DE L ’U NIVERSITÉ DE C LERMONT -F ERRAND 2 Série Mathématiques
A NGEL R ODRIGUEZ P ALACIOS
An approach to Jordan-Banach algebras from the theory of nonassociative complete normed algebras
Annales scientifiques de l’Université de Clermont-Ferrand 2, tome 97, série Mathéma- tiques, n
o27 (1991), p. 1-57
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AN APPROACH TO JORDAN-BANACH ALGEBRAS FROM THE THEORY OF NONASSOCIATIVE COMPLETE NORMED ALGEBRAS
Angel
RODRIGUEZ PALACIOSINTRODUCTION
The aim of this paper is not to make a survey of all the results which are known on Jordan-Banach
algebras,
butonly
of those results which can beobtained,
as aspecialization
for Jordan-Banachalgebras,
from
general
results of thetheory
of nonassociativecomplete
normedalgebras.
Also we willstudy
some sides of thetheory
of nonassocia- tivecomplete
normedalgebras which, surprisingly,
lead to Jordanalgebras.
For clearness we also consider the case of noncommutative Jordan-algebras,
forthey
include(commutative)
Jordanalgebras
andassociative
(even alternative) algebras. Thus,
in each case, we willrecall,
from thetheory
of(associative)
Banachalgebras,
the resultwhich
suggests
theproblem
underconsideration,
we will state its non- associative extensionand,
toconclude,
we will see itsparticulari-
zation for noncommutative Jordan-Banach
algebras.
In this way we willre-encounter the associative result of
departure.
A
systematic study
ofgeneral
nonassociative normedalgebras
hasbeen made
only
veryrecently.
However there are someimportant
classi-cal
precedents
which we also include in this survey. Also we considersome
interesting problems
on nonassociativecomplete
normedalgebras,
with indication of the answer
(when
it isknown)
in the case of non-commutative Jordan-Banach
algebras.
This paper contains also severalnew results and some new
proofs
of known results.This paper is an
improved
version of my talks at the"Colloque
surles
alg6bres
de Jordan"(Montpellier,
October1-4, 1985).
SUMMARY.
1.
C*-algebras.
2. Smooth normedalgebras.
3. Remarks on numerical ranges. 4.Uniqueness
of normtopology.
5.Decomposition
for normedalgebras.
6.H*-algebras.
7. Automaticcontinuity.
1.
C*-ALGEBRAS
There are many concepts in order to obtain Jordan structures which
are the
"analogous"
of associativeC*-algebras.
Thus we have the JB-algebras, JB*-triples, JB*-algebras
and noncommutativeJB*-algebras.
We
give
the first reference for each one of these concepts([6,43,80,58], respectively)
and the reader is referred to the books of Iochum(361,
Hanche Olsen-St6rmer[33] and Upmeier [74]
for a com-plete study
and a wide list of references.But,
since our purpose is"nonassociative",
we look for those non-associative
algebras
which are theanalogous
ones of associativeC*-
algebra*.
To this end we will recall the Vidav-Palmertheorem,
for itgives
a characterization ofC *- algebras
which does not involve theproduct
of thealgebras
butonly
its Banach space and its unit.To state the Vidav-Palmer theorem we need some concepts which we
give
here for the nonassociative case in order to avoidrepetition.
Let A be a unital nonassociative normed
algebra
and let A’ denote its dual Banach space. For any a in A we define the numerical range ofa
(V(a,a)
orV(a)
when confusion is notpossible) by
V(a) - ( f (a) :
f EA’,
(lfil -f (I) = 1) ,
where I denotes the unit of A.If A is a
complex algebra
andV(a) c [R
we will say that a is an hermi- tian elemen t of A andH(A)
will denote the closed realsubspace
of allhermitian elements of A.
By definition,
aV-algebra
is a unital non-associative
complete
normedalgebra
Asatisfying
A -H(A)
+iH(A).
Itis not difficult to see that if A is a
V-algebra
then themapping
h+ik 2013~ h-ik
(with
h and k inH(A))
is a continuous involution on the Banach space of A which will be called the natural involution of theV-algebra
A.Now we can state the Vidav-Palmer theorem
(see [16;
Theorem6.9]
for
example).
