• Aucun résultat trouvé

Microlocal Asymptotic Analysis in Algebras of Generalized Functions

N/A
N/A
Protected

Academic year: 2021

Partager "Microlocal Asymptotic Analysis in Algebras of Generalized Functions"

Copied!
22
0
0

Texte intégral

(1)

HAL Id: hal-00140656

https://hal.archives-ouvertes.fr/hal-00140656

Submitted on 8 Apr 2007

HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

Microlocal Asymptotic Analysis in Algebras of Generalized Functions

Antoine Delcroix, Jean-André Marti, Michael Oberguggenberger

To cite this version:

Antoine Delcroix, Jean-André Marti, Michael Oberguggenberger. Microlocal Asymptotic Analysis in Algebras of Generalized Functions. Asymptotic Analysis, IOS Press, 2008, 59 (1-2), pp.83-107.

�10.3233/ASY-2008-0885�. �hal-00140656�

(2)

hal-00140656, version 1 - 8 Apr 2007

Microlocal Asymptotic Analysis in Algebras of Generalized Functions

Antoine Delcroix

Equipe Analyse Alg´ebrique Non Lin´eaire – Laboratoire A O C Facult´e des sciences - Universit´e des Antilles et de la Guyane, BP 250, 97157 Pointe `a Pitre Cedex, Guadeloupe (France)

Antoine.Delcroix@univ-ag.fr Jean-Andr´e Marti

Equipe Analyse Alg´ebrique Non Lin´eaire – Laboratoire G T S I Facult´e des sciences – Universit´e des Antilles et de la Guyane,

BP 250, 97157 Pointe `a Pitre Cedex, Guadeloupe (France) Jean-Andre.Marti@univ-ag.fr

Michael Oberguggenberger

Institute of Basic Sciences in Engineering – Unit of Engineering Mathematics Faculty of Civil Engineering – University of Innsbruck,

Technikerstraße 13 – 6020 Innsbruck, Austria Michael.Oberguggenberger@uibk.ac.at

April 9, 2007

Abstract

We introduce a new type of local and microlocal asymptotic analysis in algebras of gen- eralized functions, based on the presheaf properties of those algebras and on the properties of their elements with respect to a regularizing parameter. Contrary to the more classical frequential analysis based on the Fourier transform, we can describe a singular asymptotic spectrum which has good properties with respect to nonlinear operations. In this spirit we give several examples of propagation of singularities through nonlinear operators.

Keywords: microlocal analysis, generalized functions, nonlinear operators, presheaf, propaga- tion of singularities, singular spectrum.

Mathematics Subject Classification (2000): 35A18, 35A27, 46E10, 46F30, 46T30

1 Introduction

Various nonlinear theories of generalized functions have been developed over the past twenty years, with contributions by many authors. These theories have in common that the space of distributions is enlarged or embedded into algebras so that nonlinear operations on distribu- tions become possible. These methods have been especially efficient in formulating and solving nonlinear differential problems with irregular data.

Most of the algebras of generalized functions possess the structure of sheaves or presheaves, which may contain some sub(pre)sheaves with particular properties. For example, the sheaf

Supported by FWF (Austria), grant Y237.

(3)

G of the special Colombeau algebras [2, 7, 15] contains the subsheaf G of so-called regular sections of G such that the embedding: G → G is the natural extension of the classical one:

C → D. This notion of regularity leads to G-local or microlocal analysis of generalized functions, extending the classical results on the C-microlocal analysis of distributions due to H¨ormander [8]. This concept has been slightly extended in [4] to less restrictive kinds of measuring regularity. In [14], microlocal regularity theory in analytic and Gevrey classes has been generalized to algebras of generalized functions. Many results on propagation of singularities and pseudodifferential techniques have been obtained during the last years (see [5, 6, 9, 10, 11]). Nevertheless, these results are still mainly limited to linear cases, since they use frequential methods based on the Fourier transform.

In this paper, we develop a new type of asymptotic local and microlocal analysis of gener- alized functions in the framework of (C,E,P)-algebras [12, 13], following first steps undertaken in [12]. An example of the construction is given by taking G as a special case of a (C,E,P)- structure (see Subsection 2.2 for details). LetF be a subsheaf of vector spaces (or algebras) of G and (uε)ε a representative ofu∈ G(Ω) for some open set ΩRn. We first define OFG (u) as the set of all x Ω such that uε tends to a section of F above some neighborhood ofx. The F-singular support of u is Ω\OFG (u). For fixed x and u, Nx(u) is the set of all r R+ such that εruε tends to a section of F above some neighborhood of x. TheF-singular spectrum of u is the set of all (x, r) ×R+ such that r R+\Nx(u). It gives a spectral decomposition of the F-singular support of u.

