C OMPOSITIO M ATHEMATICA
M ARIO C. M ATOS L EOPOLDO N ACHBIN
Entire functions on locally convex spaces and convolution operators
Compositio Mathematica, tome 44, n
o1-3 (1981), p. 145-181
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145
ENTIRE FUNCTIONS ON LOCALLY CONVEX SPACES AND CONVOLUTION OPERATORS
Mario C. Matos and
Leopoldo
NachbinDedicated to the memory of Aldo Andreotti
© 1981 Sijthoff & Noordhoff International Publishers - Alphen aan den Rijn Printed in the Netherlands
Abstract
In this work we
generalize
the classical results onapproximation
and existence of solutions of convolution
equations
inH(Cn).
We introduce the spacesHSNb(E)
andNb(E)
of thenuclearly
Silva entire functions of bounded type and of thenuclearly
entire functions of bounded type in acomplex locally
convex space E. These spaces areendowed with natural
locally
convextopologies.
Convolution equa- tions are considered in these space and results ofapproximation
forsolutions of
homogeneous
convolutionequations
areproved
for any E. Results of existence are demonstrated for a more restrictive class oflocally
convex spaces which includes theDF-spaces.
These resultsgeneralize
theorems ofGupta
and Matos. We also introduce the spacesN(E)
of thenuclearly
entire functions andSN(E)
of thenuclearly
Silva entire functions. For these spaces we get results ofapproximation
for solutions ofhomogeneous
convolutionequations,
thus
generalizing,
theorems ofGupta-Nachbin.
1. Introduction
In this work we
generalize
the classical results onapproximation
and existence of solutions for convolution
equations
inH(Cn) (see [57]).
We introduce the spacesSNb(E)
andHNb(E)
of the Silvanuclearly
entire functions of bounded type and ofnuclearly
entire0010-437X/81 /08145-37$00.2010
functions of bounded type in a
complex locally
convex space E.These spaces are endowed with natural
locally
convextopologies.
Convolution
equations
are considered in these spaces and results ofapproximation
for solutions ofhomogeneous
convolutionequations
are
proved
for any E. Results of existence are demonstrated for a more restrictive class oflocally
convex spaces which includes theDF-spaces.
These resultsgeneralize
theorems ofGupta [48], [49]
andMatos
[51], [52].
We also introduce the spacesHN(E)
of thenuclearly
entire functions and
SN (E)
of thenuclearly
Silva entire functions.For these spaces we get results of
approximation
for solutions ofhomogeneous
convolutionequations,
thusgeneralizing
theorems ofGupta-Nachbin [50].
We remark that in the construction of the spaces7leNb(E)
and7leN(E)
a fundamental role isplayed by
the strongtopology
on the continuous dual E’ of E. Moreprecisely,
a fun-damental role is
played by
the Von Neumannbornology
of E. Acareful examination of all the results
by
the reader will convince himself that similar spaces and theorems may be obtainedby taking
any
polar topology
on E’.(More precisely, by considering
any bor-nology
inE).
It is instructive to check which kind of "nuclear" entire functions arise from the consideration of these differentpolar topologies
in E’.Several authors have been
working
withtopics closely
related tothe
subject
of this article. In thebibliography
of this work wehope
tohave listed most of the research papers connected in some way with the infinite dimensional
theory
of convolutionequations.
We ask ourexcuses to those authors whose articles we
might
have left out of thislist.
The idea of this paper is in our minds since
1970,
but from postponement to postponement we havedelayed
for along
time thewriting
of thismanuscript
with details. The motivation behind this paper leads to theSilva-Holomorphy
types(see [7]
and[56]).
2. Silva nuclear and nuclear multilinear functions and
polynomials
Let E = lim
Ei
be abornological
vector space over C. We say that aiEl
subset B of E
belongs
toÉBE
is there is i E I such that B is a closed balanced bounded subset of the normed spaceEi.
For M =1, 2, ...
we may consider the cartesian
product
Em = E ··· x E(m times)
with the natural
bornology
inducedby
thebornology
of E. In thiscase we may take the vector space
b (mE)
of all m-linearcomplex
mappings
on E m which are bounded over each element of OOEm. Inb(mE)
we consider thelocally
convextopology
of the uniformconvergence over the elements of BEm. For m = 0 we set
5tb(oE)
asthe
complex plane
with its usualtopology.
We note that E* =5tbeE).
If m E N and A E
b(mE)
we consider the function :
E ~ Cgiven by
Â(x)
=A(x, ..., x) (m times)
for every x in E(for
m = 0 this function is the constant functionÂ(x)
= A for all je EE).
The vector space of all functionsÂ,
as A varies in5tb(mE),
is denotedby Pb(mE)
and we consider on it thelocally
convextopology generated by
theseminorms
with B
varying
in9JJE.
