<rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:dcterms="http://purl.org/dc/terms/">
<rdf:Description rdf:about="https://omeka.ihes.fr/document/P_81_58.pdf">
    <dcterms:title><![CDATA[Symmetry in condensed matter physics]]></dcterms:title>
    <dcterms:subject><![CDATA[SYMETRIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[MATIERE CONDENSEE]]></dcterms:subject>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:source><![CDATA[P/81/58]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[11/1981]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[8 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_81_58.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1981]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_82_10.pdf">
    <dcterms:title><![CDATA[The Symmetry and renormalization group fixed points of quadratic hamiltonians]]></dcterms:title>
    <dcterms:subject><![CDATA[THEOREME DU POINT FIXE]]></dcterms:subject>
    <dcterms:subject><![CDATA[RENORMALISATION]]></dcterms:subject>
    <dcterms:subject><![CDATA[GROUPES DE SYMETRIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[OPERATEUR HAMILTONIEN]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : This paper studies the number and the nature of the fixed points of the renormalization group for the ?4 model, as used for instance in the Landau theory of second order phase transitions. It is shown that when it exists the stable fixed point is unique and a condition on its symmetry is given: it is often larger than the initial symmetry.<br />
Finally counter examples, with v arbitrarily large, are given to the Dzyaloshinskii conjecture that there exist no stable fixed points when the Landau potential depends on more than V = 3 parameters. ]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:source><![CDATA[P/82/10]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[03/1982]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[15 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_82_10.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1982]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_82_33.pdf">
    <dcterms:title><![CDATA[Représentation de vibration d&#039;un cristal construite par induction de représentations]]></dcterms:title>
    <dcterms:subject><![CDATA[CRISTALLOGRAPHIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[MATHEMATIQUES]]></dcterms:subject>
    <dcterms:subject><![CDATA[VIBRATIONS]]></dcterms:subject>
    <dcterms:subject><![CDATA[ANALYSE VECTORIELLE]]></dcterms:subject>
    <dcterms:description><![CDATA[Résumé : La représentation du groupe d&#039;espcace GK d&#039;un vecteur d&#039;onde k est le produit tensoriel de la représentation vectorielle du groupe ponctuel Pk de k et d&#039;une représentation induite donnée explicitement.<br />
L&#039;utilisation du théorème de réciprocité de Frobenius simplifie l&#039;étude de la décomposition de la représentation de vibration de Gk en somme directe de représentations irréductibles.]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:creator><![CDATA[MOZRZYMAS]]></dcterms:creator>
    <dcterms:source><![CDATA[P/82/33]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[06/1982]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[4 f.]]></dcterms:format>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_82_33.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1982]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MOZRZYMAS]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_82_54.pdf">
    <dcterms:title><![CDATA[The Structure of unitary representations of space groups]]></dcterms:title>
    <dcterms:subject><![CDATA[GROUPES SPATIAUX]]></dcterms:subject>
    <dcterms:subject><![CDATA[REPRESENTATIONS DE GROUPES]]></dcterms:subject>
    <dcterms:subject><![CDATA[CRISTALLOGRAPHIE]]></dcterms:subject>
    <dcterms:description><![CDATA[Lecture given by L. Michel at the XI-th International colloquium on Group Theoretical Methods in Physics at Istanbul, August 1982<br />
<br />
Abstract : For systems with a symmetry group G, the description of physical phenomena corresponding to a representation of G, depends only on the image of this representation.The classification of the images of the unirreps (unitary irreductible representations) of the little space groups Gk is remarkably simple. The nearly four thousands inequivalent unirreps corresponding to high symmetry wave vectors k have only 37 inequivalent images.]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:creator><![CDATA[MOZRZYMAS]]></dcterms:creator>
    <dcterms:source><![CDATA[P/82/54]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[10/1982]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[7 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_82_54.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1982]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MOZRZYMAS]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_83_20.pdf">
    <dcterms:title><![CDATA[Some Use of metabelian groups in physics]]></dcterms:title>
    <dcterms:subject><![CDATA[THEORIE DES GROUPES]]></dcterms:subject>
    <dcterms:subject><![CDATA[GROUPES RESOLUBLES]]></dcterms:subject>
