On
the
Structure
of Hyperfunctions and
Ultradistributions
By
Takashi
TAKIGUCHI*
Abstract
In this article, we study global representation of ultradistributions and hyperfunctions.
For non-quasi-analytic ultradistributions, we need to assumesuitable global growthconditions
for the global representation to hold. On the other hand, it holds for any quasi-analytic
ultradistributionand hyperfunction.
\S 1.
IntroductionIn thispaper,
we
discuss thestructure of generalized functions. It is wellknown thatany distribution $f$ is locally represented as $f=P(D)g$, where $P(D)$ is a finite order differential operator with constant coefficients and $g$ is
a
continuous function, which isthe structure theorem for distributions. The structure theorems for
non
quasi-analyticultradistributions
([1], [6]), quasi-analytic ultradistributions ([10], [11]) andhyperfunc-tions ([3])
are
als$0$ known, among which, it is only the structure of hyperfunctions thatis proved to hold globally. In this paper, we shall give global structure theorem of
dis-tributions and
non
quasi-analytic ultradistributions, by assuming suitable global decayconditions. The main purpose of this article is to give the global structure theorem for
all quasi-analytic ultradistributions.
\S 2.
UltradistributionsIn this section,
we
review thedefinitionofultradistributions. Let $\Omega\subset \mathbb{R}^{n}$ bean
opensubset and $M_{p},$ $p=0,1,$$\ldots$ , be
a
sequence ofpositive numbers. For non-quasi-analyticclasses,
we
impose the following conditions on $M_{p}.$2010 MathematicsSubject Classffication(s): Primary $46F15$; Secondary $46F20.$
Key Words: global representationof hyperfunctions, structureof hyperfunctions.
Partiallysupported by JSPS Grant-in-Aidfor ScientificResearch (C) 22540214.
*Department ofMathematics,National DefenseAcademy of Japan, 1-10-20, Hashirimizu, Yokosuka,
$(M.0)$ (normalization)
$M_{0}=M_{1}=1.$
($M$.1) (logarithmic convexity)
$M_{p}^{2}\leq M_{p-1}M_{p+1}(p=1,2, \ldots)$
.
($M$.2) (stability under ultradifferential operators)there exist $G,$ $H>0$ such that $M_{p} \leq GH^{p}\min_{0\leq q\leq p}M_{q}M_{p-q}(p=1,2, \ldots)$.
($M$.3) (strong
non
quasi-analyticity)there exists $G>0$ such that $\sum_{q=p+}^{\infty}\frac{M_{q-1}}{1^{M_{q}}}\leq Gp\frac{M_{p}}{M_{p+1}}(p=1,2, \ldots)$
.
($M$.2) and ($M$.3)
are
often replaced bythe following weaker conditions respectively;$(M.2)’$ (stability under differential operators)
there exist $G,$ $H>0$ such that $M_{p+1}\leq GH^{p}M_{p}(p=0,1, \cdots)$
.
$(M.3)’$ (non-quasi-analyticity)
$\sum_{p=1}^{\infty}\frac{M_{p-1}}{M_{p}}<\infty.$
For two sequences $M_{p}$ and $N_{p}$ of positive numbers
we
define their orders.Definition 2.1. Let $M_{p}$ and $N_{p}$ be the sequences of positive numbers.
(i) $M_{p}\subset N_{p}$ if there exist constants $L>0$ and $C>0$ such that $M_{p}\leq CL^{p}N_{p}$ for
any $p.$
(ii) $M_{p}\prec N_{p}$ if for any $L>0$ there exists
a
constant $C>0$ such that $M_{p}\leq CL^{p}N_{p}$ for any$p.$In order to define quasi-analytic classes,
we
impose the following conditions, $(QA)$and $(NA)$, instead of ($M$.3)
or
$(M.3)’.$$(QA)$ (quasi-analyticity)
$p! \subset M_{p}, \sum_{p=1}^{\infty}\frac{M_{p-1}}{M_{p}}=\infty.$
Let $M_{p}$ be
a
sequence ofpositive numbers satisfying $(QA)$.
