Titre : Comptes rendus de l'Académie des sciences. Série 1, Mathématique
Auteur : Académie des sciences (France). Auteur du texte
Éditeur : Elsevier (Paris)
Éditeur : Centrale des revuesCentrale des revues (Montrouge)
Éditeur : ElsevierElsevier (Paris)
Date d'édition : 1987-10-30
Notice du catalogue : http://catalogue.bnf.fr/ark:/12148/cb34394200t
Type : texte texte
Type : publication en série imprimée publication en série imprimée
Langue : français
Format : Nombre total de vues : 29122 Nombre total de vues : 29122
Description : 30 octobre 1987 30 octobre 1987
Description : 1987/10/30 (SER1,T305,N13). 1987/10/30 (SER1,T305,N13).
Droits : Consultable en ligne
Identifiant : ark:/12148/bpt6k54944143
Source : Archives de l'Académie des sciences, 2008-94315
Conservation numérique : Bibliothèque nationale de France
Date de mise en ligne : 01/12/2010
- Aller à la page de la table des matièresI
- CONTENTS 1987 - VOLUME 305 - SECTION I - N° 13
- .......... Page(s) .......... 569
- .......... Page(s) .......... 569
- Generalized linear programming techniques are extended to the mixed integer case. Implementation of branch and bound procedures leads to solving, in every node, a number of constrained column generation subproblems, according to the criterion of the dual simplex algorithm.
- .......... Page(s) .......... 573
- The paper shows that the information necessary to compute the successive powers of an ideal in a quadratic field is contained in a certain g-adic number, where g denotes the norm of the ideal. As an application we consider computing [n] P on an elliptic curve, for all n, when P is a given point on the curve.
- Let Q be a quadratic form with rational coefficients which is Q-isotropic and of signature (n, 1). Let be a congruence subgroup of SO(Q). The group acts on the n-dimensional hyperbolic space H; let be the smallest eigenvalue 0 of - on mod . We prove that cn, where c2=3/16, c3=3/4 and c=(2n-3)/4 for n4. This generalizes earlier results of Selberg and Sarnak for n=2 and n=3.
- .......... Page(s) .......... 583
- .......... Page(s) .......... 583
- Let K((t)) be the field of Laurent series in one indeterminate over a field K of characteristic different from 2 and let a be a non-square in K. It is proved that the minimal number of terms in a representation of -1 as a sum of squares in the quaternion algebra is min ((m(a)/2)+1, s(K(a))), where m(a) is the order of the quadratic form <1, -a> in the Witt group WK and s(K()) is the level of the field K(). Inparticular, this number, if finite, is either of the form 2 or of the form 2+1. This answers a question of D. Lewis [2].
- In [2], [3], Jimbo defines the q-analog U,g of the universal envelopping algebra of a C-Lie Algebra g and shows that, for g=gl(N+1), any irreducible finite dimensional representation of g can be deformed in an irreducible representation of U1g. We show that, for any simple Lie algebra g over C, all irreducible finite dimensional representations of U1g are essentially obtained in this way (after possibly tensoring by a I-dimensional representation).
- .......... Page(s) .......... 591
- .......... Page(s) .......... 591
- We show that for any non-degenerate critical point X0 of the regular part of Green's function relative to the Laplacian on , where is a smooth and bounded domain in RN, N5, there exists a family (
) of () such that on , and
concentrates around x0 as >0 goes to 0. We prove a converse to this result.
- We classify the nonnegative solutions of the equation with m, p>1 which vanish for t=0 except at x=0. Three different situations occur, depending on the value of p-m.
- .......... Page(s) .......... 599
- The Scharfetter-Gummel scheme, i. e. the most popular scheme for 1-dimensional semiconductor problems, is proved to be a classical mixed method, suitably interpreted. The same interpretation being valid in several variables, the Scharfetter-Gummel method can then be naturally extended to 2-d and 3-d problems, as it has been sought for longtime in the literature (see e.g. [6], [8]).
- .......... Page(s) .......... 605
- .......... Page(s) .......... 605
- We consider the evolution equation: in ; on ; y=0 on , where denotes a partition of the boundary and . Its stabilizability is studied, i. e. the existence of a feed-back F(y, y') such that, for given initial data, the solution y=y(x, t) decays exponentially in the energy space when t. If satisfies very strong geometrical hypotheses several authors have proved that the system is stabilized by the feed-back F(y')=-by' with if the partition is suitably chosen. We prove in this Note the stabilizability of the system without geometrical hypotheses for the case of dimension n=2, i. e. . The proof is based on the use of the feed-back F(y')=-by' with , b0 and b(x)=0 on the interface-points x and on the construction of energy functionals well adapted to the system.
- Differential Topology
- (see Tome 307, Series I, 1987, p. 609)
- .......... Page(s) .......... 617
- .......... Page(s) .......... 617
- Several theorems for a geometrical study of global attractors are given. And then a Baire-type theorem to relate the global (and static) aspect of attractors and their dynamical aspect.
- .......... Page(s) .......... 623
- We describe, for every value of the parameters (, ), the phase portrait of the family of differential equations ,
- (<0 and >0 fixed). This family plays an important role in the resonant elimination of couples of invariant curves of plane diffeomorphisms (see [1]).
- .......... Page(s) .......... 627
- We present asymptotic equivalents for P ; here is a sequence of independent
- identically distributed random variables (i.i.d.r.v.'s), and (xn)n is a real sequence satisfying .