Theorem 1.1
(Vidav-Palmer). Every
unital associativeC*-algebra
is an(associative) V-algebra. Conversely,
every associativeV-algebra
withits natural involution is a unital associative
C*-algebra.
From our
point
of view this theorem shows that nonassociative V-algebras
are the natural nonassociativeparallel
of unital associativeC*- algebras.
Thequestion
is : how far atheory
of nonassociative V-algebras
can bedevelopped ? Surprisingly
the answer is much better that it could beexpected
at firstsight.
The fact is that we have thefollowing
first result which is crucial for our purposes.Theorem 1.2
[63].
The natural involution of every nonassociative V-algebra
is analgebra
involution.This theorem was first
proved by
Martinez[49]
for theparticular
case of Jordan
algebras.
We recall that an involution * on the vector space of acomplex algebra
is called analgebra
involution if(ab)* ~b*a*
for every a and b in thealgebra.
Thei
secondsignificant
result on nonassociativeV-algebras
wasproved by Kaidi,
Martinez andRodriguez
under theassumption
that thenatural
involution is analgebra
involution.But, by
Theorem1.2,
thisassumption
issuperfluous.
So we have:Theorem 1.3
[42]. Every
nonassociativeV-algebra
is a noncommutative Jordanalgebra.
We recall that a noncommutative Jordan
algebra
is a nonassociativealgebra
Asatisfying (ab)a - a(ba) "flexibility"
anda2b a = a2 ba
"Jordan axiom" for all a and b in A.
To state the third and
concluding
result on nonassociativeV-alge-
bras we need to recall the concept of noncommutative
JB *- algebra.
Anon-commutative
JB -algebra
is a noncommutative Jordancomplete
normedcomplex algebra
A withalgebra
involutionsatisfying IUa(a*)1 - llal,3
for all a in A
(where Ua(b) - a(ba)
+(ba)a - ba2).
Theconcept
ofJB*- algebra
was introducedby Kaplansky
in the unital commutativecase and was studied
by Wright [80]
in this case,by Youngson [86]
inthe non-unital commutative case and
by Paya,
Pdrez andRodriguez [58]
in the non-unital noncommutative
general
case. From the results in[19,59,7]
one may describe all noncommutativeJB*-algebras,
forthey
are the closed
selfadj oint subalgebras
of~-products
of noncommuta- tiveJB*-factors
and the noncommutativeJB*-factors
are well known.Now,
as a consequence of Theorem 1.2 and 1.3 and a result ofYoug-
son
[84,85]
andRodriguez [62]
on JordanV-algebras,
we have the fol-lowing
theorem which says thatstudying
nonassociativeV-algebras
isjust
the same asstudying
unital noncommutativeJB*-algebras.
Theorem 1.4
(nonassociative
Vidav-Palmertheorem).
The class of nonas-sociative
V-algebras
agrees with the class of unital noncommutativeJB*-algebras.
An
important
consequence of Theorem 1.2 and 1.3 is thefollowing corollary (see
theproof
of[63;
Theorem12]
fordetails).
Corollary
1.1 Under theassumption
of existence of a unit I, thealgebraic
axioms(flexibility
and Jordanaxiom)
aresuperfluous
in thedefinition of noncommutative
JB*-algebras
and theassumption
that theinvolution
is analgebra
involution can be weakened to theassumption
I*=I.
For the non-unital case we have also a new result
weakening
theaxioms of noncommutative
JB*-algebras.
This result is also a conse-quence of the ones above and of a theorem of
Youngson [86]
on thebidual of a non-unital
(commutative) JB*-algebra. Following [7]
a non-associative
complete
normedcomplex algebra
A is called admissible if thealgebra A+ ,
obtainedby symmetrization
of theproduct
ofA,
is aJB*- algebra
for thegiven
norm on A and for a suitable involution(notice
that this involution is not assumed to be analgebra
involu-tion on A but
only
onA+).
