C which converges to with
respect
to the norm of Then 0 is an
ips
form on03A9 (see
the Remarkabove)
and thus a GNS construction can be
performed
as in[10] ;
theoperators
obtained in this way live in the Hilbert space More
precisely,
onedefines,
for A EThen is a well-defined linear
operator
from into From(iii)
it followsthat,
for each A E E Inparticular,
if A E then maps into itself.The next
step,
of course, is to compare the results obtained in the two waysexplained
above. The first naturalquestion
is whether theclosability
of
00 implies,
or isimplied by,
theclosability
of7r~.
The secondquestion
is,
what kind of relationexists,
if any, between~ ( 7r w)
and2to.
We
begin by
asubsidiary
result that will be needed later.First,
we defineFurthermore,
for2lo,
we setThe forms
SZo
andSZ$,
B E are stillpositive sesquilinear
forms ono
x Then one has:LEMMA 2.4. - Let
00
apositive sesquilinear form
on210
x Thefollowing
statements areequivalent
(i) 00
isclosable;
(ii) S~o
isclosable;
(iii) SZ$
isclosable, for
each B E2l0.
Annales de l’Institut Henri Poincaré - Physique théorique
Proof. - (i)
#(ii):
LetS2o
be closable and let be a net ino
thatis
0: -convergent
to 0. ThenXa ~
0 andX;, X: - X~ )
- 0.Since also
Xa ~ 0,
weget
thatX;
isHo-convergent
to0;
thus 0.(ii)
#(i):
this follows from theprevious implication by taking
intoaccount that =
00.
(i)
#(iii):
Letagain Xa
be a net that is03A9oB-convergent
to 0. ThenXa ~
0 andOo((Xa - X~)B, (Xa - X~)B~ -~
0. Since alsoXaB ~ 0,
we conclude that
{X03B1B}
is03A9o-convergent
to 0.Therefore, by
theclosability
of
00,
0. Hence03A9oB
isclosable,
for each B E2L.
(iii)
~(i):
follows from the fact thato
contains the unit. 0PROPOSITION 2.5. - Let
SZa
be closable. Then03C0o03C9
ists*-closable
in,C~ ~Dw ,
and one has CProof -
Let be a net in such thatXa #0
and~
Y E£t(D, ~-C~
with D = and H =Recalling
thatelements of are
simply
cosets~W (~~,
B E weget,
inparticular
and
But
by
Lemma2.4,
it follows that0,
VB EThen
7r~
ists*-closable
inLet now X E
~ ( 1f ’" ); then, by definition,
there exists a net co
such that
Xa X
and~
Thisimplies
that bothand tend to 0 for any
B E
2to.
But117r~(Xa - Xø)Àw(B)112
=~)B, (Xa -
and
~~~w~X~ -
=~X~ - X~ )B).
Theseequalities imply easily
that X E2tn.
DThe converse statements may be proven under the much
stronger assumption that,
if C2to
is a netno-convergent
to0,
then bothX~, Xa - X~)
andX;, X: - X~ )
converge to0,
for all B E
2to.
Then one = but this result does not seem very useful inpractice.
Vol. 69, n° 2-1998.
250 J.-P. ANTOINE, F. BAGARELLO AND C. TRAPANI
EXAMPLES 2.6. -
( 1 )
Let X =[0,1],
2t -LP(X),
p > 1 and =C(X),
the
C*-algebra
of continuous functions on X. Let w be the linear functionalon
C(X)
definedby
The
sesquilinear
formHo
associated with w is then defined asIf
p > 2,
thenHo
isbounded,
as it iseasily
seen, and so it can be extended to the whole spaceLP (X ) .
If 1
p 2,
the situation is different. In this case, infact, Ho
isonly
a closablesesquilinear
form.Indeed,
assume - 0 and thatfm, fn -
isconvergent
to 0.Then,
there existsan element
f
EL~(X)
such - 0. Thisimplies that /~
converges to
f
in measure. The convergence offn
to 0 inLP(X)
in turnimplies
the convergence ofIn
to 0 in measure. And sof
= 0 a.e. in X.Therefore = - 0. Hence
H~
is closable. It is easy to check thatL2 (X)
c Toget
theopposite inclusion,
let us considerf
EDo.
Then there exists asequence {fn}
such - 0 andH(/,/) ~
The convergence ofIn
tof implies
theexistence of a
subsequence converging
tof
a.e. in X. Thenalso p
converges
to f ( 2
a.e. in X andw ~
existsby assumption.
By
Fatou’slemma,
it follows thatf
EL2 (X )
and therefore =L2 (X ).
In this case, we also have =
L~(X).
