Vol. 45, No. 1, 2015, 125-142
ON A CLASS OF ULTRADIFFERENTIABLE FUNCTIONS
1Stevan Pilipovi´c2, Nenad Teofanov3 and Filip Tomi´c4
Dedicated to Professor Stankovi´c on the occasion of his 90th birthday.
Abstract. We introduce a class of ultradifferentiable functions which contains Gevrey functions and study its basic properties. In particular, we investigate the continuity properties of certain (ultra)differentiable operators. Finally, we discuss microlocal properties in appropriate dual spaces.
AMS Mathematics Subject Classification(2010): 46F05, 46E10, 35A18 Key words and phrases: Ultradifferentiable functions; Gevrey classes;
ultradistributions; wave-front sets
1. Introduction
Since their introduction in the context of regularity properties of funda- mental solution of the heat operator in [1], Gevrey classes were used in many situations related to the general theory of linear partial differential operators such as hypoellipticity, local solvability and propagation of singularities. We refer to [6] for the definition and detailed exposition of Gevrey classes and their applications to the theory of linear partial differential operators. It is known that intersection (projective limit) of Gevrey classes contains the space of ana- lytic functions, while its union (inductive limit) is contained in the class of smooth functions. However, there is a gap between the Gevrey classes and the space of smooth functions, so that in certain situations a more refined descrip- tion of regularity might be useful. The purpose of this paper is to introduce a family of smooth functions which are less regular than the Gevrey functions, and to study its basic properties. The main motivation for our approach is that it can be used in the study of intermediate singularities between the classical C∞ and the Gevrey type singularities, see Section 4.
We recall Komatsu’s approach [4] and introduce a family of sequences of the formMpτ,σ=pτ pσ,p∈Z+, for someτ >0 andσ >1, so that the corresponding space of ultradifferentiable functions contains Gevrey classes. Such sequences
1 Acknowledgement: This research is supported by Ministry of Education, Science and Technological Development of Serbia through the Project no. 174024.
2Department of Mathematics and Informatics, Faculty of Science, University of Novi Sad, e-mail: [email protected]
3Department of Mathematics and Informatics, Faculty of Science, University of Novi Sad, e-mail: [email protected]
4Faculty of Technical Sciences, University of Novi Sad, e-mail: [email protected]
do not satisfy conditions (M.2) and (M.2)′ (cf. Subsection 1.2), which are in our analysis replaced by(M.2)^′ and(M.2), see Lemma 2.2.^
In Section 3 we define the corresponding space of ultradifferentiable func- tions and study its basic properties. For example, we show that there exists a nontrivial smooth compactly supported function in our class which does not belong to Gevrey classes.
Recall the condition (M.2) provides the stability under the action of appro- priate ultradifferentiable operators. SinceMpτ,σ does not satisfy (M.2) we can not expect that our space is closed under the action of appropriate ultradiffer- entiable operators. However, the continuity holds if we observe an inductive limit with respect to one of the parameters, Theorems 3.2 and 3.3.
In Section 4 we discuss a new approach to the study of microlocal proper- ties of ultradistributions in the context of the new class of ultradifferentiable functions.
1.1. Notation
Throughout the paper, we use the standard notation: nonnegative integers, integers, positive integers, real numbers, positive real numbers and complex numbers are denoted by N, Z, Z+, R, R+ and C, respectively. The integer part (the floor function) ofx∈R+is denoted by⌊x⌋:= max{m∈N : m≤x}. For a multi-indexα= (α1, . . . , αd)∈Nd we write∂α=∂α1. . . ∂αd and|α|=
|α1|+. . .|αd|. We will also use the Stirling formula: N! =NNe−N√
2πN e12NθN , for some 0 < θN < 1, N ∈ Z+. By Cm(K), m ∈ N, we denote the Banach space ofm-times continuously differentiable functions on a regular compact set K⊂⊂U, whereU ⊆Rd is an open set, andC∞(K) is the corresponding set of smooth functions on K, see [4]. Convolution is denoted with f ∗g(x) =
∫
Rdf(x−y)g(y)dy, whenever the integral make sense.