If$\lim_{parrow}\inf_{\infty}\sqrt[p]{\frac{p!}{M_{p}}}>0$
then$\mathcal{E}^{\{M_{p}\}}$
is theclass ofanalyticfunctions. We impose the condition that $\{M_{p}\}$ would
not define the analytic class, namely,
$(NA)$ (non-analyticity)
Definition 2.2. Let $M_{p}$ be
a
sequence ofpositive numbers and $\Omega\subset \mathbb{R}^{n}$ bean
opensubset. $A$ function $f\in \mathcal{E}(\Omega)=C^{\infty}(\Omega)$ is called an
ultradifferentiable function
of theclass $(M_{p})$ (resp. $\{M_{p}\}$) if and only iffor any compact subset $K\subset\Omega$ and for any $h>0$
there exists a constant $C$ (resp. for any compact subset $K\subset\Omega$ there exist constants $h$
and $C)$ such that
(2.1) $\sup_{x\in K}|D^{\alpha}\varphi(x)|\leq Ch^{|\alpha|}M_{|\alpha|}$ for all $\alpha$
holds. Denote the set ofthe ultradifferentiable functions of the class $(M_{p})$ (resp. $\{M_{p}\}$) on $\Omega$ by $\mathcal{E}^{(M_{p})}(\Omega)$ (resp. $\mathcal{E}^{\{M_{p}\}}(\Omega)$) and denote by
$\mathcal{D}^{*}(\Omega)$ the set of all functions in $\mathcal{E}^{*}(\Omega)$ with their supports compact in $\Omega,$ where $*=(M_{p})$ or
$\{M_{p}\}.$ Let $K\subset \mathbb{R}^{n}$ be
a
compact set, andassume
that$M_{p}$ satisfy ($M$.1) and $(NA)$. Denote
by $\mathcal{E}^{*}[K]$ the set of the ultradifferentiable functions of the class
$*=(M_{p})$ or $\{M_{p}\}$
defined on
some
neighborhood of $K$. We define $\varphi\in \mathcal{E}^{\{M_{p}\},h}[K]$ by $\varphi\in \mathcal{E}^{\{M_{p}\}}[K]$ and(2.1) holds for given $h>0.$
For $M_{p}$ satisfying ($M$
.3)’
anda
compact subset $K\subset\Omega$, set(2.2) $\mathcal{D}_{K}^{*}=\{\varphi\in \mathcal{D}^{*}(\mathbb{R}^{n});suppf\subset K\},$
where $*=(M_{p})$ or $\{M_{p}\}$ and we define
(2.3) $\mathcal{D}_{K}^{\{M_{p}\},h}=\bigcup_{C>0}\{\varphi\in \mathcal{D}_{K}^{\{M_{p}\}};\sup_{x\in K}|D^{\alpha}\varphi(x)|\leq Ch^{|\alpha|}M_{|\alpha|}\}.$
Let $M_{p}$ satisfy ($M$.1) and ($M$.3)’. We define $\mathcal{D}^{*}/(\Omega)$ as the strong dual of$\mathcal{D}^{*}(\Omega)$ for any
open set $\Omega$ and call it the set
of
ultradistributionsof
the class $*$ defined on $\Omega$.
Thesespaces are endowed with natural structure of locally
convex
spaces.For
non
quasi-analytic ultradifferentiable functions andnon
quasi-analyticultradis-tributions confer [6] and [7].