From theprevious
discussion and from
Proposition 2.5,
we know that~ (7rw)
C03A9
=L2 (X) .
Let
now f
EL~(X);
so there exists asequence {/~}
CC(X)
thatconverges
to f
inL~(X).
Then we haveIn an
analogous
way, we can prove - 0. Thereforethe sequence
7rw(fn)
ists*-Cauchy.
(2)
Let X =[0,1], Qlo
=C(X)
and Ql =LP(X),
p >1,
as inExample
1.Let,
moreover, w E r >1,
and w > 0. Let w be the linear functional onC(X)
definedby
Annales de l’lnstitut Henri Poincaré - Physique théorique
The
sesquilinear
formHo
associated with cv is then defined asLet us discuss the
closability
ofHo
when p varies in[1,
The wholediscussion can be reduced to the cases examined in
Example 1,
if we takeinto account the
following
facts:The conclusion is that
S~o
is bounded if s >2, while,
for1 s 2, no
is not
bounded,
but it is closable.(3)
We end this section with a nonabelianexample.
Let Ql be the vectorspace of all infinite matrices A :=
(amn) satisfying
the condition2t is a Banach space with
respect
to this norm. With theordinary
matrixmultiplication
and the usual involution A -A’~,
2t may also beregarded
as a
topological quasi *-algebra
over the*-algebra
of all matrices witha finite number of non-zero entries in each row and in each column
(this
isa
quasi *-algebra
withoutunit,
since I ELet
The
sesquilinear
formHo
associated to cv is then definedby
with B :=
(bmn).
Let us show that00
is closable. Let~A~~,
withAk = (akmn),
be a sequence ino
suchthat ~Ak~
- 0 andAj , Ak - Aj )
converges to 0. We will prove that
Ak )
- 0. In terms ofmatrices,
the two conditions above read
Vol. 69, n° 2-1998.
252 J.-P. ANTOINE, F. BAGARELLO AND C. TRAPANI
and
Let B denote the vector space of all infinite matrices A : =
satisfying
the condition
!8 also is a Banach space with
respect
to this norm. Then(2.5)
meansthat ~ Ak ~
is aCauchy
sequence withrespect to 11.112
and it converges toa matrix A E ~3. Thus
necessarily
Now set M ==
~°°,n-1
Then(2.6)
can be cast in thefollowing
formThis
implies that,
for all m, n EIN,
But from
(2.4)
weget
alsothat,
for all m, n EIN,
-0,
for k - oo .Hence a = 0.
The next
point
is toidentify
We claimthat,
in this case,03A9 = B.
Theinclusion B
cDo
is easy. Let now A= (amn)
ED03A9;
then there exists a
sequence {Ak},
withAk = (akmn)
such -0,
for k - oo andAk) convergent.
--~0,
it followseasily
thatamn
converges to amn for each m, n.Moreover, Ak)
converges to
A) by
definition.Finally,
weget
Therefore The
equality D03A9 = 03A9 is,
in this case, obvious.Annales de l’lnstitut Henri Poincaré - Physique théorique
3. EXTENSIONS BY
SESQUILINEAR
FORMSIn Section
2,
we have studied the extension ofrepresentations by
Hilbertspace
operators, 7r(~4)
E7~).
Now we turn to extensions in the space ofsesquilinear
forms,C ~ D, D’ ) .
3.1.
Quasi *-algebras generated by *-representations
First we consider a
*-algebra
on its own and show that a *-representation
7r 0 of210
can be used to build up aquasi *-algebra
relatedto 7r 0 .
Let 03C0o be a
*-representation
of the*-algebra 210
defined on a certaindomain :=
D,
densesubspace
of agiven
Hilbert space H. Thismeans that the linear map which maps into
/~(D),
is such that7ro (A* ) =
and7r~(A)7r~(B)
for all A and B inLet
us now
endow D with thegraph topology t~ generated by
thefollowing family
of seminorms:Then we construct the
rigged
Hilbert space(RHS) [14]:
where is the
conjugate
dual of endowed with thestrong
dualtopology.
As usual we will denote with
G(D, D’)
the vector space of all the linear maps which are continuous from into With thisconstruction,
we know that(G(D, D’), ,Ct(D))
is aquasi *-algebra [12].
Many topologies
may be introduced inG(D; D’).
For instance:(i) Uniform topology
It is definedby
the seminormswhere A4 is a bounded subset of D.
(ii) Strong topology
Ts : definedby
thefollowing
seminormswith J4 as above.
Vol. 69,n° 2-1998.