This asymptotic analysis is extended to (C,E,P)-algebras. This gives the general asymptotic framework, in which the net (εr)εis replaced by any netasatisfying some technical conditions, leading to the concept of the (a,F)-singular asymptotic spectrum. The main advantage is that this asymptotic analysis is compatible with the algebraic structure of the (C,E,P)-algebras.

Thus, the (a,F)-singular asymptotic spectrum inherits good properties with respect to nonlin- ear operations (Theorem 15 and Corollary 16).

The paper is organized as follows. In Section 2, we introduce the sheaves of (C,E,P)-algebras and develop the local asymptotic analysis. Section 3 is devoted to the (a,F)-microlocal analysis and specially to the nonlinear properties of the (a,F)-singular asymptotic spectrum. In Section 4 various examples of the propagation of singularities through non linear differential operators are given.

2 Preliminary definitions and local parametric analysis

2.1 The presheaves of (C,E,P)-algebras: the algebraic structure We begin by recalling the notions from [12, 13] that form the basis for our study.

(a) Let:

(1) Λ be a set of indices;

(2) Abe a solid subring of the ringKΛ(K=RorC); this means that whenever (|sλ|)λ (|rλ|)λ

for some ((sλ)λ,(rλ)λ)KΛ×A, that is,|sλ| ≤ |rλ|for all λ, it follows that (sλ)λ A; (3)IAbe a solid ideal of A;

(4)E be a sheaf ofK-topological algebras over a topological space X. Moreover, suppose that

(5) for any open set Ω in X, the algebra E(Ω) is endowed with a family P(Ω) = (pi)i∈I(Ω) of semi-norms such that if Ω1, Ω2 are two open subsets of X with Ω1 2, it follows that I(Ω1) I(Ω2) and if ρ21 is the restriction operator E(Ω2) → E(Ω1), then, for each pi ∈ P(Ω1) the semi-normpei=piρ21 extends pi to P(Ω2) .

(6) Let Θ = (Ωh)h∈H be any family of open sets in X with Ω = h∈Hh. Then, for each pi ∈ P(Ω), i I(Ω), there exist a finite subfamily of Θ: Ω1, . . . , n(i) and corresponding

(4)

semi-norms p1∈ P(Ω1), . . . , pn(i) ∈ P(Ωn(i)), such that, for anyu∈ E(Ω) pi(u)p1(u|1) +. . .+pn(i)(u|n(i)).

(b) Define|B|={(|rλ|)λ, (rλ)λB},B =A orIA, and set H(A,E,P)(Ω) =n

(uλ)λ [E(Ω)]Λ| ∀iI(Ω),((pi(uλ))λ∈ |A|o J(IA,E,P)(Ω) =n

(uλ)λ [E(Ω)]Λ| ∀iI(Ω),(pi(uλ))λ ∈ |IA|o C=A/IA,

Note that, from (2), |A|is a subset ofAand thatA+={(bλ)λ A, ∀λΛ, bλ 0}=|A|.

The same holds forIA. Furthermore, (2) implies also thatA is aK-algebra. Indeed, it suffices to show that A is stable under multiplication by elements ofK. Let cbe in K and (aλ)λ A.

Then (caλ)λ satisfies (|caλ|)λ(|naλ|)λ for somenN. We have (naλ)λ AsinceA is stable under addition. Thus, using (2), we get that (caλ)λ A.

For later reference, we recall the following notions entering in the definition of a sheaf Aon X. Let (Ωh)h∈H be a family of open sets inX with Ω =h∈Hh.

(F1) (Localization principle) Letu, v ∈ A(Ω). If all restrictionsu|handu|h,hH, coincide, thenu=vinA(Ω).

(F2) (Gluing principle) Let (uh)h∈H be a coherent family of elements of A(Ωh), that is, the restrictions to the non-void intersections of the Ωh coincide. Then there is an element u∈ A(Ω) such that u|h=uh for allhH.

Proposition 1 (i) H(A,E,P) is a sheaf of K-subalgebras of the sheaf EΛ; (ii) J(IA,E,P) is a sheaf of ideals of H(A,E,P).