Definition 2.3. Let $K\subset \mathbb{R}^{n}$ be a compact set,
$M_{p}$ satisfy ($M$.1) and $(NA)$. For
$f\in \mathcal{E}^{\{M_{p}\},h}[K]$ we define its
norm
by(2.4) $\Vert f\Vert_{\mathcal{E}^{\{M_{p}\},h}[K]}:=\sup_{x\in K,\alpha}\frac{|D^{\alpha}f(x)|}{h|\alpha|M_{|\alpha|}}.$
Let $\Omega$ be an open set and $K$ be a compact set. Topologies ofthe
spaces of
ultradiffer-entiable functions
are
definedas
follows.(2.5) $\mathcal{E}^{\{M_{p}\}}[K]= \lim_{arrow,harrow\infty}\mathcal{E}^{\{M_{p}\},h}[K],$
$\mathcal{E}^{(M_{p})}[K]= \lim_{arrow,harrow 0}\mathcal{E}^{\{M_{p}\},h}[K],$
$\mathcal{E}^{(M_{p})}(\Omega)=i\llcorner m\mathcal{E}^{(M_{p})}[K]K\Subset\Omega^{\cdot}$
We define $\mathcal{E}_{K}^{*J}$
as
the strong dual of $\mathcal{E}^{*}[K]$ and call it the setof
ultmdistributionsof
theclass $*$ supported by $K$. We also
define
$\mathcal{E}^{*}/(\Omega)$$:= \bigcup_{K\subset\Omega}\mathcal{E}_{K}^{*}\prime.$
Let
us
define the sheaf of ultradistributions.Definition 2.4. Let
a
sequence$M_{p}$of positive numbers satisfy ($M$.0), ($M$.
1), $(M.2)’$and
(2.6) $\lim_{parrow}\sup_{\infty}\sqrt[p]{\frac{p!}{M_{p}}}<\infty.$
For
an
open bounded set $\Omega$, we define(2.7) $Db^{*}(\Omega):=\mathcal{E}^{*}/(\mathbb{R}^{n})/\mathcal{E}^{*}/(\mathbb{R}^{n}\backslash \Omega)$,
where $*=(M_{p})$
or
$\{M_{p}\}$.
We abuse the notation and by $Db^{*}$we
define the presheafinduced by (2.7). We denote the associated sheaf by $\mathcal{D}b^{*}$ If
$M_{p}$ satisfies $(M.3)’$ then $\mathcal{D}b^{*}=\mathcal{D}^{*J}$ If
$M_{p}$ satisfies $(QA)$ and $(NA)$, then we call $\mathcal{D}b^{*}$ the
sheaf
of
thequasi-analytic ultradistributions
of
class $*.$The ultradistributions are represented as the boundary values of holomorphic
func-tions (cf. [6], [8]).
Definition 2.5. For
a
positive sequence $M_{p}$ satisfying $(NA)$, define its associatedfunctions
by(2.8) $M(t) := \sup_{p}\frac{t^{p}}{M_{p}}, M^{*}(t) :=\sup_{k}\frac{t^{k}k!}{M_{k}},$
for $t>0.$
Proposition 2.6. Let $\Omega$ be an open set in $\mathbb{R}^{n}$ and
$\Gamma_{j}(j=1, \ldots, N)$ open
cones
in$\mathbb{R}^{n}$ The following two conditions
are
equivalent.(i) $f(x)\in \mathcal{D}b^{(M_{p})}$ (resp. $\mathcal{D}b^{\{M_{p}\}}$
).
(ii) The
function
$f(x)$ is represented as a hyperfunctionwhere the
functions
$F_{j}$ are holomorphic in$\{z\in \mathbb{C}^{n};z\in\Omega+i\Gamma_{j},$ $|{\rm Im} z|<\epsilon$
for
some
$\epsilon>0\}$and
for
any compactset$K\subset\Omega$ there exist constants$L$ and$C$ (resp.for
any$L>0$there exists $C$) such that
$\sup_{x\in K}|F_{j}(x+iy)|\leq CM^{*}(L/|y|)$,
where $i:=\sqrt{-1}.$
Definition 2.7. For two classes $*$ and $\dagger$
we
define their inclusion relations.$\dagger\leq*\Leftrightarrow \mathcal{E}^{\dagger}\subset \mathcal{E}^{*},$
(2.9)
$\dagger<*\Leftrightarrow \mathcal{E}^{\dagger}\subsetneq \mathcal{E}^{*}$
Definition 2.8. $A$ function$\epsilon(t)>0$ defined for $t>0$ is said to be subordinate if it
is continuous, monotonously increasing and $\epsilon(t)/t$ is monotonously decreasing to
zero
as
$tarrow\infty$, in particular(2.10) $\lim_{tarrow\infty}\frac{\epsilon(t)}{t}=0.$
Proposition 2.9 (cf. Lemma 3.10 in [6]). Forpositive sequences $M_{p}$ and $N_{p}$
satis-fying ($M$.1), the following conditions
are
equivalent. (i) $M_{p}\prec N_{p}.$(ii) For any $L>0$, there exists a constant$C>0$ such that
$N(t)\leq CM(Lt)$, for $0<t<\infty.$
(iii) There exists a subordinate
function
$\epsilon(t)$ such that$N(t)\equiv M(\epsilon(t))$
.