It is clear that every noncommutativeJB*-
algebra
is admissible. To state the converse we must prove that thealgebra
is flexible and that thegiven
involution is analgebra
invo-lution on A. These facts are true as shows the
following.
Corollary 1.2. Every
nonassociativecomplete
normedcomplex
admissiblealgebra
isactually
a noncommutativeJB*-algebra.
Proof. Let A denote our admissible
algebra.
As in theproof
of[58,
Theorem
1.7] (where
we assume A to be a noncommutativeJB*-algebra
butwe
only
use that A isadmissible)
we have that the bidual A" of A, with the Arensproduct,
is a nonassociativeV-algebra,
the naturalinvolution of which extends the
given
involution onA+. Thus, by
Theo-rem
1.4,
A"(and
soA)
is a noncommutativeJB*-algebra.
It must be noted that Theorem 1.4 contains the associative Vidav-Palmer theorem and even its extension for alternative
algebras. By definition,
analternative
C*-algebra
is an alternativecomplete
normedcomplex algebra
Awith
algebra
involutionsatisfying Ila*all = Ilall2
for all a in A. AlternativeC*- algebras
were studied in[58,20].
From theidentity Ua(b) - aba,
whichis true for alternative
algebras,
it is not difficult to provethat,
for analternative normed
complex algebra
withalgebra involution,
the axiomsiiua(a*)11 - llaII3
andlla*all = Ila, 112
areequivalent.
Thus the alternativeC*-algebras
arejust
those noncommutativeJB*-algebras
which are alterna-tive.
Now,
as a direct consequence of Theorem1.4,
we havei
Corollary
1.3[62,20].
The class of alternativeV-algebras
agrees with the class of unital alternativeC*-algebras.
,
. ,-
It is
surprising
that thealgebras
in the abovecorollary
are theonly
unital ’nonassociative
complete
normedcomplex algebras
with involutionsatisfying
the Gelfand-Naimark axiom!ta a)) 2013 IlaII2.
Theproof
of this resultuses Theorem 1.2 and 1.3 and a theorem of
Wright-Yougson [81]
on isometriesof
JB-algebras.
Theorem 1.5
[62].
Let A be a unital nonassociativecomplete
normedcomplex algebra
with involution *satisfying I*=I (where
I denotes the unit ofA)
and
Ila*all - llall2
for all a in A. Then A is alternative and * is analgebra
involution on A
(that
is : A is an alternativeC*-algebra).
In Theoreaa’1.3 and 1.5 we have obtained from
geometric assumptions
on ageneral
nonassociativecomplete
normedalgebra
somealgebraic
identities.In the same way we can even
give
a characterization of associative and com-mutative
C*-algebras
among nonassociativecomplete
normedalgebras.
Tostate this result we recall that the numerical radius
v(a)
of an element aof a unital nonassociative normed
algebras
A is definedby
v(a) - sup( lzl :
z EV(a)},
and the numerical indexn(A)
of A is definedby n(A) - inf(v(a) :
a E A, liall -1 ) .
Now we have :Theorem 1.6
[62].
The class of nonassociativeV-algebras
with numerical radiusequal
to one agrees with the class of unital associative and commu-tative
C*-algebras.
We do not know a
geometric
characterization ofJB-algebras,
amongnonassociative
complete
normedalgebras, analogous
to the onegiven
inTheorem 1.4
for
noncommutativeJB*-algebras .
We recall thatJB-algebras (which
are the Jordan realanalogous
of associativeC*-algebras)
are defi-ned as those
(commutative)
Jordan-Banach realalgebras
Asatisfying
I1a211 = llal,2
andIla2-b211 max ( II a211 , IIb2n )
for all a and b in A. In theabsence of a
geometric
nonassociative characterization ofJB-algebras
wehave, by putting together
results of Alvermann-Janssen andIochum-Loupias,
the
following
remarkable theorem.Theorem 1.7
[7,37].
Let A be a flexiblepower-associative complete
normedreal
algebra satisfying Ila2il
=II a II 2
andlla2_b2ll {lIa2U,lIb211}
for all a andb in
A.4Then
A is aJB-algebra.
