DE L ’U NIVERSITÉ DE C LERMONT -F ERRAND 2 Série Mathématiques
B RUNO I OCHUM G UY L OUPIAS
Banach power-associative algebras : the complex and (or) non commutative cases
Annales scientifiques de l’Université de Clermont-Ferrand 2, tome 97, série Mathéma- tiques, n
o27 (1991), p. 93-106
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BANACH POWER - ASSOCIATIVE ALGEBRAS : THE COMPLEX AND
(OR)
NON COMMUTATIVE CASESBruno IOCHUM
and
Guy
LOUPIASINTRODUCTION
In
apreceeding
paper[6],
we defined the class of real Banach power- associative 1algebras (Bpa-algebras)
andproved
itsequivalence
with that ofJB-algebras.
The redundance of the Jordan conditionA.(B.A") - (A.B).A2
99 in:,
the definition of
JB-algebras
wasalready
noticed for thecomplex
case andthe more
general setting
ofV-algebras
in[10].
In[6],
this fact allowedus to deduce the Jordan structure of a
system
of observables from moreelementary
andphysical principles.
It is then natural to extend our
investigations
to the class of commu-tative and non commutative
complex Bpa-algebras
with involution. We willsee that if the
parallelism
withJB*-algebras
remains in the commutative case, itdisappears
in the non commutative one.In the
sequel,
the mention "non associative"(respectively :
"non com-mutative")
will mean : notnecessarily
associative(respectively :
notnecessarily commutative) :
see[11]. Algebras A are
called Banachalgebras
if there is a norm
on A
such thatIIAII IIBII , A,
B EA,
and A iscomplete.
For anyA,B
in analgebra A,
define A 0 B -(A.B
+B.A)/2
andU A B = A.(B.A)
+(B.A).A - B.A2.
An involution will be anapplication,
deno-ted
*,
from acomplex
vectorspace A
into itself such that ’It A -
A*,
A is calledself-adjoint
and the set ofself-adjoint
elements isdenoted
by ~,a..
Finally,
Jy will be the dual oaf AI. THE COMPLEX COMMUTATIVE CASE
The real commutative case
beeing
described in[6] ,
webegin
with somedefinitions
corresponding
to thecomplex
commutative case.Definition I .1.
A commutative Banach
power-associative *-system (Bpa*-system)
is acomplex
Banachspace A equipped
with1°)
a square map, i.e. anapplication
from A into A denotedI
such’that
inducing
a"product"
and a power
operation
If there exists some element
I
E A such thatit will be called a unit of As
If
A,B,...6 ~t, ~(A,B,...)
will be thesubspace
of 3Égenerated by A,B,...,
and n if it
exists, through
linearcombinations,
powers andproducts,
andC(A,B,...)
its closure.’
2)
an involutibn * such thatif
theproduct
is associative(8)
the square is continuous onC(A,A *)f
onSI(A,A*)
A
subsystem B c A
will be asubspace
of A stable undersquaring
andinvolution.
Proposition
1.2. Let A be a commutativeBpa* -system.
Then0*-0,
1 is uni-que if it
exists,, 0~ - 0,
A.0 -0, (-A)2 _ A ,
is stable underproduct.
If Be A is a
subsystem
of A such thatA.(iB) - i(A.B), A,B
6B,
theproduct
on B is distributive andCQ-bilinear
with A.A -A2
whereCQ
denotesthe
complex
numbers with rationnal real andimaginary
parts, the involution on 3 ismultiplicative
and(2)
is redundant if H 6 B.If A E
IIA211 - IIA,12
and thesubsystem C(A)
is an associative commutative Banachalgebra.
Inparticular
111111 - 1.Proof. The first assertions are obvious thanks to
(1)
and(5)
as02 _ (iO)2
-_02 _
0. If B is asubsystem
asquoted above,
thenA. (-B) - - (A.B)
on B and the claimedproperties
can beproved
as in([6], Proposition 1.4).
If A -A*, ~(A)
is such asubsystem
thanks to(4).
AsAlbert’s
proof
of the fact that(3) implies power-associativity
relies onthe use of rational numbers
only [ 1 j , 9(A)
is associative andIIAII2
on
d1s . a. by (6) .
IfB,
C E9(A),
then as in( [6J ,
Proposition 1.4)
so thatbilinearity
on~(A)
extends to thecomplexes by density.
Moreover llB.Cll 4 uBll llCll thanks to(6)
and theassociativity
as in([6], Corollary I.6). Finally
theproduct
onC(A) beeing
continuous onC(A)
thanks to
(8),
all theseproperties
extends to thesubsystem C(A).