Definition 2.10. $A$ differential operator
$P(D)= \sum_{\alpha}a_{\alpha}D^{\alpha}$ of infinite order is
de-fined to belong to the class $(M_{p})$ (resp. $\{M_{p}\}$), ifthere exist such constants $L$ and $C$
(resp. for any $L>0$ there exists such a constant $C$) that $|a_{\alpha}|\leq(CL^{|\alpha|})/M_{|\alpha|}$ holds
for any $\alpha$
.
We call this operator anultradifferential
operator ofthe class $(M_{p})$ (resp.$\{M_{p}\})$.
\S 3.
Known Structure TheoremsIn this section,
we
review the known resultsonthestructuretheorems. The structure theorem for the distributionswas
proved by L. Schwartz.Theorem 3.1 (cf. [9]). Any distribution $f$ is locally represented
as
(3.1) $f=P(D)g,$
where $P(D)$ is
a
differential
opemtorof
thefinite
order with constantcoefficients
and $g$is
a
continuousfunction.
H. Komatsu [6] proved the structure theorem for the strong
non
quasi-analyticul-tradistributions.
Theorem 3.2 (cf. [6]). Let the sequence$M_{p}$ satisfythe conditions ($M$.1), ($M$.2) and
($M$.3). Then$f\in \mathcal{D}b^{*},$ where $*is(M_{p})$ or$\{M_{p}\}$, is locally represented in the
form
(3.1),where $P(D)$ is an
ultmdifferential
opemtorof
class $*with$ constantcoefficients
and $g$ isa continuous
function.
This theorem
was
extended by R. W. Braun [1] for thenon
quasi-analytic ultradis-tributions.Theorem 3.3 (cf. [1]). Let thesequence$M_{p}$ satisfythe conditions ($M$.1), ($M$.2) and
($M$.3)’. Then
for
$f\in \mathcal{D}b^{*}$, where $*is(M_{p})$or
$\{M_{p}\}$, andfor
any class \dagger satisfying$*<\dagger$, there exist
an
ultmdifferential
opemtor $P(D)$of
class $*with$constant
coefficients
and an
ultmdifferentiable function
$g$of
class \dagger such that the representation (3.1) locallyholds.
In [3], [4], A. Kaneko proved the structure theorem for the hyperfunctions. Theorem
3.4
(cf. [3], [4]). Any hyperfunction $f$ is globally representedas
(3.2) $f=J(D)g,$
where $J(D)$ is a local opemtor with constant coefficients, that is, $J(D)$ is an
infinite
order
differential
opemtor $J(D)= \sum_{\alpha}a_{\alpha}D^{\alpha}$ with thecoefficients
satisfying $\lim_{|\alpha|arrow\infty}|\alpha\sqrt[1]{|a_{\alpha}|\alpha!}=0,$and $g$ is an infinitely
differentiable
function.
Theorem
3.4
was
the first result to give the structure of generalizedfunctions
more
singular than the distributions. After this work, the structure of generalized functions
was
well studied by other mathematicians, for example, Theorem 3.2 by H. Komatsu, Theorem 3.3 by R. W. Braun etc. A. Kaneko also applied the $10$cal operators to give a newcharacterization ofanalyticfunctions (cf. [3]). We note that thestructure theoremsfor the
distributions
(Theorem 3.1) and for thenon
quasi-analytic ultradistributions(Theorems 3.2 and 3.3) hold only locally, whereas the representation in (3.2) is global
on
any open set by virtue ofthe properties of the (Fourier) hyperfunctions.The structure theorem for the quasi-analytic ultradistributions had been left open,
which
was
proved by the author [10].Theorem 3.5 (cf. [10]). Let $M_{p}$ satisfy ($M$.0), ($M$.1), ($M$.2), $(QA)$ and $(NA)$
.