IfXbs(mE)
denotes the vectorsubspace
ofb(mE)
formedby
allsymmetric functions,
then the naturalmapping
A H
 gives
anisomorphism
betweenXbs(mE)
andb(mE)
which is ahomeomorphism
if we consider the relativetopology
in:£bs(mE).
Ifm = 1,2, ...
and ~1,..., cpm E E* then cpl x ... x ~m denotes the ele- ment ofb(mE) given by
~1 ···’Pm(XI,..., xm)
=~1(x1)... ~m(xm).
If ~1 = ... = ~m = cp we denote such function
by ~m.
Letbf(mE)
bethe vector
subspace
ofxb(mE) generated by
all functions ~1 x ... xcpm with
~1,...,~m ~E*.
We setXbfs(mE) = Xbs(mE)
~Xbf(mE)
andXbf(OE) = Xbfs(OE) =
C. Letbf(mE)
be thecorresponding subspace
ofPb(mE)
which isisomorphic
toXbfs(mE), mEN.
It is easy to show thatPbf(mE)
is the set of elements P ofPb(mE)
which can be written in the form P = E(~j)m, ~j
E E*for j
=1,..., n.
If m =1, 2, ...
and(E*)m
j=1
denotes the
topological
cartesianproduct,
we have the continuousm -linear
mapping:
Thus there is a
unique
continuous linearmapping 03B2m
from theprojective
tensorproduct E*~03C0··· ~03C0E* (m times)
into:£b(mE)
such that am =
f3m 0
ym where ym is the natural m-linearmapping
from(E*)m
intoE*Q97T... Q97TE*.
Themapping f3m
isinjective
and itsimage
is:£bf(m E).
The nucleartopology
in:£bf(m E)
is thelocally
convex
topology generated by
all seminorms of the formwhere
~~ij~B
=sup{|~ij(x)|;
x EB}
and BG ÉBE.
The nucleartopology
inPbf(mE)
is thelocally
convextopology generated by
all seminorms ofthe form:
where B E 93,z,. It can be shown that
for all A E
.;£bfs(mE)
and B EBE.
The nucleartopology
in.;£bf(mE)
makes this space
isomorphic
andhomeomorphic
toE*~03C0··· ~03C0E*
through
themapping 03B2m.
Themapping f3m
can be extendedcontinuously
to "the"completion E*03C0 ··· 03C0E*
ofE*~03C0 ··· ~03C0E*
into
b(mE).
This extension will be denotedby m.
We know thatPm
is
injective
if andonly
if E* has theapproximation
property. Letm
be the
injective mapping
fromE*03C0··· 03C0E*/ker Pm
intob(mE).
This
mapping
is continuous and agrees withf3m
inE*Oî, ... ~03C0E*.
If we consider in
E*03C0··· 03C0E*/ker m
thequotient topology
and ifwe denote the
image
ofPm by bN(mE),
we may consider inbN(mE)
thelocally
convextopology
transferred from thequotient through Pm.
Thus
.;£bN (m E)
is "the"completion
of.;£bf(m E)
if this spaceis considered with the nuclear
topology.
We still denoteby Il ’ JINB
theseminorm in
bN(mE)
obtainedby
continuous extension of theseminorm Il - JINB
inbf(mE).
It can beproved
that theimage bN(mE)
of.;£bN (m E) through
the naturalmapping
is
isomorphic
to "the"completion
ofPbf(mE)
endowed with thenuclear
topology.
We still denoteby~· lllvb
the continuous extension tobN(mE)
of the seminorm~·~N,B
inPbf(mE).
IfbNs(mE) =
;tbN(mE)
n.;tbs(mE)
we havefor all B E
0-4E
and A E!£bNs(mE).
As usual we setBbN(0E) = bNs(0E)
= C andJIAJINB
=lAI if
A E!£bN(oE).
2.1. DEFINITION: If m E N, the elements of
bN(mE)
are calledm-linear functions of Silva-nuclear type and the elements of
bN(mE)
are called
m-homogeneous polynomials
of Silva-nuclear type.If we consider E a
locally
convex space and if wereplace
E*by
E’in the
previous
constructions we get thefollowing
spaces:(1)
The vectorsubspace f(mE)
ofbf(mE)
formedby
the con-tinuous functions and
fs(mE) _ Yf (’E)
~bs(mE).
(2)
The vectorsubspace f(mE)
ofPbf(mE)
formedby
the con-tinuous functions.
(3)
"The"completion N(mE)
off(mE)
for the nucleartopology
and
Ns(mE) = :£N(mE)
~:£bs(mE).
(4)
"The"completion N(mE)
of9’f(’E)
for the nucleartopology.
2.2. DEFINITION: The elements of
N(mE)
andrJN(mE)
are calledrespectively
m-linear functions of nuclear type andm-homogeneous polynomials
of nuclear type.2.3. DEFINITION: We denote
by bN(E)
thealgebraic
direct sum of(rJbN(mE»mEN
andby 9N(E)
thealgebraic
direct sum of(PN(mE))m~N.