Pr6o’f
From thepower-associativity
of A it follows thatA+
is a power- -associativealgebra. By [37;
TheoremV.1] A+
is a Jordanalgebra.
Thisfact and the
flexibility
of Aimplies
that A is a noncommutative Jordanalgebra
as it is well known. But a noncommutative Jordancomplete
normedreal
algebra satisfying
the usualgeometric
axioms ofJB-algebras
is actual-ly
commutativeby [7;
Theorem7.4].
To conclude this section we state a theorem of Kadison which
gives
anonassociative characterization of the
(associative
andcommutative)
Banachalgebras
of real valued continuous functions on a Hausdorffcompact
space(which
arejust
the associativeJB-algebras
andalso, by
the commutative Celfand-Naimarktheorem,
theselfadjoint
parts of unital associative andcommutative
C*-algebras).
Thus acomplex analogous
of this Kadison’s theorem is Theorem 1.6. We need to recall theconcept
of acomplete
order unit spacewhich,
in a formequivalent
to theoriginal
one[4;
page69]
but more closeto our
approach,
can be formulated as follows : acomplete
order unit spaceis a real Banach space X with a norm-one element u
(the
order unit ofX)
such that for every x in X we have that
llxll -
sup ( I f (x) I
: f EX’ ,
11 f 11 -f (u)=1 ) (in
terms of numerical ranges in Banach spaces, see Section3,
X is a real numerical range space with nume- rical indexequal
toone).
An element x of X is said to bepositive
iff (x) ~
0 for every f in X’ with llfll -f(u) -
1. Now we have :Theorem 1.8
[41].
Let A be a nonassociative realalgebra
which is also acomplete
order unit space. Assume that the order unit of A is also a multi-plicative
unit. for A and that theproduct
ofpositive
elements of A is alsopositive.
Then A isalgebricaly
andisometrically isomorphic
to thealgebra
of all real valued continuous functions on a suitable Hausdorff compact space.
2. SMOOTH NORMED ALGEBRAS
By
definition a smooth normedalgebra
is a unital nonassociative normedalgebra
A with theproperty
that the normed space of A is smooth at the unit I of A(that
is : there is aunique
element f in A’ such thatllfll -
£(I) - 1,
or,equivalently,
the numerical range of any element in A containg aunique number).
From Bohnenblust-Karlin theorem(see [16;
Theorem4.1]),
which is also true for the nonassociative case via[62; Corollary 2(a)],
it follows that C is theunique (nonassociative)
smooth normedcomplex algebra.
But for associative realalgebras
thefollowing
result iswell known
(see [16;
Theorem6.16]) :
Theorem 2.1
(Bonsall-Duncan). Irk
and ~i(the algebra
of realquaternions),
with its usual.modulus as norm, are the
only
associative smooth normed realalgebras.
This theorem shows that the
assumption
of smoothness for normedalge-
bras is very restrictive. Thus it seems
interesting
tostudy
this assump- tion in thegeneral
nonassociative case. In this direction there are someparticular
results of Strzelecki[73]
forpower-associative algebras
andNieto
[56]
for alternativealgebras.
We
give
here adescription
of nonassociative smooth normedalgebras,
aconsequence of which is that
they
are flexiblequadratic algebras (so
non-commutative Jordan
algebras)
and that the normed space of each one of them is an innerproduct
space.Our construction
begins
with an anticommutative normed realalgebra
Ethe normed space of which is an inner
product
spacesatisfying (x
A y Iz) _ (x
I y Az)
for all x,y and z in E(where
A stands for theanticommutative
product
ofE).
Such analgebra
is called apre-H-algebra.
As an
example,
which should not beforgotten,
every innerproduct
real space with zeroproduct
is apre-H-algebra.
Let E be apre-H-algebra
and considerthe vector space IR x E with
product (z,x)(w,y)
:-(zw - (xlt), zy+wx+x
Ay)
and norm
D(z,x)1I2:- Z2+llx,12.