If A has a
unit,
we will define the numerical range of A E A as in the context of associativealgebras according
tov.4(A) -
where
DdB( n) - 1Ip1l - 1).
Thesignificance
of this defini- tion relies on the Hahn-Banachtheorem,
which also insures thatVB(A) -
if A 6 B C: .4 with The numbervA(A) -
sup(IÀI ;
; a EVA(A»
will be called the numerical radius ofA,
andA will be said hermitian if R. The set of hermitian elements will be denoted
by
and isobviously
a real Banach space. It is evident from the def inition thatVA(Àn
+ A +>Vy(A),
CVy(A)
+ andIIAII where E C and
A, B
E JI . If A -A*,
thefollowing results,
valid in associative Banach
algebras,
are still truein 3Yby
restriction toC(A) :
t
(9)
~
V.4(A)
is a nonempty compact
convex subsetof C ;
(10)
j If p is . thespectral radius,
thenPC(A)(A) - v .4(A) -
IIAII.",J.. *
Proposition
I.3. Let A be a commutativeBpa*-system
with unit. Thend1s. a... H(A); A= H(A)
+iH(A)
andIIA*II
2llAll.lemma
5.2) applied
toC(A). Conversely,
let A E and A -Al+iA2
whereAl - (A+A*)/2
andA2 - (A-A*)/2i.
ThenA 1
andA2 beeing self-adjoint
arehermitian,
and so isiA2 - A-A!.
So then~(A2)
E IR which
implies successively
thatcp(A2) = 0, v(A2) -
0 andA2-0 by
(10).
Hence A -Ai 6
Let now A -Al+iA2 E H(.4)
0iH(A) -
Proposition
1.4. Let A be a commutativeBpa*-system
with unit and a G dÉbesuch that carries an associative
product.
ThenC(A,A*)
is an asso-ciative commutative
C*-algebra.
Moreover if A -A*
then3)(A,A*)
is associa-tive, C(A) nos.a.
is a realJB-algebra
and is a realBpa-system.
Proof.
By (7)
andProposition 1.2, F(A,A*)
has adistributive, -bilinear
and associative
product.
IfB,C
E with B -Bl+iB2,
C -Cl+iC2
and2
Bi, Ci
° ° for i -1, 2,
then llB. Cll 21libill IIC111*Hence bilinearity ij-1
extends to the
complexes
because ifXr -
+ i tends to X EC,
then
_
llBjll IlCkil
+la-ar
I IIB. CII tends to zero. Moreover(B.C)* - B*.C*,
is associative andIIB.Cn2 - llB*.B.C*.Cll
2llB*.Bll 11C*. CII = 211B112 IICII2,
whence IIBII IICIIby
induction. Inparticular
* is isometric on31(A,e),
and also onC(A,A*)
(by Proposition 1.3)
which is then an associative commutativeC*-algebra.
If A S
A*, C(A) s.a.
is a realJB-algebra,
and a realBpa-system by [6], Corollary II.4).
j
,
Definition
1.5. A commutativeBpa*- algebra
is a commutativeBpa*- system
~ such that
(1) A. (iB) = i(A.B) A,B
E 4lHence the involution is
multiplicative
on A and(2)
is redundant(see Proposition 1.2).
Definition 1.6. A
JB*- algebra
is acomplex
Banachspace A which
is acomplex
Jordanalgebra
with involution such thatIt has been noted in
[10] that,
in thisdefinition,
themultiplicabi- lity
of the involution and the Jordanidentity
could bereplaced by
theweaker condition I* - 1l in the case of a unital
JB*-algebra.
Definition 1.7. A commutative
V-algebra
is a commutative and non associa- tive Banachalgebra.
with unit such that A -H(~
0 If A -A,
+iA2
with
Ai
EH(~,
i -1,2,
thenA* = A,-iA2
defines a natural continuousinvolution on dl
It is
proved
in([10],
theorem12)
that the class of unital commutativeJB*- algebras
coincides with the one of commutativeV-algebras
with their natural involution andconsequently
is made ofcomplex
unital Jordanalge-
bras with
multiplicative
and isometric involution.Theorem 1.8. A commutative
JB*- algebra
is a commutativeBpa*-algebra.
Conversely,
is a unital commutativeBpa *- algebra,
then it is *-isomor-phic
andhomeomorphic
to aJB *- algebra
withrespect
to a norm 1111,
suchthat IIAII
IIAIi l .
Proof. Let A be a commutative
JB*-algebra.