The elements of
PbN(E)
andPN(E)
are calledrespectively poly-
nomials of Silva nuclear type and
polynomials
of nuclear type.Throughout
this article we consider E such that E* has the ap-proximation
property. In the end of this paper wepoint
out themodifications needed in order to prove similar results for any E.
3.
Nuclearly
entire f unctions andnuclearly
entiref unctions of bounded type
If E is a
bornological
vector spaceKe(E)
denotes thefamily
of allbalanced strict compact subsets of E
and 93É
denotes thefamily
ofelements of éBE which are convex. If E is a
locally
convex spaceK(E)
denotes thefamily
of all balanced compact subsets of E.Throughout
this paper we consider E alocally
convex space hencea
bornological
vector spacerelatively
to the Von Neumann bor-nology.
The reader will not have anydifficulty
inthinking
how thetheory
would work for ageneral bornological
vector space. For astudy
of Silvaholomorphic mappings
and Silvaholomorphic
types in this context see[56]
and[7].
We usefreely
the notations and results of[56].
3.1. DEFINITION: An element
f
ofks(E)
is called anuclearly
Silva entire function if:(1) 5’"/(0)
ErJbN(mE)
for all m E N;(2)
For every BE 00 É
and K E3t(EB)
there is E > 0 such thatHere EB denotes the vector
subspace
of Egenerated by
Bnormed
by
the Minkowskifunctional Il ·~B
associated to B. We denoteby KSN(E)
the vector space of allnuclearly
Silva entire functions in E.3.2. DEFINITION: An
element f
ofKS(E)
is called anuclearly
entire function if
f
EKSN(E) and 03B4mf(0)
EPN(mE)
for all m ~ N. We denoteby HN(E)
the vector space of allnuclearly
entire functions in E.3.3. PROPOSITION:
If
Pm EPbN(mE) (respectively,
Pm EPN(mE)) for
m E N, thenf or
every B ~ B c thefollowing
conditions areequivalent :
(1)
For each K EK(EB)
there is E > 0 such that(2)
For each K EK(EB)
and each p > 0 there is 5 > 0 such thatPROOF: It is obvious that
(2) implies (1).
Now we prove that(1) implies (2).
Let K E3t(EB)
and p > 0 begiven.
If À > 0 then there isE > 0 such that
We
applied (1) to ÀpK
EK(EB).
Thusand
Hence, if we take À > 1, we have
3.4. DEFINITION: An element
f
ofXs(E)
is called anuclearly
Silvaentire function of bounded type if:
(i) f(0), belongs
to9PbN(mE)
for all m E N;(ii)
For each Bin ôA É, ~1 m!(0)~ 1/mN,B=0.
We denoteby
YsNb(E)
the vector space of allnuclearly
Silva entire functions of bounded type in E.3.5. DEFINITION: An element
f
EHSNb(E)
is called anuclearly
entire function of bounded type if
f(0) belongs
to9PN(mE)
for allm E N. We denote
by ;¡(Nb(E)
the vector space of allnuclearly
entirefunctions of bounded type in E.
3.6. REMARK: When E is a Banach space the spaces
HSN(E)
andHN(E)
coincide with the spaceHN(E)
introduced inGupta-Nachbin [50].
Also the spacesHSNb(E)
andXNb(E)
coincide with the spaceNb(E)
introduced inGupta [48].
The spaceHNb(E)
is the same spaceHNb(E)
which appears in Matos[51]
and[52].
In[48] Gupta gives
anexample
of a Banach space E such thatXNb(E) CYN(E).
In the definitions of
HSN(E), HN(E), HSNb(E)
andYeNb(E)
theorigin plays
a veryspecial
role. We show that this fact can be avoided asfollows.
3.7. PROPOSITION: An element
f of Xs(E)
isnuclearly
Silva entire(respectively, nuclearly entire) if
andonly if
(i) 5mf(x)
E9PbN(mE) (respectively, 8mf (x)
E9PN(mE» for
all x in Eand m E N.
(ii)
For eachB E 00 É
and everyK, J ~ J(EB)
there is ~ > 0 such thatPROOF: It is clear that
(i)
and(ii) imply f E HSN(E) (respectively, f
EHN(E)).
We prove the reverseimplication.
Let BEE ô-4É
andK,
J E
3t(EB).
Let 8 > 0 be such thatIf we take ~ =
1 203B4
we have:where the last
inequality
follows from Lemma 3.8 with r = s =1 2.
3.8. LEMMA:
If f
EHSN(E) (respectively, f
EHN(E))
thenmf(x)
EPbN(mE) (respectively, mf(x)
EPN(mE)) for
each x E E and m E N.Furthermore :
PROOF: We know that the
following equalities
holdpointwise
in E:where
Pm+k
=ym
+k)!]-1 m+kf(0).