As-sume that $f\in \mathcal{D}b^{*}$, where $*=(M_{p})$ or $\{M_{p}\}$
.
Thenfor
any class \dagger satisfying $*<\dagger$there exist $g\in \mathcal{E}^{\uparrow}and$ an
ultradifferential
opemtor$P(D)$of
class $*such$ that therepre-sentation
(3.3) $f=P(D)g$
locally holds.
The mainpurpose ofthis paper is to extend Theorem 3.5 in orderthat the structure theorem of quasi-analytic ultradistributions holds globally, which shall be discussed in
the next section.
\S 4.
Main TheoremsItis
our main
purpose inthis articletogive theglobalstructure theorem fordistribu-tions
and
non-quasi-analytic ultradistributions with suitable global growth conditionsand prove the global structure theorem for the all quasi-analytic ultradistributions,
which shall be discussed in this section. We first define the ultradistributions with growth conditions.
Definition 4.1. Let $M_{p}$ be a sequence of positive numbers. then
a
function $f\in$$\mathcal{E}^{(M_{p})}(\mathbb{R}^{n})$ $($resp. $f\in \mathcal{E}^{\{M_{p}\}}(\mathbb{R}^{n}))$ belongs to$\mathcal{P}^{(M_{p})}$
(resp. $\mathcal{P}^{\{M_{p}\}}$) if for any $h>0$ there
exists
a
constant $C=C_{h}>0$ $(resp.$ there exists $a$ constants $h>0, C>0)$ such that(4.1) $\sup\underline{|D^{\alpha}f(x)|}<C|h|^{|\alpha}IM_{|\alpha|},$ $x\in \mathbb{R}^{n}M(h|x|)$
for any multi-index $\alpha$. Let us define
$\mathcal{P}^{\{M_{p}\},h}=\bigcup_{C>0}\{f\in \mathcal{P}^{\{M_{p}\}};\sup_{x\in \mathbb{R}^{n}}\frac{|D^{\alpha}f(x)|}{M(h|x|)}\leq C|h|^{|\alpha|}M_{|\alpha|}$ (for all $\alpha$)$\}.$
For $f\in \mathcal{P}^{\{M_{p}\},h}$,
we
define itsnorm
byFor topologies
of
ultradifferentiable
classes, the followingrelations hold.
(4.3) $\mathcal{P}^{\{M_{p}\}}=\lim_{arrow}\mathcal{P}^{\{M_{p}\},h}, \mathcal{P}^{(M_{p})}=\lim_{arrow}\mathcal{P}^{\{M_{p}\},h}$
$harrow\infty harrow 0$
The set $\mathcal{Q}^{*};=\mathcal{P}^{*J}$ is defined
as
the strong dual of$\mathcal{P}^{*},$ where $*=(M_{p})$ or $\{M_{p}\}$, and iscalled
as
the spaceof
the Fourier ultmdistributionsof
class $*.$Proposition 4.2. Assume that
a
sequence $M_{p}(p=0,1,2, \ldots)$of
positive numberssatisfies
the conditions ($M$.0), ($M$.1), ($M$.2) and $(NA)$. Then the following conditionsare equivalent.
(i) The
function
$\hat{f}$is the Fourier-Laplacetmnsform of
$f\in \mathcal{P}^{(M_{p})}$ (resp. $f\in \mathcal{P}^{\{M_{p}\}}$).(ii) For $h>0$ there exists
a constant
$C=C_{h}>0$ (resp. there existconstants
$h,$$C>0)$ such that
(4.4) $|P_{1}(D)(P_{2}( \xi)\hat{f}(\xi))|\leq\frac{C}{M(h|\xi|)},$ $for\xi\in \mathbb{R}^{n},$
for
anyultmdifferential
operator $P_{1}(D)$ and$P_{2}(D)$of
thesame
class.Theorem 4.3 (The Paley-Wiener Theorem for $NA$ Ultradistributions).