It is not difficult to see([63; Proposition 24])
that in this way we have obtained a smooth normedalgebra
which(being obviously
a flexiblequadratic algebra)
is called the flexiblequadratic algebra
of thepre-H-algebra
E. Now we can state the main result in thissection.
Theorem 2.2
[63]. Every
nonassociative smooth normedalgebra
is the flexi- blequadratic algebra
of a suitablepre-H-algebra.
The
proof
of this theoremgiven
in[63]
uses the main results in thepreceding
section. Wegive
here a newproof
of Theorem 2.2 which does not involve the results in Section 1and, consequently,
we think that it ismore
simple. Previously
we prove two lemmas.Lemma
2.1. Let a be inH(A),
where A denotes a unital nonassociativecomplete
normedcomplex algebra.
Then the numberllall2 belongs
to the nume-rical range of
a2.
Proof. We may assume llall - 1 and
also, by
the nonassociative Sinclair theorem(see
the comments before[63;
Lemma3]),
that 1 EV(a).
Let g be in A’ such thatligil - g(I) = g(a) =
Iand,
for any F in the unital Banachalgebra BL(A)
of all continuous linear operators on A, writei(F):-g(F(I)).
Thus g belongs
to(BL(A))’
and satisfiesg(La) - g(IA) = llgll
=IlLall = 1,
where
La (the
operator of leftmultiplication by a) belongs
toH(BL(A)) by [62; Corollary 2]. Applying [17; Corollary 26.10]
we obtain thatg(a2) - g L2 =
a 1. Therefore 1 EV(a2)
asrequired.
Lemma 2.2. Let A be a unital nonassociative
complete
normed realalgebra
and let E denote the closed
subspace
of all elements x in A withV(x)-(0).
Then we have :
i) xy - yx E E
for x and y in E.ii) (xy)z - x(yz)
E E for x,y and z in E.iii)
-llx,12
EV(x 2)
for x in E.iv)
llzj +xl,2 _ z2
+lix,12
for x in E and z in IR.Proof. As in the associative case
[18;
Section13]
we can consider thecomplete
normedcomplexification Ac
of A. Let a be in A, thenV(A,a) - ReV(AC,a) [63;
Lemma25] and,
inparticular,
a E E if andonly
ifia E
H(AC).
Nowi)
andii)
follows from[42;
Lemma3], iii)
from thepreceding lemma,
andiv)
from[63;
Lemma3(b)].
A’Proof of Theorem 2.2. Let A denote our nonassociative smooth normed
alge- bra,
which can be assumedcomplete,
and let f be theunique
element in A’with llfll -
f(I) -
1. We haveV(a) - ( f (a) )
for every a in Aand,
inparti- cular,
E =Ker(f) (where
E has the same sense that in thepreceding lemma).
From Lemma 2.2
i)
andiii)
it followsthat,
if for x,y in E we write(xly)
:--f(xy) ,
then( I )
is asymmetric
bilinear form on Esatisfying (xlx) a Ilxll2 .
Therefore E is an Hilbert space. From Lemma 2.2i)
we havethat E is closed under the anticommutative
product given by
x A y :.,
(1/2(xy-yx) .
Sinceclearly
we have IIX Ayll
IIXIIllyll
and the equa-lity (x
nylx) - (xly
nz)
is deduced from Lemma2.2.i)
andii),
it followsthat E is an
H-algebra (complete pre-H-algebra).
For x in E we havex2 = wI+y
for suitable w in IR and y in E.But, by
Lemma 2.2iii),
we-IlxII2
and so,
by
Lemma 2.2iv), llxll4
+lly2ll2 Ilxll4,
whichimplies y-0.
Thus wehave
proved
.
that
x2 = _Ilx,12,,
so(1/2)(xy+yx) - -(xly)I
and soxy -
-(xly)I
+xAy
for all x,y in E. From the lastequality
it is clearthat the
mapping
zI+x ~(z,x)
fromA(=
[II 0E)
onto the flexiblequadratic algebra
of theH-algebra
E is anisomorphism.
Thisisomorphism
is an isome-try by
Lemma 2.2.iv),
which concludes theproof.