For locally convex topological spaces X and Y we write X ,→ Y when X ⊆Y and the identity mapping fromX to Y is continuous. If, in addition, X ̸=Y then the embedding is strict. By X′ we denote the strong dual of X and by⟨·,·⟩X the dual pairing betweenX andX′. The set of continuous linear operators fromX toY is denoted by L(X, Y).
A linear map B ∈ L(X, Y), X, Y are Banach spaces, is quasi-nuclear if there exists a sequence {x′j} in X′ such that ∑∞
j=1
∥x′j∥X′ < ∞ and ∥Bx∥Y ≤
∑∞ j=1
|⟨x, x′j⟩X|. In particular, a quasi-nuclear map A ∈ L(X, Y) is nuclear if there exists bounded sequencesx′j ∈X′ (with respect to the strong topology) andyj∈Y,j∈Z+, and a sequenceλj ∈C,j∈Z+, such that ∑∞
j=1
|λj|<∞and Ax=
∑∞ j=1
λj⟨x, x′j⟩Xyj. We refer to [11, Section III.7] and [8] for an extension of nuclear and quasi-nuclear mappings to arbitrary locally convex topological spaces.
1.2. Classical spaces of ultradifferentiable functions
We use Komatsu’s approach to the theory of ultradistributions as follows, see [4].
ByMp= (Mp)p∈N we denote a sequence of positive numbers such that:
(M.0) M0= 1;
(M.1) Mp2≤Mp−1Mp+1, p∈Z+; (M.2) (∃A, B >0) Mp+q ≤ABpMpMq, p, q∈N;
(M.3)′ ∑∞
p=1 Mp−1
Mp <∞.
ThenMpalso satisfies weaker conditions: (M.1)′MpMq ≤Mp+qand (M.2)′ Mp+q ≤ABqpMp for some A, B >0,p, q∈N.
Let there be given sequenceMp which satisfies (M.0)−(M.3) and letU ⊆ Rd be an open set. A functionϕ∈C∞(U) is anultradifferentiable functionif on each compact subset K⊂⊂U there exist positive constantsC andhsuch that
(1.1) sup
x∈K|∂αϕ(x)| ≤Ch|α|M|α|, α∈Nd.
IfKis a fixed compact set inRdand ifh >0 is given, thenϕ∈ E{Mp},h(K) ifϕ∈C∞(K) and if (1.1) holds for someC >0. Ifϕ∈C∞(Rd) and suppϕ⊂ K,thenϕ∈D{KMp},h.
The space of ultradifferentiable functions of class{Mp}is given by E{Mp}(U) = limK←−
⊂⊂U
lim−→
h→∞
E{Mp},h(K) = ∩
K⊂⊂U
∪
h→∞
E{Mp},h(K),
and its strong dual is the space of ultradistributions of Roumieu type of class Mp. The space of ultradifferentiable functions of class{Mp} with support in K is given by
D{Mp}(U) = limK−→
⊂⊂U
lim−→
h→∞
DK{Mp},h= ∪
K⊂⊂U
∪
h→∞
D{KMp},h.
and its strong dual is the space of compactly supported ultradistributions of Roumieu type of classMp.
In particular, if Mp is Gevrey sequence,Mp =p!t, t >1, then E{p!t}(U) is theGevrey class of ultradifferentiable functions. Note thatp!t, t >1, satisfies (M.0)−(M.3). We refer to [4] for a detailed study of different classes of ultradifferentiable functions and their duals.
Let there be given t ≥ 1, (x0, ξ0)∈ U ×Rd\{0}. Then the Gevrey wave front setW Ft(u) ofu∈ D′{p!t}(U) can be defined as follows: (x0, ξ0)̸∈W Ft(u)
if and only if there exists an open neighborhood Ω ofx0, a conic neighborhood Γ ofξ0 and a bounded sequenceuN ∈ E′{p!t}(U), such thatuN =uon Ω and
|buN(ξ)| ≤AhNN!t
|ξ|N , N ∈Z+, ξ∈Γ,
for some A, h > 0. Here, and in what follows, the Fourier transform buof a distributionuis normalized to beu(ξ) =b ∫
Rdu(x)e−2πixξdx,ξ∈Rd, whenever the integral is well defined. Ift= 1, then the Gevrey wave front set is sometimes called theanalytic wave front setand denoted byW FA(u),u∈ D′{p!}(U). We refer to [5, 6] for details.