Let B ~ BcE and x E EB. Thus for each p > 0, p
1 2
there is 03B4 > 0 such thatHere
{}
denotes the closed convex balanced hull of{x}.
The in-equality
above and Lemma 3.9imply
By
Lemma 3.9 andby
the fact that BC= -04 c
isarbitrary
we concludethat {03A3Nk=0 mPm+k(x)}~N=0
is aCauchy
sequence inPbN(mE) (respectively, ,PN(’E».
Hence its limitmf(x)~PbN(mE) (respectively, Smf (x) E
PN(mE)).
N ow for r,s E[0, 1),
r + s ~1,
we have:3.9. LEMMA: For every x E E and
k E N,
k ~ m, the linearmapping
P E
PbN(mE) ~ kP(x)
EPbN(kE) (respectively,
P EPN(mE) ~
kP(x)
EPN(kE))
is continuous andfor
all BC= 1-54É
with x E EBPROOF: For P E
Pbf(mE) (respectively,
P EPf(mE))
with P =03A3nj=1 cpj, 8j
E E*(respectively,
EE’), j
= 1,..., n, we have(respectively, kP(x)
EPf(kE)).
Hence for each B~ BcE
with x E EBit follows that
Therefore
The result follows from the
density
ofPbf(mE)
inPbN(mE) (respectively,
of0-Pf(mE)
inON(mE)).
3.10. PROPOSITION: Let
f
E7les(E).
Thenf
E7leSNb(E) (respectively, f
EHNb(E)) if
andonly if
(i) mf(x) ~ PbN(mE) (respectively, smf (x)
EPN(mE)) for
all x E Eand m E N.
(ii)
For each B EBcE
and x EEB
PROOF: It is clear that
(i)
and(ii) imply f
EHSNb(E) (respectively, f
E7leNb(E».
Now we prove the converse. Iff
E7leSNb(E) (respec- tively, f
E7leNb(E»,
for each B E OA É and each x E EB we chooseE > 0 such that
~ ~x~B ~
1. Thus there is C > 0 such thatfor all m G N.
By
Lemma 3.8 and the the fact thatWsNb (E)
CYSN (E) (respectively, YNb (E)
CZN (E»
we get1 m!mf(x) ~ PbN(mE) (respectively, 1 m!mf(x) ~ PN(mE)).
If we use Lemma 3.9 we maywrite
Hence
As E goes to 0 we get
3.11. PROPOSITION: Let
f
be inXs(E).
Thenf
EHSNb(E) (respec- tively, f
ENb(E)) if
andonly if mf(0) ~ PbN(mE) (respectively,
mf(0) ~ PN(mE)) for
each m E N andfor each
B ~ BcE.PROOF: We observe that
implies
thatfor all p E R, p > 0. Hence this holds for p = 1. Thus we have
proved
that
f
EHsNb(E) (respectively, f
EHNb(E)) implies
condition(*)
andmf(0) E 1PbN(mE) (respectively, mf(0)
EPN(mE))
for all m E N . In order to prove the converse we observe thatfor all p > 0 and B E
BcE.
Hencefor all p > 0 and B
E 9JJ É.
It follows thatfor each B E
00 E.
4.
Topologies
inHSNb(E)
and inHN(E)
4.1. DEFINITION: The natural
topology
inWSNB(E) (respectively, HNb(E))
is thelocally
convextopology generated by
the seminormsfor B E
BcE, f
EHSNb(E) (respectively, f
EHNb(E)).
4.2. PROPOSITION: The spaces
HSNb(E)
andHNb(E)
arecomplete
under their natural
topologies.
PROOF: We prove the result for
HSNb(E).
Theproof
forHNb(E)
issimilar. Let
(fa)aEA
be aCauchy
net inHSNb(E)
for the naturaltopology.
Hence for eachE > 0, B ~ BcE,
there is03B1~ ~ A
such that~f03B1-f03B2~N,B
E for a ~ 03B1~ and(3
~ aE. Hence for each m ~ N we have1 m!~mf03B1(0)-mf03B2(0)~N,B~
for 03B1~03B1~ and03B2~03B1~.
Thus(mf03B1(0))03B1~A
is a
Cauchy
net inpbN(mE),
which iscomplete.
Therefore we have Pm EPbN(mE)
suchthat 1 m! ~mf03B1(0) - Pm~N,B ~
E for 03B1 ~ a.. Inparti- cular,
if wecall f k
=f03B1(1/k),
we havefor all k ~ N -
{0},
andif e 2: k and we take
03B11 ~ ~ 03B11 k
for t - k(this
ispossible by induction).
H ence there is M ~ 0 such
that 1 m! ~mfk(0)~N,B ~
M f or all k ~ N -{0}.
Now we may write for all m ~ N and kEN -
101
Therefore
It follows that
for all B
E -0-e É.
Hence if BE 00 É
and 8 > 1and
for all B ~ BcE.