Remark 2.1. Theorem 2.2
gives
acomplete description
of commutative smooth normedalgebras,
since the flexiblequadratic algebra
of apre-H-algebra
iscommutative if and
only
if thegiven pre-H-algebra
has zeroproduct,
thatis : the
pre-H-algebra
is anarbitrary
innerproduct
spaceequipped
withthe zero
product.
Toget
a similar fulldescription
of noncommutative smooth(even complete)
normedalgebras
we need to know theH-algebras
with nonzero
product.
In Section 6 we will find some information about thisproblem.
Remark 2.2. For a unital normed
algebra
A definea(A)
as the diameter of the set(f
E A’ : 11 f 11 -f(I) =
1) . The smooth normedalgebras
are thencharacterized as those unital normed
algebras
Asatisfying a(A) -
0. Lummer[47] proved
thefollowing
extension of Theorem 2.1 : There is apositive
number k such
that,
if a unital associative normedalgebra
A satisfiesa(A) k,
then A isisomorphic (not necessarily isometric)
toIR,
C or H.It would be
interesting
to find a nonassociative extension of this result.From Lummer theorem it follows
easily
that if A is a unitalpower-associa-
tive normed
algebra
witha(A) k,
then A is aquadratic algebra
with theproperty
that every element is invertible in the(associative) subalgebra generated by
it. Inparticular
if A isalternative,
then A isisomorphic
toR, C, H
or 0(the algebra
of realoctonions).
We conclude this section with a result in which we enclose the theorem of
Albert-Urbanic-Wright [2,3,79,75]
on absolute valuedalgebras
with unitand the theorem of Nieto
[56]
on alternative smooth normedalgebras.
Thisresult can be obtained from Theorem 2.2 with more or less difficulties
(see [56,63]
fordetails).
We recallthat, by definition,
an absolute valuedalgebra
is a real orcomplex algebra
with a normsatisfying
Ilabll -llallllbll
for all
a,b
in thealgebra. C
is theunique
unital(nonassociative)
abso-lute valued
complex algebra.
But, for the real case, we have :. ’
Theorem 2.3
[50,75].
Let A be a realalgebra.
Then thefollowing
statements are
equivalent :
i)
A is a unital nonassociative absolute valuedalgebra ii)
A is an hlternative smooth normedalgebra
iii)
A -R, ~,~i
or 0 with its usual modulus as norm.3. REMARKS ON NUMERICAL RANGES
In the
preceding
sections we have seen the more attractive results onnumerical ranges in
general
unital nonassociativecomplete
normedalgebras,
with the remarkable consequence
that,
if such analgebra
has a"good
beha-viour" for numerical ranges, then it is a noncommutative Jordan
algebra.
Itwas first noted in
[49,84]
that most of thetheory
of numerical ranges in(associative)
Banachalgebras [16,17]
can be extended to Jordan-Banachalgebras,
and in[42,62,63]
one may find someingenuous (but powerful) techniques
in order to transfer results on associative numerical ranges to thegeneral
nonassociative case. Theproof
of Lemma 2.1 is anexample
ofthis
procedure.
Thus one istempted
todevelop
atheory
of nonassociative numerical rangesby reproving directly
in the nonassociative case the results which are known for the associative one.Actually
this ispossible
and the author has
given
at theUniversity
of Granada apostgraduate
cour-ses on this
topic. However,
in absence ofpower-associativity,
thearguments
in theproofs
are sometimesunnecessarily
intrincate and no more instruc- tive than the associative ones. In conclusion it ispreferable
to prove theresult in the associative case first and
later, making
use of the abovementioned
techniques,
extend it(if possible)
to the nonassociative case.Even for unital noncommutative Jordan-Banach
algebras,
in which a spec- >dtral
theory
isdeveloped,
therelationship
between the spectrum and the : numerical range of an element is reduced to the associative caseby
the"full closed associative" localization theorem
(see [48]).
,In view of the above comments we think
that,
if one wishworking.in
numerical ranges and if one is weary of associative numerical ranges, then the best direction is to
study
numerical ranges in Banach spaces X(without product)
in which a norm-one element u is selected in order toplay
therole of the
multiplicative
unit in the case of unitalcomplete
normedalge-
bras. Such a
couple (X,u)
is called a numerical range space. The numerical rangeV(x)
of an element x in X is def inedby V(x) _ { f (x) :
llfll -f (u)=1 ~ .