2. New classes of ultradifferentiable functions
In this section we introduce new spaces of ultradifferentiable functions in an analogy toE{Mp}(U) andD{Mp}(U). We introduce more general sequences than the Gevrey type sequences p!t, t > 1, and begin our investigations by studying their basic properties. We start with a simple but useful Lemma.
Lemma 2.1. Let τ >0,σ > 1 and Mpτ,σ =pτ pσ, p∈ Z+, M0τ,σ = 1. Then there existA, B, C >0 such that
(2.1) Mpτ,σ≤ACpσ⌊pσ⌋!τ /σ and ⌊pσ⌋!τ /σ≤BMpτ,σ. Proof. Bypσ≤ ⌊pσ⌋+ 1 andpσ≤2⌊pσ⌋, p∈Z+, we have
pτ pσ ≤pτ(⌊pσ⌋+1)≤pτ (
2⌊pσ⌋)τ⌊pσ⌋/σ
≤eτ pσ2τ⌊pσ⌋/σ⌊pσ⌋τ⌊pσ⌋/σ, and the left hand side inequality in (2.1) follows from the Stirling formula.
The right hand side inequality in (2.1) follows directly from the Stirling formula:
⌊pσ⌋!τ /σ≤(
e−⌊pσ⌋√
2π⌊pσ⌋⌊pσ⌋⌊pσ⌋)τ /σ
≤B⌊pσ⌋τ⌊pσ⌋/σ≤Bpτ pσ, for someB >0.
Next we study properties of the sequence Mpτ,σ, τ >0,σ >1 with respect to the conditions (M.0)−(M.3)′.
Lemma 2.2. Let τ >0,σ > 1 and Mpτ,σ =pτ pσ, p∈ Z+, M0τ,σ = 1. Then the following properties hold:
(M.1) (Mpτ,σ)2≤Mpτ,σ−1Mp+1τ,σ,p∈Z+,
(M.2)^′ Mp+qτ,σ ≤CqpσMpτ,σ, for some sequence Cq ≥1,p, q∈N,
(M.2)^ Mp+qτ,σ ≤ Cpσ+qσMpτ2σ−1,σMqτ2σ−1,σ, p, q ∈ N, for some constant C >1.
Proof. Note that (M.0) holds by the assumption and (M.3)′ will be proved in Lemma 3.1.
We may assume thatτ= 1 without loos of generality.
The condition (M.1) obviously holds when p= 1. Ifp−1∈Z+ then the sequence lnMp is convex since the second derivative off(t) =tσlnt, t >0, is positive when t > eσ(σ−1)1−2σ . This implies (M.1).
The conditions(M.2)^′ and(M.2) trivially hold when^ p= 0 (or q= 0). Let p, q∈Z+.
To prove(M.2)^′ we putσ=n+δwheren∈Z+ and 0< δ≤1. Ifσ̸∈Z+
then n=⌊σ⌋, 0< δ <1,while n=σ−1, δ= 1,ifσ∈Z+. By the binomial formula we have:
(p+q)σ ≤ (p+q)n(pδ+qδ) =pσ+
∑n
k=1
(n k )
pσ−kqk
+
∑n
k=0
(n k )
pn−kqk+δ ≤pσ+ 2n(pσ−1qn+pnqσ)
≤ pσ+ 2n+1qσpσ−δ, wherefrom
(2.2) (p+q)σln(p+q)≤pσln(p+q) + 2n+1qσpσ−δln(p+q).
We will use the fact that for anyα >0 there existsA >0 such that lnx≤Axα, x≥1. Thereforep≤Cpδ, for someC >1 whenp∈Z+ and 0< δ≤1.
The first term on the right hand side of the inequality (2.2) can be estimated by
pσln(p+q) = pσ (
lnp+ ln (
1 +q p
))≤pσlnp+pσ−1q
≤ pσlnp+qpσ, (2.3)
while for the second term we use
2n+1qσpσ−δln(p+q) = 2n+1qσpσ−δ (
lnp+ ln (
1 +q p
))
≤ 2n+1qσpσlnC+ 2n+1qσpσln(1 +q). (2.4)
Now (2.3) and (2.4) imply (M.2)^′ by taking the exponentials in (2.2).