254 J.-P. ANTOINE, F. BAGARELLO AND C. TRAPANI
(iii) Strong * topology
Ts~ : In this case the seminorms are(iv)
Weaktopology
Tw : The seminorms arewhere rp
and 1jJ belong
to D.The involution
A - A*
is continuous forTV,
T~ and Tw, but of coursenot for Ts. The
multiplication
from theright by
elements from is continuous forTD
and Tw, and that from the left is continuous forTD,
Tsand
Whenever 7r 0 is a faithful
representation
of the*-algebra
we canintroduce on a
topology
which is linked to the one introduced in therepresentation
space. Let us assume, forinstance,
that~(D, D’ )
is endowedwith the uniform
topology TV. Then,
if A4 is a bounded set in we define a seminorm onby
Since 7r 0 is
faithful,
this is aseparating family
of seminorms.Calling TD
thistopology,
we caneasily
conclude thatQ{o (Tj’)
is alocally
convex*-algebra.
Remark. - An
analogous
result holds if wereplace
the uniformtopology by
the weak one.However, Q{o
fails to be alocally
convex*-algebra
forthe
corresponding strong
and thestrong* topologies.
Let now Ql be the
completion
ofQ{o
withrespect
toTf.
It is clear that( ~t. ~TD~ ,
is atopological quasi *-algebra. By
the constructionitself,
the
representation
is continuous from into,C(D, D’) ~TD~.
As aconsequence we have the
following
PROPOSITION 3.1. - Let 03C0o be a
*-representation of
in D. Then thefollowing
statements hold true:(i) If
03C0o isfaithful,
then there exist alocally
convextopology TD
on210
such that 7ro is continuous
from
into,C(D,
(ii) If ,C(D, D’)
iscomplete,
then 03C0o has an extension 7r to thequasi
*-algebra 2(0),
where ~ denotes theTf-completion
The map~r has
the following properties:
Annales de l’Institut Henri Poincaré - Physique théorique
We will discuss some
examples
of this situation below. Beforethat,
it isworth
remarking
that theprocedure
outlined in this section for one faithfulrepresentation
can beeasily
extended to a faithfulfamily {7~,
a EI~
of
*-representations
of Herefaithful
meansthat,
for each non-zeroA E there exists a E I such that
7r~ (A) ~
0. Of course, each7r~
is a*-representation
on a domainDa,
thatis,
E,Ct (D~ ) .
Then we candefine a
locally
convextopology
ono
as the weakestlocally
convextopology
such that each7r~
is continuous from210
intowhere Top stands for any of the
topologies TV,
Ts, T w, andproceed
asbefore to
get
an obvious extension ofProposition
3.1.EXAMPLES 3.2. -
( 1 )
Let X :=[0, 1]
and P theself-adjoint operator
defined onby
Define the domain
Then D coincides with
D°°(P},
and thetopology
coincides with thetopology given by
thefollowing family
ofseminorms:
It is easy to check that D is a
*-algebra
and that themultiplication
isjointly
continuous
[12] :
forany k
EIN,
there exists apositive
constant ck such thatWe can now define a
*-representation
of D on D itselfby
This
representation
is faithful since the functionu(x)
=[0,1], belongs
to D.Vol. 69, n° 2-1998.
256 J.-P. ANTOINE, F. BAGARELLO AND C. TRAPANI
Let D’ be the
conjugate
dual of D withrespect Using (3.1 ),
wesee that if 03A6 is an element of D’ and
f
is any vector ofD, then 03A6f
ED’,
where the
product
is defined in thefollowing
natural way:One has indeed:
If we endow D’ with the
strong
dualtopology,
then(D’ , D)
is atopological quasi *-algebra [19J.
In an obvious way we can define a*-representation
of
D’ :
In this case E
£(D, D’~, ~
extends therepresentation
1ro and it isfaithful too. We want to show that this
representation
isexactly
the onedefined in the first
part
of this section.In order to do
this,
we startby introducing
the sets B ={~(~) : ~ ~ 1)’}
and
Bo
=-~~o ~ f ~ : f
ED ~ .
We have to prove that B isuniformly complete
and that
Bo
is dense in it. This can be proveneasily by shewing
that theTf-topology
on D isequivalent
to thetopology
inducedby
1)’ on D itself.Let indeed .~t be a bounded subset of
P~ ~],
then we have:It may be
worthwhile
to remindthat,
of course, thejoint continuity
of themultiplication implies
that the set M . .M is bounded.On the other hand if we consider the norm then we have
where
u(x)
is the unit function.(2)
Our secondexample
is that of the CCRalgebra
on an interval[6].
Thestarting point
isagain
therigged
Hilbert space considered in theprevious
example.