Let $M_{p}$ satisfy ($M$.0), ($M$
.
1), $(M.2)’$ and $(NA)$.
For any compactconvex
set $K\subset \mathbb{R}^{n},$the following conditions are equivalent. (i) $\hat{f}$is the Fourier-Laplace
transform of
$f\in \mathcal{D}b_{K}^{(M_{p})}$ $($resp. $f\in \mathcal{D}b_{K}^{\{M_{p}\}})$.
(ii) $\hat{f}(\zeta)$ is
an
entirefunction of
$\zeta\in \mathbb{C}^{n}$ whichsatisfies
the following: there exist $L,$$C>0$ $(resp. for any L>0,$ there exists $C>0)$ such that
for
any $\xi\in \mathbb{R}^{n}$(4.5) $|\hat{f}(\xi)|\leq CM(L|\xi|)$,
and
for
any $\epsilon>0$, there exists $C_{\epsilon}>0$ such thatfor
any $\zeta\in \mathbb{C}^{n},$(4.6) $|\hat{f}(\zeta)|\leq C_{\epsilon}\exp(H_{K}({\rm Im}\zeta)+\epsilon|\zeta|)$,
where $H_{K}(y)$ $:= \sup_{x\in K}\{x\cdot y\}(y\in \mathbb{R}^{n})$ is the supporting
function
of
$K.$ (iii) $\hat{f}(\zeta)$ is an entirefunction of
$\zeta\in \mathbb{C}^{n}$ whichsatisfies
the following: there exist $L,$$C>0$ $(resp. for any L>0,$ there exists $C>0)$ such that
for
any $\zeta\in \mathbb{C}^{n},$(4.7) $|\hat{f}(\zeta)|\leq CM(L|\zeta|)e^{H_{K}({\rm Im}\zeta)}.$
Definition 4.4. Let $\mathbb{D}^{n}$ $:=\mathbb{R}^{n}\sqcup S^{n-1}$ be the directional compactification of $\mathbb{R}^{n}$
For a compact subset $K\subset \mathbb{D}^{n}$,
we
define the space ofultradifferentiable test functionsas
follows:$\mathcal{P}^{\{M_{p}\}}(K)=\{\varphi(x)\in C^{\infty}(K\cap \mathbb{R}^{n})$;there exist $C,$ $h>0$ such that for any
We define
$\mathcal{P}^{(M_{p})}(K)$ in thesame
way. The growth condition is meaningful only if $K$contains points at infinity. Notice that compact subsets of $\mathbb{D}^{n}$ restricted to $\mathbb{R}^{n}$ not
necessarily bounded in the usual
sense.
By the same wayas
Definition 2.4, $\mathcal{Q}^{*}$ itselfis defined as a sheaf of Fourier ultradistributions of class $*$ on $\mathbb{D}^{n}$ whose restriction
to $\mathbb{R}^{n}$ agrees with the usual sheaf$\mathcal{D}b^{*}$ ofultradistributions, since $\mathcal{Q}^{*}$ is defined on the
directionalcompactification of$\mathbb{R}^{n}.$ $\mathcal{P}^{*}$ being invariant under the Fourier transformation
by virtue ofProposition 4.2, $\mathcal{Q}^{*}$ is also invariant under the Fourier transformation.
Theorem 4.5. Let $M_{p}$ satisfy ($M$.0), ($M$.1), ($M$.2)’ and $(NA)$. The following
con-ditions are equivalent.
(i) $f\in \mathcal{Q}^{(M_{p})}$ (resp. $f\in \mathcal{Q}^{\{M_{p}\}}$)
(ii) $f\in \mathcal{D}b^{(M_{p})}$ $($resp. $f\in \mathcal{D}b^{\{M_{p}\}})$ and there exist constants $L>0$ and $C>0$ (resp.
for
any $L>0$ there exists a constant $C>0$) such thatfor
any $\xi\in \mathbb{R}^{n}$(4.8) $|\hat{f}(\xi)|\leq CM(L|\xi|)$.