    <dcterms:subject><![CDATA[CLASSIFICATION]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : Metabelian groups are those whose structure differ the least from Abelian groups. We explain the classification of finite metabelian groups and give some examples of physics problems where they play an important role.]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:creator><![CDATA[MOZRZYMAS]]></dcterms:creator>
    <dcterms:source><![CDATA[P/83/20]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[03/1983]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[8 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_83_20.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1983]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MOZRZYMAS]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_83_21.pdf">
    <dcterms:title><![CDATA[Landau theory of second order phase transitions and invariant theory]]></dcterms:title>
    <dcterms:subject><![CDATA[INVARIANTS]]></dcterms:subject>
    <dcterms:subject><![CDATA[POLYNOMES]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE DE LANDAU]]></dcterms:subject>
    <dcterms:subject><![CDATA[TRANSITIONS DE PHASES]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : We give some basic concepts on group actions and theorems in invariant theory useful for the contrcution and the study of Landau polynomials. We apply them to the study of the isotropy groups of extrema of Landau polynomials. We explain some technique for finding new extrema from old ones and we state some recent results concerning Landau theory of second order phase transitions.]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:source><![CDATA[P/83/21]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[03/1983]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[9 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_83_21.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1983]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_83_23.pdf">
    <dcterms:title><![CDATA[Zeros of covariant vector fields for the point groups : Invariant formulation]]></dcterms:title>
    <dcterms:subject><![CDATA[INVARIANTS]]></dcterms:subject>
    <dcterms:subject><![CDATA[ENSEMBLE DE POINTS]]></dcterms:subject>
    <dcterms:subject><![CDATA[MATHEMATIQUES]]></dcterms:subject>
    <dcterms:subject><![CDATA[ZERO]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE DES GROUPES]]></dcterms:subject>
    <dcterms:subject><![CDATA[ANALYSE VECTORIELLE]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE DES CHAMPS]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract. 2014 All finite as well as infinite (matrix) point subgroups of full orthogonal groups in two and three dimensions<br />
are considered. For each point group a polynomial integrity basis for invariants and the basic polynomial vector fields are first given. Then, the strata are defined via equations and inequalities involving the integrity basis. Finally, equations for zeros of a covariant vector field are given on each stratum in terms of the integrity basis, which appears via coefficients in the expansion of the vector field on the vector-field basis. All the results are tabulated and an illustration using the cubic group is presented. Mathematical background sufficient for extensions of the results is also given.<br />
<br />
Résumé. - Pour tous les groupes ponctuels (sous-groupes fermés) finis ou continus des groupes orthogonaux<br />
0(2) et 0(3) nous donnons une base d’intégrité e?(x) pour les polynômes invariants et pour les champs de vecteurs polynomiaux, nous donnons les équations et inégalités définissant les strates (union des orbites de même type). Finalement, nous écrivons des équations donnant les zéros d’un champ de vecteurs covariants sur une strate donnée; ces équations sont linéaires dans les composantes (invariantes) du champ de vecteurs sur les e?(x), les coefficients de ces termes étant eux-mêmes des invariants. Tous ces résultats sont résumés dans des tables et illustrés par un exemple d’application physique de symétrie cubique. La méthode mathématique pour obtenir ces résultats est expliquée de façon à permettre au lecteur de l’appliquer à d’autres groupes.]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:creator><![CDATA[JARIC]]></dcterms:creator>
    <dcterms:creator><![CDATA[SHARP]]></dcterms:creator>
    <dcterms:source><![CDATA[P/83/23]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[03/1983]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[47 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_83_23.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1983]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[JARIC]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[SHARP]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_83_35.pdf">
    <dcterms:title><![CDATA[Renormalization group fixed points of general n-vector models]]></dcterms:title>
    <dcterms:subject><![CDATA[RENORMALISATION]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEOREME DU POINT FIXE]]></dcterms:subject>