The involutionbeeing multipli-
cative, I is also isometric
([13],
lemma3)
so thatIIA*All = IIA112
if A andA*
generate
an associativesubalgebra
as in([12],
definition andremarks,
p.291-292Y.
The.otherpoints
are obvious is a Jordanalgebra.
Conver-sely,
let A be a unital commutativeBpa*-algebra. By Proposition 1.4,
~.a, = H(~
is a realBpa-algebra,
that is to say aJB-algebra ([6],
Theorem
V.1) . By ([12],
Theorem2.8),
there exists a norm II111
on A suchthat II
111)
is aJB*-algebra
andIIAII1 -
inf(a ;
A E A convB* } ) .
HenceA E A It is easy to check that IIAII -
IIA,ll if
A( [ 12 ] ,
lemma2.3).
1
Hence,
ifA, B E -%.a.’ IIAII - T
IIA+iB +A-iBll1 IIA+iBill
andMax(IIAII, IIBII)
IIAII + IIBII. As * iscontinuous,
the two norms areequivalent.
Corollary
1.9. be a unitalBpa*- algebra.
Then thefollowing
areequivalent :
Proof.
1 ) -~ 2 )
and3)
are obviousby
definition.2 ) -~ 1) by Proposition 1.3,
which means that A is aV-algebra,
and([10] ,
Theorem12). 3) - 1)
because then
IIAII, 4
IIAII as in( ( 12 ] ,
lemma1.1) .
Infact,
if IIAII1,
letBn
the sequence definedby Bo - A, Bnh-UBn-1Bn-1.
Thentends to zero as
T’
n
tends to
infinity. By equivalence
of the norms, the same would be true forn
IBnU .
1 1But this isimpossible
becauselibno IAU3n -
1.Corollary
I.10. be a commutativeBpa*-system
with unit. InDefini-
tion
1.1,
the condition(6)
isequivalent
toIIA,13
if’i’(A,A*)
isassociative.
Proof.
By Proposition 1.4, (6) implies
the new condition.Conversely,
assume-
thenew
definition. LetA, A*,
Igenerate
an associativesubalgebra
and
B,C,D
E the involution ismultiplicative on 3’(A,A*).
The"algebraic identity B.C*.D
allows towrite that
*
__
27
_ _
Thus ))B.C*.D!) 27
IIBII IICII IIDII andreplacing
C or B and Dby 1, product
and2
involution are continuous on t)B.O)
klIBIl
IICII andllC*ll
kllCll with k >1.Consequently IIB113 = kIlB.B*l
IIBII and11BI12 kIIB.B*II.
.So
and
By induction,
. On the otherhand, by
induc -tion,
andIIBII - DB I by symmetry. Using
the sametrick,
weget
nowThus
k1/3U:BU2
andby
inductionIIBU2.
So inparticular IIAll2
and(6)
is verified.The above
proof
is anadaptation
of([2],
Theorem1.1).
Hence Defini-tion 1.5 is a weakened definition of Alvermann’s commutative
F*-algebras.
In fact Alvermann’s
proofs
do not use the Jordanidentity
butonly
thepower-associativity.
But on the other hand he defines commutative JB- andJB*-algebras
as Jordanalgebras,
which is redundant.II. THE REAL NON COMMUTATIVE CASE
By analogy
with the real commutative case, we introduce thefollowing
definition.
Definition 11.1. A non commutative
Bpa-algebra
is a real Banachspace equipped
with a non commutative non associative bilinearproduct
such thatThe
following concepts
are standard(see [3], [2]) :
Definition II.2. An
F-algebra
is a real non commutative unital Jordanalgebra complete
with respect to a norm such thatDefinition II.3. A non commutative unital
JB-algebra A
is anF-algebra
such that
is a Banach
algebra).
Let us recall that in a non associative unital
algebra 0,
the Jordan condition(A.B).A2 _ A.(B.A2) implies
theflexibility
and theequivalence
of the Jordan condition with either one or the other of the
following
ones :
(A2.B).A = A2.(B.A) ; A.(A2.B) - A2.(A.B) ; (B.A2).A - (B.A).A2
sothat
~ (the symmetrized algebra)
is a Jordanalgebra. Conversely,
isflexible and
~
isJordan,
then A is Jordan([11],
p.141-142).
From theseremarks it is easy to conclude that a non commutative non associative real unital
algebra A
is anF-algebra
if andonly
if it is flexible and~
is acommutative unital
JB-algebra ([2], Corollary 2.3). Similarly,
a non commu-tative non associative real Banach
algebra A
is a non commutative non asso-ciative unital
JB-algebra
if andonly
if it is flexible and~
is a commu-tative unital
JB-algebra.