Theorem 4.6.
If
the class $*is$ quasi-analytic, then(i) $\mathcal{Q}^{*}$ isflabby.
(ii) The restriction $\mathcal{Q}^{*}(\mathbb{D}^{n})arrow \mathcal{D}b^{*}(\mathbb{R}^{n})$ is surjective.
This theorem isproved by L. H\"ormander ([2]) for the $\{M_{p}\}$ classes, the idea of which
can
be extended for the $(M_{p})$ classes.Now
we
study the global structure theorems. The following theorem is well known.Theorem 4.7. Any tempered distribution $f\in S’$ is globally represented as
(4.9) $f=P(D)g,$
where $P(D)$ is
a
differential
opemtorof finite
order with constantcoefficients
and$g$ isa
continuousfunction.
It is essential for this theorem to hold that the Fourier-Laplacetransformation is
an
isomorphism on$S’.$
Let
us
proveour
main theorem in this article.Theorem 4.8. Let the sequence $M_{p}$ satisfy the conditions, ($M$.1), ($M$.2) and$p!\subset$ $M_{p}$.
Assume
that$f\in \mathcal{Q}^{*}(\mathbb{D}^{n}),$ where $*is(M_{p})$ or$\{M_{p}\}$.
Thenfor
any class\dagger satisfying$*<\dagger$ there exist$g\in \mathcal{P}^{\dagger}(\mathbb{R}^{n})$ and an
ultmdifferential
opemtor $P(D)$of
class $*such$ thatthe representation
(4.10) $f=P(D)g,$
holds.
If
$M_{p}=p!$, we only consider the $\{M_{p}\}$ class, which yields that $\mathcal{Q}^{\{M_{p}\}}(\mathbb{D}^{n})=$ $\mathcal{Q}(\mathbb{D}^{n})$ is the spaceof
Fourier hyperfunctions.Before
proving this theorem, letus
prepare
a
lemma.Lemma 4.9. Let a sequence $M_{p}$ satisfy ($M$.0), ($M$.1), $(M.2)’$ and$p!\subset M_{p}$.
If for
any $h>0$ there exists a constant $C=C_{h}>0$ (resp. there exist constants $h>0$ and
$C>0)$ such that
(4.11) $|f(x)| \leq\frac{C}{M(h|x|)},$
then $\hat{f}\in \mathcal{E}^{(M_{p})}$ (resp. $\hat{f}\in \mathcal{E}^{\{M_{p}\}}$).
If
$M_{p}=p!$, we only consider the $\{M_{p}\}$ class.Proof of
Theorem4.8.
I. The proof
for
the $(M_{p})$ class.By Theorem 4.5, there exist $L>0$ and $C>0$ such that (4.8) holds. Define the ultradifferential operator ofclass $(M_{p})$ by
(4.12) $P(D) := \sum_{p=0}^{\infty}\frac{(-C\Delta)^{p}}{M_{2p}}.$
for
some
suitable constant $C$ such that $| \frac{\hat{f}(\xi)}{P(\xi)}|$ is bounded. By lemma 4.9(4.13) $g := \mathcal{F}^{-1}(\frac{\hat{f}(\xi)}{P(\xi)^{2}})\in \mathcal{E}^{\{M_{p}\}},$
where $\mathcal{F}^{-1}$ is the inverse Fourier-Laplace transformation operator. We have
(4.14) $f(x)=P(D)^{2}g(x)$
.
By virtue of ($M$.2),
we
see
that $P(D)^{2}$ isan
ultradifferential operator of class $(M_{p})$.
II.The prooffor $\{M_{p}\}$ class.
Let $\{M_{p}\}<\dagger=(N_{p})$
or
$\{N_{p}\}.$ $L_{p}$ $:=\sqrt{M_{p}N_{p}}$ yields $M_{p}\prec L_{p}\prec N_{p}$.