Proof. The proof can be found in [12, 13], so we just recall the main steps. We start from the statement that E andEΛ are already sheaves of algebras. From (5), we infer thatH(A,E,P) andJ(IA,E,P)are a presheaves (the restriction property holds) and that the localization property (F1) is valid. To obtain the gluing property (F2) we need property (6), which generalizes the situation fromC to E.

Theorem 2 The factor H(A,E,P)/J(IA,E,P) is a presheaf satisfying the localization principle (F1).

Proof. From the previous proposition, we know thatA=H(A,E,P)/J(IA,E,P) is a presheaf.

For Ω1 2, the restriction is defined by A(Ω2) R

21

−→ A(Ω1) u 7−→ u|1 := [uλ|1]

where (uλ)λ is any representative of u ∈ A(Ω2) and [uλ|1] denotes the class of (uλ|1)λ. The definition is consistent and independent of the representative because for each (uλ)λ∈Λ H(A,E,P)(Ω2) and (ηλ)λ∈Λ∈ J(IA,E,P)(Ω2), we have

(uλ)λ|1 := (uλ|1)λ∈ H(A,E,P)(Ω1) , λ)λ|1 := (ηλ|1)λ ∈ J(IA,E,P)(Ω1) The localization principle is also obviously fulfilled because J(IA,E,P) is itself a sheaf.

Proposition 3 Under the hypothesis (2), the constant sheaf H(A,K,|.|)/J(IA,K,|.|) is exactly the ring C=A/IA.

(5)

Proof. We clearly haveH(A,K,|.|)=Aand J(IA,K,|.|)=IA.

Definition 1 The factor presheaf of algebras over the ring C=A/IA: A=H(A,E,P)/J(IA,E,P)

is called a presheaf of (C,E,P)-algebras.

Notation 1 We denote by[uλ]the class inA(Ω)defined by(uλ)λ∈Λ ∈ H(A,E,P)(Ω). Foru∈ A, the notation (uλ)λ∈Λ u means that (uλ)λ∈Λ is a representative of u.

Remark 1 The problem of rendering A a sheaf (and even a fine sheaf ) is not studied here. It is well known that the Colombeau algebra G, which is a special case of a (C,E,P)-algebra (see Subsection 2.2), forms a fine sheaf [1, 7]. The sheaf property can be inferred from the existence of a C-partition of unity associated to any open covering of an open setofRd. This existence is fulfilled becauseX=Rdis a locally compact Hausdorff space. On the other hand, Cis a fine sheaf because multiplication by a smooth function defines a sheaf homomorphism in a natural way. Hence the usual topology and C-partition of unity defines the required sheaf partition of unity. Observing thatG is a sheaf of C-modules and using the well known result that a sheaf of modules on a fine sheaf is itself a fine sheaf, we obtain the corresponding assertion aboutG. In the general case, turning Ainto a sheaf requires additional hypotheses, which are not necessary for the results in this paper. Indeed, the presheaf structure of A and the (F1)-principle are sufficient to develop our local and microlocal asymptotic analysis.

Remark 2 The map ι:KA defined byι(r) = (r)λ is an embedding of algebras and induces a ring morphism from K → C if, and only if, A is unitary (Lemma 14, [13]). Indeed, if A is unitary, (r)λ =r(1λ)λ is an element of A since A is a K-algebra, and ι is clearly an injective ring morphism. The converse is obvious. Moreover, if Λ is a directed set with partial order relation and if

(7) IA

(aλ)λA|lim

Λ aλ = 0

,

then the morphism ιis injective. Indeed, if (r)] = 0, relation (7) implies that the limit of the constant sequence (r)λ is null, thus r = 0.

2.2 Relationship with distribution theory and Colombeau algebras

One main feature of this construction is that we can choose the triple (C,E,P) such that the sheaves C andD are embedded in the corresponding sheafA. In particular, we can multiply (the images of) distributions inA.

We consider the sheafE= CoverRd, wherePis the usual family of topologies (P)Ω∈O(Rd).

HereO Rd

denotes the set of all open sets ofRd; this notation will be used in the sequel. Let us recall thatP is defined by the family of semi-norms (pK,l)K⋐Ω,l∈Nwith

∀f C(Ω), pK,l(f) = sup

x∈K,|α|≤l

|∂αf(x)|.