Now,
from~f03B1-f03B2~N,B
E for 03B1 ~ (Xe,j3
~ 03B1~ we getfor 03B1 ~ ci,. If we prove that
defines an element of
ks(E),
we get thatf
EWSNB(E)
andlim fa
=f
aEA
for the natural
topology
ofHSNb(E).
First we prove thatf
isfinitely holomorphic
in E. If x EE,
let Bx be the closedabsolutely
convexhull of
{x}.
Hence Bx E BcE andNow, in order to prove that
f~HS(U),
we must show thatf
isbounded over each K E
3t(EB),
as B variesover 00 É.
Let BK be the closedabsolutely
convex hull of K. ThusBK E BcE,
and4.3. COROLLARY:
If
E has a countablefundamental
systemof
bounded
subsets,
thenHSNb(E)
andHNb(E)
are Fréchet spaces under their naturaltopologies.
4.4. PROPOSITION:
If f
EHSNb(E) (respectively, f
EHNb(E))
itsTay-
lor series at 0 converges to
f for
the naturaltopology.
PROOF: It is immediate from the
following
fact which holds for all B E 9JJEas n ~ ~.
4.5. PROPOSITION: The vector
subspace 9 of HSNb(E) (respectively, HNb(E)) generated by {e~;
cp EE*l (respectively, {e~;
cp EE’l)
is densein
7leSNb(E) (respectively,
inHNb(E)) for
the naturaltopology.
PROOF: We prove the result for
HSNb(E).
Theproof
forHNb(E)
issimilar.
By Proposition
4.4. it isenough
to show that Pcz 9
for all P EPbN(mE), m ~ N .
Since the naturaltopology
ofHSNb(E)
inducesin each
PbN(mE)
the nucleartopology
it isenough
to prove that PE 9
for all P ePbf(mE), m ~ N.
We havefor every cp E E* and À E C in the sense of the natural
topology
ofHsNb(E).
Thus for each BE 00 É
ad
[03BB| ~ 0 for_all ~ ~ E*.
Hence~ ~ ~
for all~ ~ E*.
Now wesuppose that
W’ E Y
for i =1, 2,..., n - 1
and cp E E*. Thenas M |~0
for each cp E E* and B EBcE, Hence, by induction,
we haveproved
thatebf ("E) ~ ~
for n E N.4.6. REMARK:
kNb(E)
is "the"completion
of its vectorsubspace generated by
the continuous functions.5.
Topologies
inHSN(E)
and inN(E)
5.1. DEFINITION: Let
B ~BcE
and K EX(EB).
A seminorm p inYSN(E) (respectively,
inHN(E))
is said to beN-ported by (K, B)
if for each E > 0 there isC(e)
> 0 such thatfor all
f
EHSN(E) (respectively, f
EHN(E)).
The naturaltopology
inHSN(E) (respectively,
inHN(E))
is thelocally
convextopology
generated by
all seminorms which areN-ported by (K, B),
where B E 1-5-A É and K E7«EB)
5.2. PROPOSITION: For each
f OE WSN (E) (respectively, f
EHN(E))
its
Taylor
series at 0 coverges tof
in the naturaltopology.
PROOF: We prove the result
for f
EHSN(E).
Iff
EHN(E)
theproof
is similar. Let p be a seminorm in
HSN(E) N-ported by (K, B).
SinceB E BcE and K E
K(EB)
we know that there is E > 0 such thatHence there is
C(e)
> 0 such thatfor all g E
HSN(E).
Henceana inis tencis to u as n renas to +~.
5.3. PROPOSITION: The vector
subspace of HSN(E) (respectively, HN(E)) generated by {e~;~
EE*} (respectively, {e~;
cp EE’})
is dense inHSN(E) (respectively, N(E)) for
the naturaltopology.
PROOF: It follows the pattern of the
proof
ofProposition
5.4.5.4. REMARK: For more information about the
topology
of the spaceHSN(E)
see Bianchini[7].
6. Translations and directional derivatives
6.1. DEFINITION: If
f
is acomplex
function defined in E anda E E, we define the translation
03C403B1f
off by
a in thefollowing
way:6.2. PROPOSITION: Let a E E and
f
EHSNb(E) (respectively, f
E;JeNb(E)).
Then:(i) nf(·)
EHSNb(E) (respectively, nf(· )a
EHNb(E))
andin the sense
of
the naturaltopology of
the space,for
all n E N.(ii) 03C4af
EHSNb(E) (respectively, T0.f
EeNb(E»
andin the sense
of
the naturaltopology of
the space.PROOF: We prove the results
for f
E7JeSNb(E).
Theproof
forf
ENb(E)
is similar.(i) By Proposition
3.36 of Matos-Nachbin [56] we havefor each x E E, the series
converging
in the naturaltopology
ofPb(iE).