It remains to prove(M.2). From (p^ +q)σ ≤2σ−1(pσ+qσ) it follows that (p+q)(p+q)σ ≤(p+q)2σ−1pσ(p+q)2σ−1qσ.
Since
2σ−1pσln(p+q) = 2σ−1pσ (
lnp+ ln (
1 + q p
))
≤ 2σ−1pσlnp+ 2σ−1qpσ−1
≤ 2σ−1pσlnp+ 2σ−1(p+q)σ,
by taking the exponentials we obtain (p+q)2σ−1pσ ≤p2σ−1pσe2σ−1(p+q)σ.Simi- larly, (p+q)2σ−1qσ ≤q2σ−1qσe2σ−1(p+q)σ.Therefore
(p+q)(p+q)σ ≤p2σ−1pσq2σ−1qσe2σ(p+q)σ and(M.2) is proved.^
Remark 2.1. From the proof of (M.2)^′ it follows that Mpτ,σ does not satisfy the Komatsu condition (M.2)′. As a first guess one might assume that the sequenceMpτ,σ satisfies
(2.5) Mp+qτ,σ ≤Cpσ+qσMpτ,σMqτ,σ, C >0, p, q∈N,
instead. Assume that (2.5) holds forMpτ,σ, and thatτ= 1. Then, forp=q̸= 0, (2.5) gives
(2.6) p(2p)σ ≤(C1p)2pσ, p∈Z+, with C1 = C
22σ−1. By taking the logarithm we obtain 2σ−1lnp ≤ lnC1p, p ∈ Z+, but this holds only for finitely many p ∈ Z+. This contradiction explains why(M.2)^′ is an appropriate substitution of (M.2)′when considering Mpτ,σ.
The next simple Lemma will be used later on.
Lemma 2.3. Let τ >0 andσ >1 be fixed. Then (2.7) T˜τ,σ(h) := sup
ρ>0
hρσ
ρτ ρσ =eσeτh
σ
τ , h >0.
Proof. Put f(ρ) = ρhτ ρσρσ , ρ >0. Since (lnf(ρ))′ =ρσ−1(σlnh−τ σlnρ−τ), ρ >0, forρ0:=h1τe−σ we have maxρ>0lnf(ρ) =f(ρ0) = eστ hστ, and Lemma is proved.
Remark 2.2. In the theory of ultradifferentiable functions, for a given sequence Mp,p∈N, the functionTgiven byT(h) = supp>0hMpM0
p ,h >0, is calledthe as- sociated functionof the sequenceMp,p∈N(in [4] the function supp>0lnhMpM0
p
is considered instead of T(h)). It plays an important role in the study of the spaces of ultradifferentiable functions and their dual spaces. Notice that ˜Tτ,σ given by (2.7) is not the associated function of the sequenceMpτ,σ. It is known that the associated function Tτ(h) of the sequence p!τ, τ > 0, satisfies the estimate of the formC1eτeh
1
τ ≤Tτ(h)≤C2eτeh
1
τ, for someC1, C2>0, and for everyh >0, cf. [2, Chapter IV.2]. This implies that
C′(Tτ(hσ))1/σ≤T˜τ,σ(h)≤C′′(Tτ(hσ))1/σ for someC′, C′′>0,h >0 and for any givenτ >0,σ >1.
Next we introduce a family of spaces of ultradifferentiable functions in an analogy to the spacesE{Mp}(U) andD{Mp}(U) from the Introduction.
LetU ⊆Rdbe an open set,K⊂⊂U andh >0. Thenϕ∈C∞(U) belongs to the spaceEτ,σ,h(K) if there existsA >0 such that
(2.8) |∂αϕ(x)| ≤Ah|α|σ|α|τ|α|σ, α∈Nd. ThenEτ,σ,h(K) is a Banach space with the norm given by (2.9) ∥ϕ∥Eτ,σ,h(K)= sup
α∈Nd
sup
x∈K
|∂αϕ(x)| h|α|σ|α|τ|α|σ.