Annales de l’ lnstitut Henri Poincaré - Physique théorique
Let now
210
denote the vector space of all formalpolynomials Q
in onevariable p with coefficients in
D,
i.e.Q
=¿~=o
N E IN with2to
can be made into analgebra by introducing
amultiplication
in thefollowing
way: if3i
=2::=0
andQ2
= then weput
An involution can also be introduced
easily
in210 by
means of thefollowing
formula:
With this definition is a
*-algebra.
Let now P be theoperator
defined inExample
1. Asalready mentioned,
in this case D =D°(P)
and thetopology t~
coincides with thegraph topology
definedby
P. Of courseP E
,C~ (D) ,
so that it admits aunique extension, again
indicated with thesame
symbol,
toD’,
definedby
Let 03A6 be the
multiplication operator defined,
for 03A6 ED’,
as in(3.2).
Then E
£(D, D’) and,
inparticular,
if 03A6 ED,
thenbelongs
to This allows us to define a
representation
03C0o of210
on D inthe
following
way:The
representation
7r 0 isfaithful;
indeed if7!~(Q)
=0,
then=
0,
for E D.Now,
for~) = u(x) = 1,
b’x E[0,1],
we
get
po =0;
the choice of~(x)
= x, Vx E[0,1], implies
that pi =0,
and so on. Thus we may have7r o( Q)
= 0only
if all coefficients are zero. This in turnimplies
thatQ
= 0.Let us now endow with the
topology TD
definedby
the seminormswhere .Mis a bounded subset in D. It is shown in
[ 12]
that thecompletion 2to
ofo
withrespect
to thistopology
contains thefollowing
spaceVol. 69, n 2-1998.
258 J.-P. ANTOINE, F. BAGARELLO AND C. TRAPANI
Incidentally
we observe that is aquasi *-algebra.
Therepresentation
03C0o can be extended to the wholeQlo.
This extension isclearly given by:
It is easy to check
(by
means of the sametechnique
as in theprevious example)
that 7r coincidesagain
with the one discussed in the firstpart
of this section.3.2.
Sesquilinear
form extensions within agiven quasi *-algebra
We have proven in the
previous
section that a faithful*-representation
of a
*-algebra generates
atopological quasi *-algebra,
to which03C0o can be extended. Now we consider the
problem
of the extension of a*-representation
when thetopological quasi *-algebra
isgiven
apriori.
Let (2t[r],
be atopological quasi *-algebra
and ~-o a*-representation
of on the domain := D. As we have seen in the
introduction,
one has
Thus another
possibility
forextending
is toimpose closability
in£(D, D’)
instead of,Ct (D, H) .
Thisrequires
that we consider the varioustopologies
described in Section 3. i . Thus we assume that,C(D, D’)
isendowed with Top, where Top stands for any of the
topologies
Ts, Tw.
DEFINITION 3.3. - We say that
03C0o is op-extendible if
it is closable asa linear map
from
to£(D,
This meansthat, for
any net{X~}
such thatX~ --~
0 and~
Y E£(D, D’),
itfollows
that Y = 0.
It is clear that the four notions of
extendibility
we havegiven
compare in thefollowing
way:T1) -extendible
~s*-extendible
~s-extendible
~Tw-extendible.
If 03C0o is
op-extendible,
then weput
Annales de l’lnstitut Henri Poincaré - Physique théorique
For X E we =
Top- lim
Thus 7r is well-defined and extends ~o .LEMMA 3.4. -
If
Ts, then X Eimplies X*
ETop).
If
ToP =TD
or Top = thenA ~ o imply
AX, XA
EProof. -
The first statementdepends
on thecontinuity
of theinvolution;
the second on the
continuity
of themultiplications,
as discussed inSection 3.1. D
Thus we
get
twoquasi *-algebras
overPROPOSITION 3.5. - and
T-w)
arequasi *-algebras
overOf course, what we want are
topological quasi *-algebras,
and thisrequires
some additionalinput.
Let p~ be a(directed) family
of seminormsgenerating
thetopology
T of 2tand qa
a(directed) family
of seminormsgenerating
Top, where Top or Top = Then we can define a newtopology
TJop onby
thefamily
of seminormsBy
the construction itself it follows thatPROPOSITION 3.6. - is a
topological quasi *-algebra
overIf
both and,C(D, D’) ~~rop~
arecomplete,
thenTop)
iscomplete.
If
,C(D, D’)
isop-complete,
thenTop)
can be rewritten in thefollowing
wayIt turns out that in several
examples
this domain D has aspecial
form.This
happens,
forinstance,
when there exists aself-adjoint operator
H in Hilbertspace H
such that D =D~(H).
In this case the
topology ~ ±
coincides with thetopology
definedby
the seminorms
Without loss of
generality,
we may assume that H >1;
in this case we haveVol. 69, n° 2-1998.