From Lemma 14 in [13], it follows that the canonical maps, defined for any Ω∈ O Rd by σ: C(Ω)→ H(A,E,P)(Ω) f 7→(f)λ,

are injective morphism of algebras if, and only if, A is unitary. Under this assumption, these maps give rise to a canonical sheaf embedding of C into H(A,E,P) and (using a partition of

(6)

unity in C inducing a sheaf structure on A) to a canonical sheaf morphism of algebras from C into A. This sheaf morphism turns out to be a sheaf morphism of embeddings if Λ is a directed set with respect to a partial order and if relation (7) holds.

We shall address the question of the embedding of D for the simple case of Λ = (0,1]. For a net (ϕε)ε of mollifiers given by

ϕε(x) = 1 εdϕx

ε

, xRd where ϕ∈ D(Rd) andR

ϕ(x)dx= 1, and T ∈ D Rd

, the net (Tϕε)ε is a net of smooth functions in C Rd

, moderately increasing in 1

ε. This means that

(8) ∀K Rd,∀lN, ∃mN: pK,l (T ϕε) = o(ε−m), asε0.

This justifies to choose A=n

(rε)εR(0,1] | ∃mN : |uε|= o(ε−m), asε0o I =n

(rε)εR(0,1]| ∀qN : |uε|= o(εq), asε0o .

In this case (withE = C), the sheaf of algebras A=H(A,E,P)/J(IA,E,P)is exactly the so-called special Colombeau algebraG [2, 7, 16]. Then, for all Ω∈ O Rd

, C(Ω) is embedded inA(Ω) by

σ : C(Ω)→ A(Ω) f 7→[fε] with fε=f for all εin (0,1], because the constant net (f)ε belongs to H(A,E,P) Rd

and (f)ε ∈ J(IA,E,P) implies f = 0 in C(Ω). Furthermore, D Rd

is embedded in A Rd

by the mapping ι:T 7→(T ϕε)ε

Indeed, relation (8) implies that (T ϕε)ε belongs to H(A,E,P) Rd

and (T ϕε)ε ∈ J(IA,E,P) implies thatTϕε0 inD Rd

, asε0 andT = 0. Thus,ιis a well defined injective map.

With the help of cutoff functions, we can define analogously, for each open set Ω in Rd, an embedding ι of D(Ω) into A(Ω), and finally a sheaf embedding D → A. This embedding depends on the choice of the net of mollifiers (ϕε)ε. We refer the reader to [3, 15] for more complete discussions about embeddings in Colombeau’s case and to [13] for the case of (C,E,P)- algebras.

2.3 An association process

We return to the general case with the assumption that A is unitary and Λ is a directed set with partial order relation .

Let us denote by:

Ω an open subset ofX,

• F a given sheaf (or presheaf) of topological K-vector spaces (resp. K-algebras) over X containing E as a subsheaf of topological algebras,

aa map from R+ to A+ such thata(0) = 1 (for rR+, we denote a(r) by (aλ(r))λ).

(7)

In the Colombeau case, a typical example would be aε(r) =εr,ε(0,1].

For (vλ)λ ∈ H(A,E,P)(Ω), we shall denote the limit of (vλ)λfor theF-topology by lim

Λ F(Ω)vλ

when it exists. We recall that lim

Λ F(V)uλ|V =f ∈ F(V) iff, for each F-neighborhoodW off, there existsλ0Λ such that

λλ0 = uλ|V W.

We suppose also that we have, for each open subsetV Ω,

(9) J(IA,E,P)(V)

(vλ)λ ∈ H(A,E,P)(V) : lim

Λ F(V)vλ = 0

.

Definition 2 Consider u= [uλ]∈ A(Ω), r R+, V an open subset of and f ∈ F(V). We say that u isa(r)-associated with f inV:

u a(r)

F(V)f if lim

Λ F(V)(aλ(r) uλ|V) =f.

In particular, if r = 0, u and f are called associated in V.

To ensure the independence of the definition with respect to the representative of u, we must have, for any (ηλ)λ ∈ J(IA,E,P)(Ω), that lim

Λ F(V)aλ(r) ηλ|V = 0. As J(IA,E,P)(V) is a module over A, (aλ(r) ηλ|V)λ is in J(IA,E,P)(V). Thus, our claim follows from hypothesis (9).

Example 1 Take X =Rd, F =D, Λ =]0,1], A=G, V = Ω, r = 0. The usual association between u= [uε]∈ G(Ω) and T ∈ D(Ω)is defined by

uT ⇐⇒u a(0)

D(Ω)T ⇐⇒ lim

ε→0D(Ω)uε=T.