Let Dτ,σ,hK be the set of ϕ ∈ C∞(Rd) with support in K such that (2.8) holds for some A >0.
Then we define the spacesEτ,σ(U) and Dτ,σ(U)of ultradifferentiable func- tions as follows:
(2.10)
Eτ,σ(U) := limK←−
⊂⊂U
lim−→
h→∞
Eτ,σ,h(K), and Dτ,σ(U) := limK−→
⊂⊂U
lim−→
h→∞
Dτ,σ,hK .
Remark 2.3. The spacesEτ,σ(U) andDτ,σ(U) can be represented as projective and inductive limits of a countable family of spaces as follows, cf. [4]. Let {Ki}i∈N be a sequence of compact sets with smooth boundary such thatKi⊂ Ki+1,i∈N,and∪i∈NKi =U. Then, forj∈N,
Eτ,σ(U) = limi←−→∞jlim−→→∞Eτ,σ,j(Ki), and Dτ,σ(U) = limi−→→∞jlim−→→∞Dτ,σ,jKi .
Remark 2.4. From Lemma 2.1 it follows that the norms (2.9) and (2.11) ∥ϕ∥∼Eτ,σ,h(K)= sup
α∈Nd
sup
x∈K
|∂αϕ(x)|
h|α|σ⌊|α|σ⌋!τ /σ <∞, h >0.
are equivalent in Eτ,σ,h(K).
Obviously,
(2.12) Eτ1,σ1,h1(K),→ Eτ2,σ2,h2(K), h1< h2,0< τ1< τ2,1< σ1< σ2. Moreover, the following proposition holds.
Proposition 2.1. Let σ1 ≥ 1. Then for every σ2 > σ1 we have the strict embedding
(2.13) τlim−→→∞Eτ,σ1(U),→ lim←−
τ→0+
Eτ,σ2(U).
Proof. Let τ > 0 be given and let ϕ ∈ Eτ0,σ1,h(K) for some h, τ0 > 0 and K⊂⊂U. Then
(2.14) ∥ϕ∥Eτ,σ2,h(K)≤ sup
α∈Nd
h|α|σ1|α|τ0|α|σ1
h|α|σ2|α|τ|α|σ2 ∥ϕ∥Eτ0,σ1,h(K).
Putε:=σ2−σ1. Then there is a constantCε>0 so that τ0pσ1lnp≤Cετ0pσ1+ε=Cετ0pσ2 p∈N,
wherefrompτ0pσ1 ≤eCετ0pσ2 (note thatCε blows up ifε→0+). IfC:=eCετ0 andch:= max{1/h,1}, we have
(2.15) sup
α∈Nd
h|α|σ1|α|τ0|α|σ1
h|α|σ2|α|τ|α|σ2 ≤ sup
α∈Nd
(C ch)|α|σ2
|α|τ|α|σ2 ≤T˜τ,σ2(Cch) =eeστ2(C ch)
σ2 τ ,
where ˜Tτ,σis given in (2.7). Now by (2.14) and (2.15) it follows thatEτ0,σ1,h(K),→ Eτ,σ2,h(K), for arbitrary τ, τ0 >0, which implies (2.13), the embedding obvi- ously being strict.
As an immediate consequence we obtain that (2.16) Eτ0,σ1(U),→ ∩
τ >τ0
Eτ,σ1(U),→ Eτ0,σ2(U),
for any τ0>0 wheneverσ2> σ1≥1. In particular, if E{p!t}(U),t >1, is the Gevrey space of ultradifferentiable functions on U, then, for everyτ >0 and σ >1 we have
(2.17) ∪
t>1
E{p!t}(U),→ Eτ,σ(U).
Furthermore, with the notation E∞,σ(U) := limτ−→→∞Eτ,σ(U), Proposition 2.1 implies that for fixedτ0>0 andσ0>1, we have
lim−→
t→∞E{p!t}(U),→ lim←−
σ→1+
E∞,σ(U),→ E∞,σ0(U),→σlim−→→∞Eτ,σ(U),→C∞(U).
Note that our classes are larger then Gevrey classes but their inductive limits with respect toτ andσare continuously embedded inC∞(U).