Hencefor every x E E. It is easy to see
that 03B4i+n(0)ai~PbN(nE) and,
forevery B ~ BcE with a E EB, we have:
Hence
for every i E N. Thus
if(· )a
EHSNb(E)
for each i EN. We have:as k ~ ~,
for all B E BcE with a E EB.(ii)
We considerNow
given ~>0,
withellailB 1,
E1,
there isc(E)
> 0 such that[(i
+n)!]-1~i+n(0)~N,2B
~c(e)ei+n
for all i EN. Thereforewhich tends to 0 as k ~ ~
6.3. PROPOSITION: Let a ~ E and
f OE 2tsN (E) (respectively, f
EHN(E)).
Then :(i) nf(·)a
eHSN(E) (respectively, nf(· )a
EHN(E))
andin the sense
of
the naturaltopology, for
all n E N.fin
in the sense
of
the naturaltopology.
PROOF: We prove the results for
f ~HSN(E).
Theproof
forf ~ XN(E)
is similar.(i)
Iff
EHSN(E)
then5"/(.)a
EHS(E)
for every a E E.(See
Matos-Nachbin[56]).
Let B~ BcE
with a EEB
and K E3t(EB).
Thusthere is E > 0 such that
We have
We note that
where
a(a)
> 0 is such that[a(a)]-la
e K + eB. HenceHence nf(· )a
ESN(E)
for all n E N. Sinceis the
Taylor
seriesof nf(· )a
at 0, the result follows from 5.2.(ii)
Let p be a continuous seminorm inHSN(E) N-ported by (K, B)
with B EBcE,
K EK(EB),
a E EB. Let KI be the balanced hull of K U{a}.
Hence Kt E71(EB)-
If p > 2 isgiven
there is E > 0 such that(See
3.3 part(2)).
Thus there is c > 0 such thatfor all n E N. We also find
c(e)
> 0 such thatfor all g E
KSN(E).
NowWe note that as in part
(i)
there is03B1(a) > 0
such that a Ea(a)[Ki + eB].
In this case we may takea (a)
= 1 since a E Kt.7. Convolution operators and convolution
products
From now on every time we write
2tsNb(E), 2tNb(E), 2tsN(E)
andKN(E)
we consider these spaces endowed with their naturaltopolo- gies.
7.1. DEFINITION: A
mapping O:HSNb(E)~HSNb(E) (respectively,
O:hNb(E)~HNb(E), O:HSN(E), O:HSN(E)~HN(E))
iscalled a convolution operator in
HSNb(E) (respectively, HNb(E), HSN(E), HN(E))
if it is linear continuous and translation invariant(1,e., O 03BF
Ta =’Ta 0 (J
for all a EE).
The vector space of all such convolution operators is denotedby ASNB (respectively,
ANb,ASN, AN).
It isobviously
analgebra
withunity
undercomposition
ofmappings
asmultiplication.
7.2. DEFINITION: If
T ~H’SNb(E) (respectively, H’Nb(E), H’SN(E), H’N(E))
andf
EHSNb(E) (respectively, HNb(E), HSN(E), HN(E))
we define the functionand we call T
* f
the convolutionproduct
of T andf.
7.3. PROPOSITION: If
T ~ H’SNb(E) (respectively, H’Nb(E))
thenT *
f
EHSNb(E) (respectively, HNb(E)) for
allf
EHSNb(E) (respec- tively, HNb(E)).
Moreover T* == C E ASNB(respectively, ANb)·
We need a lemma for the
proof
of thisproposition.
7.4. LEMMA: Let T E
H’SNb(E) (respectively,
T EH’Nb(E))
so that there is B~ BcE
and C > 0 suchthat |T(f)| ~ C~f~N,B for
everyf
EHSNb(E) (respectively, f E HNb(E)).
Thenfor
each P EPbN(nE) (respectively, PN(nE))
with A in5tbNs(nE) (respectively, 5tNs(nE»
suchthat P = Â,
thepolynomial
y E E -T(A. k y n-k )
E C denotedby T(A . is in 9PbN(n-kE) (respectively, PN(n-kE)) for
every k ~ n. Fur- ther~T~N,B ~ C~P~N,B
PROOF: We suppose first that P E
Pbf(nE)
and A E5tbfs (nE)
withÂ
=P. If P =
03A3mj=1 ~ with ~i
E E*for j
=1,...,
m, we haveT(A. k)(y) =
T(A. ·kyn-k)=03A3mj=1 T[~j(y)]n-k
for every y EE,
so thatWe also have
Thus
This
gives
that~T~N,B ~ C~P~N,B
for everyP ~Pbf(nE)
andk S n. The result for
arbitrary
P EPbN(nE)
follows from thedensity
of
Pbf(nE)
inPbN(nE).
The result for the other case has a similar Proof.PROOF oF 7.3:
By
6.2 we have:Now
by
Lemma7.4, T(03B4i+nf(0)· i) E 9JbN(nE)
for every n and~T(03B4i+nf(0)· i)~N,B ~ C~i+nf(0)~N,B
where B ~ B É and C > 0 are such that|T(f)| ~ C~f~N,B
for allf
in(KSNb(E).