2.4 The F-singular support of a generalized function

We use the notations of Subsection 2.3. According to the hypothesis (9), we have, for any open set Ω in X,

J(IA,E,P)(Ω)

(uλ)λ∈ H(A,E,P)(Ω) : lim

Λ F(V)uλ= 0

. Set

FA(Ω) =

u∈ A(Ω) | ∃(uλ)λu, ∃f ∈ F(Ω) : lim

Λ F(V)uλ=f

. FA(Ω) is well defined because if (ηλ)λ belongs to J(IA,E,P)(Ω), we have lim

Λ F(V)ηλ = 0.

Moreover, FA is a sub-presheaf of vector spaces (resp. algebras) of A. Roughly speaking, it is the presheaf whose sections above some open set Ω are the generalized functions of A(Ω) associated with an element of F(Ω).

Thus, for u∈ A(Ω), we can consider the set OFA(u) of allxΩ having an open neighbor- hoodV on whichu is associated with f ∈ F(V), that is:

OFA(u) ={x | ∃V ∈ Vx:u|V ∈ FA(V)}, Vx being the set of all the open neighborhoods of x.

This leads to the following definition:

(8)

Definition 3 TheF-singular support of u∈ A(Ω) is denoted SAF(u) and defined as SAF(u) = Ω\OFA(u).

Remark 3 (i) The validity of the gluing principle (F2) is not necessary to get the notion of support (and of F-singular support) of a section u ∈ A(Ω). More precisely, the localization principle (F1) is sufficient to prove the following: The set

OA{0}(u) ={x | ∃V ∈ Vx, u|V = 0}

is exactly the the union A(u) of the open subsets of on which u vanishes.

Indeed, (F1)allows to show that uvanishes on an open subsetO ofif, and only if, it vanishes on an open neighborhood of every point of O. This leads immediately to the required assertion.

Moreover,A(u) =O{0}A (u) is the largest open set on whichuvanishes, SA{0}(u) = Ω\O{0}A (u) is exactly the support ofu in its classical definition, and theF-singular support of uis a closed subset of its support.

(ii) In contrast to the situation described above for the support, we need the gluing principle (F2) if we want to prove that the restriction of u to OFA(u) belongs to FA(OFA(u)). We make this precise in the following lemma.

Lemma 4 Take u∈ A(Ω)and set FA(u) =i∈Ii,(Ωi)i∈I denoting the collection of the open subsets of such that u|i ∈ FA(Ωi). Then, if FA is a sheaf (even if Ais only a prehesaf ), (i) ΩFA(u) is the largest open subsetO of such that u|O belongs toFA(O);

(ii) ΩFA(u) =OAF(u) andSAF(u) = Ω\FA(u).

Proof. (i) ForiI, setu|i =fi∈ FA(Ωi). The family (fi)i∈I is coherent by assumption:

From (F2), there existsf ∈ FA(ΩFA(u)) such thatf|i =fi. But from (F1), we have f =u on

i∈Ii= ΩFA(u). Thusu|F

A(u) ∈ FA(ΩFA(u)), and ΩFA(u) is clearly the largest open subset of Ω having this property.

(ii) First,OFA(u) is clearly an open subset of Ω. Forx∈ OAF(u), setu|Vx =fx∈ FA(Vx) for some suitable neighborhoodVx. The open setOAF(u) can be covered by the family (Vx)x∈OF

A(u). As the family (fx) is coherent, we get from (F2) that there existsf ∈ FA

x∈OF

A(u)Vx

such that f|Vx =fx. From (F1), we have u =f on x∈OF

A(u)Vx and, therefore, u|OF

A(u) ∈ FA(OFA(u)).

Thus OAF(u) is contained in ΩFA(u). Conversely, if x FA(u), there exists an open neigh- borhood Vx of x such that u|Vx ∈ FA(Vx). Thus x ∈ OAF(u) and the assertion (ii) holds.

Proposition 5 For any u, v ∈ A(Ω), if F is a presheaf of topological vector spaces, (resp.

algebras), we have:

SAF(u+v)⊂ SAF(u)∪ SAF(v).

Moreover, in the resp. case, we have

SAF(uv)⊂ SAF(u)∪ SAF(v).

Proof. If x Ω belongs to OAF(u)∩ OFA(v), there exist V and W inVx such that u|V FA(V) and v|W ∈ FA(W). Thus (u+v)|V∩W ∈ FA(V W) (resp. (uv)|V∩W ∈ FA(V W)), which implies

OAF(u)∩ OAF(v)⊂ OFA(u+v) (resp. OFA(u)∩ OAF(v)⊂ OAF(uv) ).