3. Basic properties of the new classes of ultradifferen- tiable functions
In this section we study the basic properties of Eτ,σ(U). In separate sub- sections we show thatEτ,σ(U) are non-quasianalytic and nuclear spaces, closed under differentiation and pointwise multiplication. Finally, we study the action of ultradifferentiable operators onEτ,σ(U).
3.1. Compactly supported test functions
In this subsection we construct a compactly supported function inEτ,σ(U) following the ideas presented in [5]. We begin by showing that the sequence Mpτ,σ satisfies the non-quasianalyticity condition.
Lemma 3.1. Let τ >0,σ >1 and letMpτ,σ=pτ pσ. Then
(3.1) (M.3)′
∑∞ p=1
Mpτ,σ−1 Mpτ,σ
<∞.
Proof. Sincepσln(1 +1p) =pσ−1ln(1 +1p)p,p∈Z+, we have (3.2) τ pσ−1ln 2≤τ pσln
( 1 + 1
p
)≤τ pσ−1, p∈Z+,
so that
(3.3) 2τ pσ−1 ≤( 1 +1
p )τ pσ
≤eτ pσ−1, p∈Z+.
The left hand side of (3.3) and pσ ≥ (p−1)σ−1p = (p−1)σ+ (p−1)σ−1, p∈Z+, give
∑∞ p=1
(p−1)τ(p−1)σ
pτ pσ ≤ ∑∞
p=1
(p−1)τ(p−1)σ pτ((p−1)σ+(p−1)σ−1)
=
∑∞ p=1
( (1−1
p)τ(p−1)σ
) 1 pτ(p−1)σ−1 (3.4)
≤ ∑∞
p=1
1
(2p)τ(p−1)σ−1 <∞, which implies (3.1).
Corollary 3.1. There exists a compactly supported function ϕ ∈ E{τ,σ}(U) such that 0≤ϕ≤1 and∫
Rdϕ dx= 1.
Proof. Our goal is to construct a function inDτ,σ(U) which is not inD{p!t}(U), for any t >1. We follow the ideas from [5, Theorem 1.3.5], and repeat some steps of its proof to make the exposition self contained.
We start with one dimensional case. Letχbe the characteristic function of interval (0,1), and for c >0 letHc(x) = 1cχ(xc). Clearly ∫
RHcdx= 1 and we recall that
(3.5) (Hc∗f)′(x) = 1 c
(∫ x x−c
f(t)dt )′
=f(x)−f(x−c)
c ,
for any continuous function f onR.
Further we set
ap:= 1
(2(p+ 1))τ pσ−1, p∈N,
and note that (3.4) implies
(3.6) Mpτ,σ
Mp+1τ,σ ≤ap, p∈N.
Put um(x) = Ha0 ∗Ha1· · · ∗Ham, m ∈ N. Then, by [5, Theorem 1.3.5] it follows that the sequence{um}m∈N has a uniform limitu∈C∞(R) supported in [0, a] wherea= ∑∞
p=0
ap <∞, and∫
Ru dx= 1.
Next we estimate the derivativesu(p)m,p≤m−1. After applyingpiterations of (3.5) and by using (3.6) we obtain
|u(p)m(x)| =
p∏−1
k=0
|Hap∗ · · · ∗Ham(x)−Hap∗ · · · ∗Ham(x−ak)| ak
≤ 2p
p∏−1
k=0
1 ak sup
x∈R
|Hap∗Hap+1· · · ∗Ham(x)|
≤ 2p (p∏−1
k=0
1 ak
) sup
x∈R
|Hap(x)|( ∏m
k=p+1
∫
R
Hak(x)dx )
= 2p
∏p
k=0
1 ak ≤2p
∏p
k=0
Mk+1τ,σ
Mkτ,σ = 2pMp+1τ,σ M0τ,σ
= 2p(p+ 1)τ(p+1)σ ≤Cpσpτ pσ, (3.7)
where(M.2)^′ is used in the last inequality.
From the uniform convergence it follows that the derivatives ofualso satisfy (3.7), so thatu∈ D[0,a]τ,σ,C.