Thus for each p > 1 we haveHence the series
L 7f T(f(0)· ’)
converges inPbN(nE)
to an ele-ment Pm E
PbN(nE). (The
aboveinequality
holds for B’replacing
B ifB’ D B, B’ E
BcE).
Also for all p >1,
and B’~BcE,
B’ DB,
This
implies
for all p > 1 and B’ ~ BcE, B’ ~ B. Hence
f or all
B’~BcE
andT * f = i 1, Pn
EHSNb(E).
In order to prove that the
mapping
is
continuous, given
BI E BcE we have from(1)
for all p > 1. Hence
It is very easy to show that T * E ASNb. The
proof
for the other resultis similar.
7.5. PROPOSITION:
If T E (lfsN(E) (respectively, H’N(E))
thenT
* f
EHSN(E) (respectively, HN(E)) for ail f E HSN(E) (respectively, HN(E)).
Moreover (J = T * ~ ASN(respectively, AN).
PROOF: T E
H’SN(E) implies
that there are B E BcE and K EK(EB)
such that for each e > 0 we find
C(e)
> 0satisfying
for all
/ E 2tsN (E).
We fix
f
EHSN (E).
Let D E 00 É and J EK(ED)
begiven.
Let p > 2 be considered.By Proposition 3.3,
there are C > 0, 5 > 0 such thatfor all n E N, where
0393(D
UB)
is the closed bounded balanced convexhull of D U B. We note that
(*)
holds for Kreplaced by
K U J and Breplaced by 0393(D
UB).
Fromprevious
results we know thatWe have
0393(03B4n+mf(0) · m)
EPbN(nE)
for all n E N and(The proof
goes like theanalogous
result of7.4).
HenceHence T *
f
EWSN (E).
It is easy to see that T * is linear and translation invariant in
HSN(E).
In order to show that T * is continuous we consider aseminorm q in
HSN(E) N-ported by (J, D)
with D ~ BcE and J ~K(ED).
Hence for each e > 0 there isd(e)
> 0 such thatfor all g E
7JesN(E).
We want to show that p = q 0 T * is a continuous seminorm inHSN(E).
We have:for all E > 0 and
f
EHSN(E).
It follows that q - T * is a seminorm in7lfSN (E) N-ported by (2(J U K), 0393(D ~ B)).
Theproof
for the otherpart is similar.
7.6. DEFINITION: The
mapping
ysNb is definedby
where
(03B3SNbO)(f) = (Of) (0)
for allf
E7leSNb(E).
We definesimilarly
themappings
7.7. PROPOSITION: The
mappings
ysNb, 03B3Nb, 03B3SN and yN are linearbijections.
PROOF: We
just
show that ysNb is a linearbijection.
Theproof
for the other cases are similar. We consider the
mapping ySNb H’SNb(E) ~ ASNb
definedby ysNb (T )
= T * for all T EH’SNb(E).
We have
Hence
ysNb
° ’YSNb =identity
inASNb.
Also for every T EH’SNb(E)
andf
EHSNb(E)
we haveHence ysNb
° ysNb
=identity
inH’SNb(E)·
7.8. DEFINITION: For
Ti
EHSNb(E) (respectively, H’Nb(E), H’SN(E), H’N(E)), fi;
=Ti
*, i =1,
2 we defineTl *
T2=YSNb(01 - (J2) (respec- tively, Tl
*T2
=03B3Nb(O1 03BF O2), Ti
*T2 = 03B3SN(O1 03BF (J2), T1
*T2
=03B3N(O1 ° O2))
which is an element ofH’SNb(E) (respectively, H’Nb(E), Y’sN(E), H’N(E)).
We say thatTl
*T2
is the convolutionproduct
orsimply
the convolution ofT and T2.
7.9. REMARK: We note that
(Tl
*T2) * f
=Tl * (T2 * f )
ifTi, T2
EY’sNb(E) (respectively, H’Nb(E), H’SN(E), H’N(E))
andf e HSNb(E) (respectively, HNb(E), HSN(E), HN(E)).
We also note that the map-pings
ysNb, yNb, yN, ysN preserve convolutionproducts.
In all spaces considered the convolutionproduct
is associative and have aunity
8defined
by 03B4(f)=f(0).
HenceH’SNb(E), H’Nb(E), H’SN(E)
andH’N(E)
are
algebras
withunity
under the usual vector spacesoperations
andthe convolution
product
asmultiplication. They
are called con-volution
algebras.