The result follows by taking the complementary sets in Ω.

This proposition leads easily to the following:

(9)

Corollary 6 Let (uj)1≤j≤p be any finite family of elements in A(Ω). If F is a presheaf of topological vector spaces, (resp. algebras), we have

SAF( P

1≤j≤p

uj) S

1≤j≤p

SAF(uj).

Moreover, in the resp. case, we have SAF( Q

1≤j≤p

uj) S

1≤j≤p

SAF(uj).

In particular, if uj =u for 1j p, we have SAF(up)⊂ SAF(u).

Example 2 Taking E = C; F =D; A=G leads to the D-singular support of an element of the Colombeau algebra. This notion is complementary to the usual concept of local association in the Colombeau sense. We refer the reader to [12, 13] for more details.

Example 3 In the following examples we consider X=Rd, E = C and A=G.

(i) Take u σ(C(Ω)), where σ : C(Ω) → G(Ω) is the canonical embedding defined in Subsection 2.2. Then SGCp(u) =∅, for all pN.

(ii) Take ϕ∈ D(R), withR

ϕ(x) dx= 1, and set ϕε(x) =ε−1ϕ(x/ε). Asϕε ε→0

D−→(R)δ, we have:

SGD([ϕε]) ={0}. We note also that SGCp([ϕε]) = {0}. Indeed, for any K R =R\ {0} and ε small enough, ϕε is null on K and, therefore, ϕε ε→0

C−→(R)= 0.

(iii) Take u = [uε] with uε(x) = εsin(x/ε). We have that limpK,0(uε) = 0, for all K R, whereas limpK,1(uε) does not exist for l1. Therefore

SGC0(u) =, SGC1(u) =R.

Remark 4 For any (p, q)N2 with pq, andu∈ G, it holds that SGCp(u)⊂ SGCq(u).

3 The concept of (a,F)-microlocal analysis

Let Ω be an open set inX. Fixu= [uλ]∈ A(Ω) andx Ω. The idea of the (a,F)-microlocal analysis is the following: (uλ)λ may not tend to a section of F above a neighborhood of x, that is, there exists no V ∈ Vx and no f ∈ F(V) such that lim

Λ F(V)uλ = f. Nevertheless, in this case, there may exist V ∈ Vx, r 0 and f ∈ F(V) such that lim

Λ F(V)aλ(r)uλ = f, that is [aλ(r)uλ|V ] belongs to the subspace (resp. subalgebra) FA(V) of A(V) introduced in Subsection 2.4. These preliminary remarks lead to the following concept.

3.1 The (a,F)-singular parametric spectrum

We recall thatais a map fromR+ toA+such thata(0) = 1 andF is a presheaf of topological vector spaces (or topological algebras). For any open subset Ω of X, u = [uλ] ∈ A(Ω) and xΩ,set

N(a,F),x(u) =

rR+ | ∃V ∈ Vx, ∃f ∈ F(V) : lim

Λ F(V)(aλ(r)uλ|V ) =f

=n

r R+ | ∃V ∈ Vx : [aλ(r)uλ|V ]∈ FA(V)o .

It is easy to check thatN(a,F),x(u) does not depend on the representative of u. If no confusion may arise, we shall simply write

N(a,F),x(u) =Nx(u).

Références

Documents relatifs

We study microlocal limits of plane waves on noncompact Riemannian mani- folds (M, g) which are either Euclidean or asymptotically hyperbolic with curvature −1 near infinity.. The

For the algebra A of absolutely convergent Fourier series on T, Kahane ([7], pp. 39-43) has proved that the restriction algebra A(E) is generated by its idempotents whenever E is

We show that the generalized Radon transform arising in a model of pure industry taking into account the substitution of production factors at the micro-level is an integral

The main goal of this paper is to prove a formula that expresses the limit behaviour of Dedekind zeta functions for Re s > 1/2 in families of number fields, assuming that

The abelian core of the category of cocommutative Hopf algebras over a field of characteristic zero is the category of commutative and cocommutative Hopf algebras.. Roughly speaking

In [7] we have constructed sequence spaces forming algebras which correspond to Colombeau type algebras of ultradistributions and periodic hyper- functions.. The main objective of

I hope it adds some news ideas and results to the …xed point theory in the framework of generalized functions algebras, with application to the Cauchy-Lipschitz problem in a

After a short overview of classical results in distribution theory and propagation of singularities under linear and nonlinear operators, we will give a characterisation of the