- .......... Page(s) .......... 631
- We provide several characterizations of measurability for multifunctions defined on an abstract measurable space and whose values are weakly locally compact and contain no line, in a Lindelöf locally convex vector space. We especially give results about the existence of a measurable selection and of a Castaing's representation. Moreover, we show that, for this kind of multifunction, measurability is preserved under finite or countable intersection.
- .......... Page(s) .......... 635
- .......... Page(s) .......... 635
- We consider a controlled recurrent diffusion on . We study models where either the control or the observations or both are step functions on a sample interval. We prove the convergence of the stationary probabilities of these models to the stationary probability of the diffusion when the sampling interval goes to zero.
- Numerical Analysis
- (see Tome 307, Series I, 1987, p. 599)
- COMPTES RENDUS DE L'ACADEMIE DES SCIENCES MATHEMATIQUE 1987 - Tome 305 - Série I - n° 13 Contents with Enghish abstracts I-III
- .......... Page(s) .......... 569
- .......... Page(s) .......... 573
- .......... Page(s) .......... 591
- .......... Page(s) .......... 609
- Topologie différentielle
- (voir tome 307, série I, 1987, p. 609)
- Analyse numérique
- (voir tome 307, série I, 1987, p. 599)
- Les "Comptes Rendus de l'Académie des Sciences" figurent dans "Current Contents" et "Pascal"
C. R. Acad. Sci. Paris, t. 305, Série 1, p. 599-604, 1987 599
Equations aux dérivées partielles/Partia/ Differentiai Equations
(Analyse numérique/Numerical Analysis)
Méthodes d'éléments finis mixtes et schéma de
Scharfetter-Gummel
Franco BREZZI, Luisa Donatella MARINI et Paola PIETRA
Résumé — On démontre que la méthode de Scharfetter-Gummel (c'est-à-dire la méthode la plus
largement employée dans l'analyse des semi-conducteurs en dimension un) est une méthode mixte
de type classique, interprétée de façon convenable. Comme la même interprétation s'applique au
cas de plusieurs variables, cela donne la possibilité d'étendre la méthode de Scharfetter-Gummel à
deux et trois dimensions, ce qui était recherché depuis longtemps dans la littérature (cf. par
ex. [6], [8]).
Mixed finite élément methods and Scharfetter-Gummel scheme
Abstract — The Scharfetter-Gummel scheme, i. e. the most popular scheme for \-dimensional semi-
conductor problems, is proved to be a classical mixed method, suitably interpreted. The same
interprétation being valid in several variables, the Scharfetter-Gummel method can then be naturally
extended to 2-d and 3-d problems, as it has been sought for longtime in the literature (seee. g. [6], [8]).
Abridged English version — When dealing with semiconductor device problems, one has to
solve, among others, équations of the type:
where the function x(x) is considered hère as given, and 3Q = ri U T2. See, for instance,
[5L [7]- The change of variable
brings problem (o. 1) in the symmetric form:
provided that we assume dyjdn = o on T2-
The use of a non standard finite élément discretization for (0.3) (hybrid, mixed-hybrid etc.,
see [3]) will produce, in the end, a set of discrète équations in the unknown ph. By a suitable
inverse, transformation
one obtains discrète équations in the unknown uh. When applied to one-dimensional problems
(Q=]a, b[, T2 = 0) this procédure gives back the so-called Scharfetter-Gummel scheme (or
exponential fitting method), see [5], [9]. In more than one dimension, one has new schemes
Note présentée par Roland GLOWINSKI.
0249-6291/87/03050599 S 2.00 © Académie des Sciences
Equations aux dérivées partielles/Partia/ Differentiai Equations
(Analyse numérique/Numerical Analysis)
Méthodes d'éléments finis mixtes et schéma de
Scharfetter-Gummel
Franco BREZZI, Luisa Donatella MARINI et Paola PIETRA
Résumé — On démontre que la méthode de Scharfetter-Gummel (c'est-à-dire la méthode la plus
largement employée dans l'analyse des semi-conducteurs en dimension un) est une méthode mixte
de type classique, interprétée de façon convenable. Comme la même interprétation s'applique au
cas de plusieurs variables, cela donne la possibilité d'étendre la méthode de Scharfetter-Gummel à
deux et trois dimensions, ce qui était recherché depuis longtemps dans la littérature (cf. par
ex. [6], [8]).
Mixed finite élément methods and Scharfetter-Gummel scheme
Abstract — The Scharfetter-Gummel scheme, i. e. the most popular scheme for \-dimensional semi-
conductor problems, is proved to be a classical mixed method, suitably interpreted. The same
interprétation being valid in several variables, the Scharfetter-Gummel method can then be naturally
extended to 2-d and 3-d problems, as it has been sought for longtime in the literature (seee. g. [6], [8]).
Abridged English version — When dealing with semiconductor device problems, one has to
solve, among others, équations of the type:
where the function x(x) is considered hère as given, and 3Q = ri U T2. See, for instance,
[5L [7]- The change of variable
brings problem (o. 1) in the symmetric form:
provided that we assume dyjdn = o on T2-
The use of a non standard finite élément discretization for (0.3) (hybrid, mixed-hybrid etc.,
see [3]) will produce, in the end, a set of discrète équations in the unknown ph. By a suitable
inverse, transformation
one obtains discrète équations in the unknown uh. When applied to one-dimensional problems
(Q=]a, b[, T2 = 0) this procédure gives back the so-called Scharfetter-Gummel scheme (or
exponential fitting method), see [5], [9]. In more than one dimension, one has new schemes
Note présentée par Roland GLOWINSKI.
0249-6291/87/03050599 S 2.00 © Académie des Sciences
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