The
following
lemma is then obvious thanks to([6], Corollary II.3)
aspowers coincide and
~.
Lemma II.4. The condition
IIA2+B2U
in Definitions II.2 and II.3 isequivalent
toMax(IIA112,
A non commutative unital JB-algebra
is anF-algebra
which is in turn a non commutative unitalBpa-algebra.
But
i
conversely
one has :Theorem
II.5. Let .4 be a non commutative non associative realalgebra
which is also a Banach space. Then
is a non commutative unital
Bpa-algebra
if andonly
if 011; is flexibleand
~~is
a commutative unitalBpa-algebra,
and is then anF-algebra ; 2)
The conditionIIB,12)
in Definition II.1 isequiva-
lent to
IIA2+B211
if A has aunit ;
3) Among
the non commutative unitalBpa-algebras,
the non commutative uni- talJB-algebras
are those for which IIAII IIBII and form a non trivialsubclass made of
necessarily
commutative unitalJB-algebras.
Proof. The
flexibility implies A2.A - A.A2 which, together
withA2.A2 = A2.A2 ~ A4,
isequivalent
to thepower-associativity
conditionA.A [1], ([11],
p.130).
Hence~
is a commutativeBpa-algebra,
orelse a commutative
JB-algebra by ([6],
TheoremV.1),
the conversebeeing
obvious under the
flexibility hypothesis.
is anF-algebra according
tothe remarks
following
Definition11.3,
and theequivalence
between the twometric conditions follows from
([6], Corollary 11.3)
as powers in A and~"
coincide. The same remarks
joined
to([3],
theorem7.4)
and([2], example 3.1)
assert the last claim.Hence Definition II.1 is a weakened definition of
F-algebras.
If we addthe condition
IIA.Bli 4
IIAII IIBII weget
a weakened definition of non-commuta- tive(and
hence commutativeby [3])
unitalJB-algebras.
III. THE COMPLEX NON COMMUTATIVE CASE
By
combination of thepreceeding
cases, it is then natural tobegin
with the
following
definition.Definition III.L. A non commutative
Bpa *- algebra
is acomplex
Banach space Aequipped
with a non commutative non associative bilinearproduct
suchthat
and with an involution such that
llA*O
All -llAll2
if A andA* generate
an associativesubalgebra
withI respect to the
product
o .As
above it will beinteresting
to compare this class ofalgebras
withthe next ones . ’
Definition III.2. A non associative unital
JB*-algebra
is a non commuta-tive non associative
complex
Banachalgebra A equipped
with an involutionsuch that
As indicated after Definition
1.6,
it is then a non commutativecomplex
Jordan
algebra
withmultiplicative
and isometric involution([10],
Theorem12).
Notice that the remarks
following
Definition II.3 remain valid for noncommutative
JB*-algebras (see [8], Proposition
1.2 and the fact that the involution isnecessarily multiplicative
onJB*-algebras) :
a non commuta-tive non associative
complex
Banachalgebra A
is a non commutative unitalJB*- algebra
if andonly
if it is flexible and~
is a commutative unitalJB*-algebra.
Definition III.3. A non commutative
V-algebra
is the non commutative version of the commutativeV-algebra
of Definition 1.7.According
to the different forms of the Vidav-Palmertheorem,
one hasthe
following
identifications between the above classes ofalgebras :
o (associative non commutative
C*-a1gebra) =
( associative non commutativeV-algebras) ([7],
Theorem3.1) ;
. (non associative non commutative
C*-a1gebra) =
( alternative non commuta- tiveV-algebras) =
(non commutativeV-algebras
such that))A*.A)) - IIAU2)
([10],
section2) ;
. (non commutative unital
JB*-algebras} =
( non commutativeV-algebras) ([10],
Theorem12).
’
Finally,
as in SectionII,
one can introduce the class ofF*-algebras.
Definition III.4. An
F*-algebra
is a non commutativecomplex
unital Jordanalgebra compltte
with respect to a norm andequipped
with an involutionsuch
thatWe are indebted to Professor A.
Rodriguez-Palacios
fornoticing
to usthat the condition
llA*11 -
IIAII in Alverman’soriginal
definition ofF*-
algebras
is redundantby
the sameargument
as in([5],
lemma(2.13)).
The remark
following
Definition II.3 remains valid forF*-algebras ([2],
Corollary 2.3) :
a non commutative non associativecomplex algebra A
is anF*- algebra
if andonly
if it is flexible and~
is a commutative unitalJB *- algebra
whose involution ismultiplicative
on AThe
following
lemma is then obvious.Lemma 111.5. A non commutative unital
JB *- algebra
is anF*- algebra
whichis in turn a non commutative unital
Bpa*-algebra.