Next, we extend this to higher dimensions by puttingψ(x) =u(x+a/2) and ϕ(x) = ∏d
k=1ψ(xk) for x= (x1, x2, . . . , xd). Since the sequence Mpτ,σ fulfills the (M.1) property, we obtain
|∂αϕ(x)|=
∏d
k=1
|∂αkψ(xk)| ≤
∏d
k=1
Cαkσαkτ αkσ ≤C|α|σ|α|τ|α|σ, α= (α1, α2, . . . , αd),
wherefromϕ∈ Dτ,σ,CK withK= [−a/2, a/2]d.
Although K does not have a smooth boundary, by [5, Lemma 1.4.3] one can find an appropriate open setU and conclude thatϕ∈ Dτ,σ(U).
At the same time, ϕ̸∈ D{p!t}(U), for anyt >1. Otherwise the derivatives u(p)m in (3.7) should be bounded by Cpp!t =
p∏−1
k=0
C(k+ 1)t, for some C > 0, t >1, and for arbitrary largem∈N. In that case, the estimates in (3.7) would imply (k+ 1)t> C(2(k+ 1))τ kσ, which is obviously not true forklarge enough.
We refer to [5, Lemma 1.3.6] for a discussion about the precision of the presented construction.
3.2. Nuclearity
In this subsection we show that the spaces in (2.10) are nuclear. This is in agreement with Komatsu’s result about the nuclearity of E{Mp}(U) when Mp satisfies (M.2)′ (see [4, Theorem 2.6 ]).
Let us show that for every h > 0 there exists k > h such that identity mapping X → Y is quasi-nuclear, where X = Eτ,σ,h(K) and Y = Eτ,σ,k(K) (resp. X =Dτ,σ,hK andY =Dτ,σ,kK ). This means that seminorms onEτ,σ(K) :=
lim−→
h→∞
Eτ,σ,h(K) (resp. DKτ,σ := limh−→
→∞
Dτ,σ,hK ) are prenuclear, cf. [11, page 177].
By [11, Theorem IV 10.2] this implies that Eτ,σ(K) (resp. Dτ,σK ) is a nuclear space.
The classes under consideration can be represented as projective and induc- tive limits of a countable family of spaces, cf. Remark 2.3. The nuclearity of Eτ,σ(U) andDτ,σ(U) then follows from [11, Theorem III 7.4].
Theorem 3.1. The spaces Eτ,σ(U),DKτ,σ andDτ,σ(U) are nuclear.
Proof. We follow the idea presented in [4]. Let ϕ ∈ Eτ,σ,h(K) and let uα,j, α∈Nd,j∈Zd, be the sequence of linear functionals onEτ,σ,h(K) given by (3.8) ⟨ϕ, uα,j⟩=⟨∂αϕ, vj⟩Cd+1(K)
k|α|σ|α|τ|α|σ , where vj∈(Cd+1(K))′ is defined by the following procedure:
Choosel >0 such thatK is contained in the interior ofL= [−l, l]dand let CLd+1(πL) be the space of all d+ 1 times differentiable functions on πLwith support in L. Let B ∈ L(Cd+1(K), CLd+1(πL)) be the (Whitney’s) extension operator such that Bf|K=f and lettj ∈(CLd+1(πL))′ be given by
⟨f, tj⟩:=
∫
πL
f(y)e−iyj/ldy, j∈Zd.
From [4, Lemma 2.3] it follows that the identity operator from Cd+1(K) to C(K), given by
f(x) = 1 (2πl)d
∑
j∈Zd
e−ixj/l⟨Bf, tj⟩Cd+1
L (πL), x∈K,
is quasi-nuclear. In particular, if we put vj=tj◦B,j∈Zd, it follows that (3.9)
∑∞ j∈Zd
||vj||(Cd+1(K))′ <∞, and ||f||C(K)≤
∑∞ j∈Zd
|⟨f, vj⟩Cd+1(K)|.
By (2.9), (3.8) and the righthand side of (3.9) we obtain
∥ϕ∥Y = sup
α∈Nd
sup
x∈K
|∂αϕ(x)|
k|α|σ|α|τ|α|σ ≤ ∑
α∈Nd
∑
j∈Zd
|⟨ϕ, uα,j⟩|.