The concepts of numerical radius of x,
v(x),
and of numerical index ofX, n(X) , may
be deducedby analogy
with the case of unitalcomplete
normedalgebras.
Weexplain,
with someexamples,
how thetheory
of numerical range spaces maygive light
even in associative and nonassociative numerical ran-ges. The first
example
is motivatedby
thefollowing
result of Smith.Theorem 3.1
[72].
Let A be a unitalcomplex
Banachalgebra
and let K be aclosed convex subset oft with a non-empty interior.
Then,
for each F in A"with
V(A",F) C
K, there exists a net(a~)
in A which converges to F in thew * -topology
and such thatV(A,aX)
c K for every X.Theorem 3.1 can be
extended, by using techniques
different to the onesin
[72],
toarbitrary
real orcomplex
numerical range spaces and so, inparticular,
to unital nonassociativecomplete
normed real orcomplex alge-
bras. Thus we have :
Theorem 3.2
[50].
Let X be a numerical range space and let K be a closedconvex subset of the base field with non-empty interior.
Then,
for each Fin W" with
V(F)
C K, there exists a net(x~)
in X which converges to F in thew -topology
and such thatV(xX) c
K for all A.As a consequence we obtain the
following
result which was not observedpreviously
even for unital Banachalgebras.
Corollary
3.1[50].
For every numerical range space X we have thatn(X")-n(X).
New Proof.
Clearly n(X") n(X)
and so it isenough
to prove the converseinequality.
Let F be in X" and let E be anarbitrary positive
number. ThenV(F)
is contained in (z C- 0 : lzl %v(F)
+ E } which is a closed convexsubset of the base field K with non-empty interior.
By
the theorem there*
w B
exists
{xh}
} in X such that(xX) w
F andv(x ) £ v(F)
+ E. Sincen(X)lIx>..1I ~ v(x~)
for allB,
we have alson(X)
IIFIIv(F)
+ E in view of thew*-lower-semicontinuity
of the norm on X".Thus,
since E isarbitrary, n(X) IIFII v(F),
and son(X") > n(X)
asrequired.
Some results on numerical ranges in unital
complete
normedalgebras cannot ’,be
extended to the context of numerical range spaces becausethey
involve
i
in the statement the
product
of thealgebra. But,
even if the pro- duct is notinvolved,
there are results onalgebra
numerical ranges whichare not
true for numerical range spaces. Asimple example
is the Bohnenblust- -Karlin,theorem, stating
thatn(A) > 1/e
for every unitalcomplete
normedcomplex algebra
A, which fails in everycomplex
numerical range space(X,u)
with X a Hilbert space of dimension greater or
equal
to two. This shows that thegeometry
of the numerical range spaces of unitalcomplete
normedalgebras
is verypeculiar.
In this respect we must cite a relevantgeometric property
of unitalcomplete
normedalgebras
which is easy to prove and which was first noticed in[50].
To state this result we recall some con- cepts. For x in the unitsphere S(X)
of agiven
Banach space X we writeD(x) - (f
E X’ : llfll -f (x) - 1 }
Themapping
x -+D(x)
fromS(X)
into theset of
non-empty
subsets of X’ is called theduality mapping
of X. Follo-wing [32],
theduality mapping
of a Banach space X will be said(n,n) -
(resp. (n,w)-) upper-semicontinuous
at apoint
x inS(X)
if for every n-(resp. w-) neighbourhood
of zero U in X’ there is an E > 0 such that if y ES(X)
andlix-yll
E, thenD(y)
CD(x)
+U,
where n(resp. w)
denotes thenorm
(resp. weak) topology
on X’. Now we have :Proposition
3.1[50].