8. The Borel transformations
8.1. DEFINITION: The Borel transformation
T
of T EH’SNb(E) (respectively, W%N(E))
is definedby
The Borel
transformation S
of S E¡¡(Nb(E) (respectively, ¡¡(ME»
isgiven by
We shall use later the
following
result8.2. PROPOSITION:
(1)
Themapping 03B2b : P’bN(nE)
HP(nE*) defined by [03B2b(T)](~)
=T() for
every cp E E* and T EP’bN(nE)
establishesan
isomorphism
between the two spaces such thatf or
each B EBE,
T
~ P’bN(nE).
(2)
Themapping (3 : P’N(nE) ~ (PnE’) defined by [(3(T)] (cp)
=T(cpn) for
all cp E E’ and T EP’N(nE)
establishes anisomorphism
between the spaces such thatfor
every B~ BE,
T EP’N(nE),
Here
PROOF: We prove part
(1).
Theproof
of part(2)
is similar. It is clear that03B2b
islinear
and well-defined. For each cp E E* we have|[03B2b(T)](~)| = |T()|~~T~N,B~~~nB. (Here IITIJNB
may be +~ and weknow that for each T E
P’bn(nE)
there is a B E0-eE
which makesHence
|T(P)|~~03B2b(T)~B2022~P~N,B
and~03B2b(T)~B2022~ ~T~N,B.
Thus for everyT
~ P’bN(nE)
and B EBE~T~N,B
=~03B2b(T)~B2022(Here
when one of the sides is finite the other is alsofinite).
Hence13
isinjective. Now,
forP’ E
P(nE*)
definewhere P
== 2: cp E Pbf(nE).
We havewith
IIP’IIB8
+~ for some B E’,JCE. Hence |Tp’(P)| ~ ~P’~B2022~P~N,B
forall P E
Pbf(nE).
ThusTp,
is linear and continuous for the nucleartopology
inrlbf(nE).
SincePbf(nE)
is dense inPbN(nE)
we can extendTp, continuously
torlbN(nE).
We also haveTP,(cpn) = P’(~)
for all~ ~ E*. Thus
(3b(Tp’)
= P’and (3b
issurjective.
8.3. DEFINITION: An entire function
f
EH(E*)
is said to be ofexponential-type
on E* if there are B ~ BcE and C > 0 suchthat |f(~)| ~ Ce~~~B
for all cp E E*. We denoteby Exp E*,
thealgebra,
under usual vector-space
operations
andpointwise multiplication,
ofentire functions of
exponential
type on E*. Similar definition forExp
E’.8.4. PROPOSITION:
(1)
For each T EHSNb(E)
the Boreltransfor-
mation
1
EExp
E* and themapping
T EH’SNb(E) ~ ~ Exp
E* isan
algebra isomorphism
between the two spaces.(2)
For every T EH’Nb(E),
we haveE Exp
E’ and themapping
T E
H’Nb(E) ~ T
EExp
E’ is analgebra isomorphism
between the two spaces.PROOF: We prove part
(1).
Theproof
of part(2)
is similar. Since for eachcp E E*
we havee~=1 n! n
in the sense of’i1eSNb(E),
wecan write
(~) = 2: 1 n!T
As we knowPbN(nE)
is closed sub- space ofHSNb(E).
We set Tn = T|PbN(nE)
eP’bN(E). By Proposition 8.2,
there is aunique P’n~P(nE*)
such thatTn() = P’n(~)
for allcp E E* and
~Tn~N,B
=~P’n~B2022
for all n ~ N and an B~ BcE.
Since T is continuous inHSNb(E)
there is D E BcE and C > 0 suchthat |T(f)| ~ CllflIN,D
for ailf
EHSNb(E)·
Thisgives IITnIIN,D
=~P’n~D2022~
C andHence
defines an entire function of
exponential
type on E*. Thus T EH’SNb(E)
~~ Exp D*
is a well defined linearmapping
and it isinjective by Proposition
4.5.If,
now, H= 1 n! P’n~Exp E*,
thenthere is
D ~BcE
such thatn DO
is a bounded sequence. Hence thereare C > 0 and p > 0 such that
JIP ’n~D2022 ~ CP n
for all n E N.By 8.2,
there is aunique Hn
EP’bN(nE )
such thatHn() = P’n(~)
f or all ~ E E * andIIHnIIN,D
=~P’n~D2022.
For everyf
EYSNb(E), f = 03A3~n=0
Pn we setT(f)
=03A3~n=0 Hn (Pn).
NowThus T E
7leSNb(E)
andfor all ~ E E*. Thus
T
= H and the Borel transformation T EH’SNb(E)
HT
EExp
E* issurjective. Now, using
the fact that T * e~ =e~T(e~)
for all T EH’SNb(E)
and ~ E E* we proveeasily
thatT1
* T2 =Tl . T2
for allTi, T2
EH’SNb(E)·
8.5. DEFINITION: A
function f
EX(E*) (respectively, Ye(E’»
issaid to be of compact
exponential
type if there areB ~ BcE, K
EK(EB)
such that for every e > 0 there isc(E)
> 0satisfying
for all cp E E*