There exists a subordinate function $\epsilon_{1}$ such that $L(t)=M(\epsilon_{1}(t))$, hence there exist such a positivedecreasing sequence $l_{p}^{(1)}$ with $\lim_{parrow\infty}l_{p}^{(1)}=0$ and
a
constant $A_{1}>0$ that(4.15) $P_{1}( \xi):=\sum_{p=0}^{\infty}\frac{(l_{2p}^{(1)}|\xi|)^{2p}}{M_{2p}}\geq A_{1}M(\epsilon_{1}(|\xi|))$ ,
for any $\xi\in \mathbb{R}^{n}$ By virtue of Theorem 4.3, there exists
a
subordinate function $\epsilon_{2}$ suchthat
for any $\xi\in \mathbb{R}^{n}$
.
There exista
positive decreasing sequence $l_{p}^{(2)}$ satisfying$\lim_{parrow\infty}l_{p}^{(2)}=0$
and
a
constant $A_{2}>0$ such that(4.17) $P_{2}( \xi):=\sum_{p=0}^{\infty}\frac{(l_{2p}^{(2)}|\xi|)^{2p}}{M_{2p}}\geq A_{2}M(\epsilon_{2}(|\xi|))$,
for any $\xi\in \mathbb{R}^{n}$. Let
us
define(4.18) $g := \mathcal{F}^{-1}(\frac{\hat{f}(\xi)}{P_{1}(\xi)P_{2}(\xi)})$,
then it is proved that $g\in \mathcal{E}^{\{L_{p}\}}\subset \mathcal{E}^{\dagger}$. We have
(4.19) $P_{1}(D)P_{2}(D)g(x)=f(x)$
.
By the condition ($M$.2), the ultradifferential $operatorP_{1}(D)P_{2}(D)$ belongs to the $\{M_{p}\}$
class. $\square$
By the proof of this theorem, we obtain the following global structure theorem for non quasi-analytic
ultradistributions.
Theorem 4.10.
Let $M_{p}$ satisfy the conditions ($M$.1), ($M$.2) and $(M.3)’$.
Assume
that $f\in \mathcal{D}b^{*}(\mathbb{D}^{n})$, where $\Omega\subset \mathbb{R}^{n}$ is open and
$*$ is $(M_{p})$ or $\{M_{p}\}$, satisfying the
condition that there exist constants $L>0$ and $C>0$ (resp.
for
any $L>0$ there existsa constant $C>0$) such that the estimate (4.8) holds. Then
for
any class \dagger satisfying$*<\dagger$ there exist$g\in \mathcal{P}^{\dagger}(\mathbb{R}^{n})$ and an
ultmdifferential
opemtor$P(D)$of
class $*such$ thatthe representation (4.10) globally holds.
By virtue of Theorems 4.6 and 4.8, we obtain the globalrepresentation ofany quasi-analytic ultradistribution.
Theorem 4.11.
Assume
that $f\in \mathcal{D}b^{*}(\Omega)$, where $\Omega\subset \mathbb{R}^{n}$ is open $and*is$ aquasi-analytic class satisfying the condition ($M$.2). For any class \dagger satisfying$*<\dagger$ there exist
$g\in \mathcal{E}^{\dagger}$ and
an
ultmdifferential
opemtor$P(D)$of
class $*such$ that the representation(4.20) $f=P(D)g,$
globally holds (on $\Omega$).
\S 5.
ConclusionWe have proved aglobalrepresentationtheorem for any quasi-analytic ultradistribu-tion (Theorem 4.11), hyperfuncultradistribu-tional counterpart of which has been proved A. Kaneko
(Theorem3.4). The proofs
of these two
global representations essentially dependson
the flabbiness ofthe sheaves ofthe quasi-analytic ultradistributions and the hyperfunctions(Theorem 4.6).
Onthe other hand, in order to obtain the global representation ofthe distributions and the
non
quasi-analytic ultradistributions,we
had to restrict theirgrowth towardin-finity (Theorems 4.7and 4.10). It may be interesting to study whether the assumptions in Theorems 4.7 and 4.10
are
optimal for the global representations to hold.References
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