Let A be a unital nonassociativecomplete
normedalgebra
and let I denotethe
unit of A. Then theduality mapping
of theBanach space of A is
(n,n)- (so
also(n,w)-) upper-semicontinuous
at I.Proposition
3.1 and the Bohnenblust-Karlin theorem(for
thecomplex case)
are twoindependent important geometric properties
of unitalcomplete
normed
algebras
from which many others suchproperties
can be codified. Asan
example :
for any numerical range space(X,u)
the fact"n(X)
> 0" and"X’ is the linear span of
D(u)"are equivalent [50],
and so the Bohnenblust- -Karlin theorem and the Moore-Sinclair theorem([17;
Theorem31.1])
can bededuced each one from the other. To show another
example,
consider the ,I’~following
result :Theorem 3.3
([16;
Theorem12.2]).
Let A be a unital Banachalgebra.
Thenfor every F in A" we
have V(F) = (F(f) :
f ED(I))- (where -
denotesclosure).
This theorem
(and
even its nonassociative extension[62])
is now adirect consequence
ofProposition
3.1 and thefollowing
1
Theorem 3.4
[32].
Let(X,u)
be a numerical range space. Then thefollowing
..
statements are
equivalent :
i)
Theduality mapping
of X is(n,w)-upper-semicontinuous
at u.ii)
Theequality V(F) = (F(f) :
f ED(u))-
is true for every F in X".We conclude this
quick
incursion in numerical ranges in Banach spacesby stating
a result on thistopic
from which one canobtain,
for unitalcomplete
normedalgebras,
animportant generalization
of Theorem 3.3.Theorem 3.5.
[8].
Let(X,u)
be a numerical range space such that X is the dual space of a suitable Banach space~~.
Assume that theduality mapping
of X is
(n,n)-upper-semicontinuous
at u. Then for every f in X we haveV{f ) = t f (p) :
I pE X,~, Ilpli = u(p) = 1}-.
.Now,
fromProposition
3.1 and Theorem3.5,
we obtain thefollowing
ex-tension of Theorem 3.3.
Corollary
3.2. Let A be a unital nonassociativecomplete
normedalgebra,
the Banach space of which is the dual space of a suitable Banach space
A*.
Then for every f in A we have
V (f ( f (p) :
pE A*, llpll - I(p) = 1)
Normed
algebras
whichsatisfy
theassumptions
of thiscorollary
are,among
others,
the biduals of unital normedalgebras
with Arensproduct (for
which our
corollary
isjust
Theorem3.3),
the(associative) W*-algebras
[65],
the noncommutativeJW*-algebras [58],
and the extremalalgebra
of acompact
convex subset of C[17;
Section24].
Remark 3.1. The content of this section may be considered as a modest
project
of reconciliation between Banachspacits
and Banachalgebrists,
which sometimes are not well behaved. As an
anecdote,
in the paper[32],
where Theorem 3.4 is
proved (in
anequivalent
form and with different termi-nology),
no reference is made on theapplication
of this theorem to unitalnormed
algebras. Fortunately,
such aproject
of reconciliation has now manyprotectors
once the Jordan-Banachalgebrists
have beennicely surprised by
the recent Dineen’s
proof [26] (see
also[15~)
that the bidual of aJB *- triple
is anotherJB *- triple , by using
theprinciple
of localreflexitivity.
In
>spite
of what was said before about the interest of Banach spacenumerical
ranges versusalgebra
numerical ranges, we wish cite some aspects ofalgebra
numerical ranges which can beexplored.
The reader should take adecision on wether or not this line seems
interesting.
Thestarting
idea isto weaken no much the usual axiom Ilabli liall Ilbil for normed
algebras
insuch a way that the classical
theory
of numerical ranges in unitalcomplete
normed
algebras
is notperturbed.
Since"weakening
axioms" is not a sugges- tivephrase
inmathematics,
wegive
a motivation which appearnaturally
inthe context of
(commutative)
Jordanalgebras.
Let A be a real or
complex
Jordanalgebra
with unit I which is also aBanach space
satisfying
IIIII - 1.Taking
into account theequivalent
axiomsfor Jordan
algebras given by
MacCrimmon[51]
in terms of thequadratic
ope- ratorUat
it seems to be more natural to assumeIIUa(b)1I ~ llall2 llbll
insteadof the usual axiom lia.bll liall llbli