But
conversely,
Theorem III.6. Let A be a non commutative non associative
complex algebra
which is a Banach space. Then
1)
~ is a non commutative unitalBpa*-algebra
if andonly
is flexi-ble and
~
is a commutative unitalBpa*-algebra
whose involution is multi-plicative
on A. Inparticular
it is anF*-algebra
if moreoverIIA,13
or IIA 0 IIAII IIBII.
2) Among
the non commutative unitalBpa *- algebras,
the Banachalgebras
arethe non commutktive unital
JB*-algebras.
Proof. The
flexibility
conditiongiving
thatUA - U+
whereU+
is definedwith respect to o, all these assertions are obvious thanks to
Corollary
1.9and the remarks
following
Definitions 111.2 and III.4.Corollary
111.7. Thefollowing
classes ofalgebras
are identical :(non commutative unital
JB * -algebras) =
(non commutative unitalBpa*-alge-
bras such that IIA.Bli IIAII
IIBII )
E (non commutativeV-algebras).
Corollary
III.S. In DefinitionIII.1,
thefollowing
subset ofhypothesis
if A and
A* generate
an associativesubalgebra
with respect to the
product
ocan be
replaced by
thefollowing
oneif there is a unit. Moreover, in the case of Banach
algebras,
the Jordan condition is redundant in the second set ofhypothesis.
Hence,
Theorem III.6provides
with a weakened definition ofF*-algebras
- *
and of non commutative unital
JB -algebras.
REFERENCES
1. A.A.
ALBERT,
On thepower-associativity
ofrings,
SummaBrasil, Math., t.2, 1948,
p. 21-32.2. K.
ALVERMANN,
Themultiplicative triangle inequality
in non commutative JB andJB*-algebras, Preprint.
3. K. ALVERMANN and G.
JANSSEN,
Real andcomplex
non commutative Jordan Banachalgebras,
Math.Z.,
t.185, 1984,
p. 105-113.4. F.F. BONSALL and J.
DUNCAN,
Numerical ranges of operators on normed spaces and of elements of normedalgebras,
London MathematicalSociety
Lectures Notes Series
2, Cambridge University Press,
1971.5. R.B.
BRAUN,
A Gelfand-Neumark theorem forC*-alternative algebra,
Math.Z.,
t.185, 1984,
p. 225-242.6. B. IOCHUM et G.
LOUPIAS, Banach-power-associative algebras
andJB-algebras,
Ann. Inst. HenriPoincaré,
t.43, 1985,
p. 211-225.7.
T.W. PALMER,
Characterization ofC*- algebras-II,
Trans. Amer. Math.Soc.,
t.148, 1970,
p. 577-588.8. R.
PAYA,
J. PEREZ and A.RODRIGUEZ,
Non commutative JordanC*-algebras,
Manuscripta Math.,
t.37, 1982,
p. 87-120.9. A.
RODRIGUEZ-PALACIOS,
A Vidav-Palmer theorem for JordanC*-algebras
and related
topics,
J. London Math.Soc.,
t.22, 1980,
p. 318-332.10. A. RODRIGUEZ
PALACIOS,
Non associative normedalgebras spanned by
hermitian
elements,
Proc. London Math.Soc.,
t.47, 1983,
p. 258-274.11. R.D.
SCHAFER,
An introduction to non associativealgebras,
AcademicPress, New-York,
1966.12. J.D.M.
WRIGHT,
JordanC*-algebras, Michigan
Math.J.,
t.24, 1977,
p.291-302.
13. M.A.
YOUGSON,
A Vidav theorem for Banach Jordanalgebras,
Math. Proc.Cam. Phil.
Soc.,
t.84, 1978,
p. 263-272.Corrigendum
o Reference r61.
Proposition
II.2. Proof : the sentence :"Conversely
ifIIAII ~ 1 ... max
(aC21, DD21)"
is useless and should bereplaced by :
is an orderunit-space
and as squares arepositive,
thenIIC2_D21 4
max(U C2g, II D2U ) .
o
R_ef_, e-ce
r61. should be read : "The class ofJB-algebras
coincides with the class of real Banach spaces with a square map
inducing
aproduct
such that ..."Bruno IOCHUM
University de provence Marseille et Centre de
Physique Théorique
CNRS, Luminy,
Case907,
13288 MARSEILLECedex
9,
FranceGuy
LOUPIASLaboratoire de
physique Mathematique
University
Montpellier
IIPlace
Eugène
Bataillon34095 MONTPELLIER Cedex