    <dcterms:subject><![CDATA[ANALYSE VECTORIELLE]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : We make a general study of symmetry and stability of the fixed points of the quartic Hamiltonian<br />
of an n-component field (or order parameter} for n&amp;4. Simple proofs of known results are given.<br />
Among new results, we shou that when it exists the stable fixed point is unique; we give some precision<br />
on its symmetry and on its attractor basin.]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:source><![CDATA[P/83/35]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[06/1983]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[14 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_83_35.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1983]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_83_56.pdf">
    <dcterms:title><![CDATA[Une Nouvelle et abondante source d&#039;énergie ?]]></dcterms:title>
    <dcterms:subject><![CDATA[RADIOACTIVITE ARTIFICIELLE]]></dcterms:subject>
    <dcterms:description><![CDATA[Article demandé pour le volume jubilaire du cinquantenaire de la découverte de la radioactivité articficielle]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:source><![CDATA[P/83/56]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[09/1983]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[9 f.]]></dcterms:format>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_83_56.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1983]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_83_66.pdf">
    <dcterms:title><![CDATA[L&#039;Unification de la physique]]></dcterms:title>
    <dcterms:subject><![CDATA[PHYSIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYMETRIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[HISTOIRE MODERNE ET CONTEMPORAINE]]></dcterms:subject>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:source><![CDATA[P/83/66]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[10/1983]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[8 f.]]></dcterms:format>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_83_66.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1983]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_83_67.pdf">
    <dcterms:title><![CDATA[Charge conjugation : a Contribution to the history of this internal quantum number of particle physics]]></dcterms:title>
    <dcterms:subject><![CDATA[PARTICULES]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE NUCLEAIRE]]></dcterms:subject>
    <dcterms:description><![CDATA[Conference given at the First International Meeting on the History of Scientific Ideas Symmetrie in Phyiscs, Sant Feliu de Guixols, Catalonia, Spain, September 20-26, 1983]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:source><![CDATA[P/83/67]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[11/1983]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[13 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_83_67.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1983]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_83_77.pdf">
    <dcterms:title><![CDATA[Mixing angles, B-meson life-time in the six quark model based on S0(10) × U(1)PQ]]></dcterms:title>
    <dcterms:subject><![CDATA[QUARKS]]></dcterms:subject>
    <dcterms:subject><![CDATA[MESONS]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : We show that a recently proposed multigenerational, grand unified model with three parameters (top-quark mass and two phases of Higgs vacuum expectation values) yields results in good agreement with the most recent phenomenological limits placed on the weak mixing angles of the quarks. These limits take into account the experimental value for B-meson life-time.]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:creator><![CDATA[NAIR]]></dcterms:creator>
    <dcterms:creator><![CDATA[WALI]]></dcterms:creator>
    <dcterms:source><![CDATA[P/83/77]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[12/1983]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[10 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_83_77.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1983]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[NAIR]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[WALI]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_84_43.pdf">
    <dcterms:title><![CDATA[Covariant vector fields and renormalization groups]]></dcterms:title>
    <dcterms:subject><![CDATA[GROUPE DE RENORMALISATION]]></dcterms:subject>
    <dcterms:subject><![CDATA[CHAMPS VECTORIELS]]></dcterms:subject>
    <dcterms:subject><![CDATA[ANALYSE DE COVARIANCE]]></dcterms:subject>
    <dcterms:description><![CDATA[Invited lecture given at th XIIIth international Colloquium on group theoretical methods on Physics]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:source><![CDATA[P/84/43]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[09/1984]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[13 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_84_43.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1984]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_85_27.pdf">
    <dcterms:title><![CDATA[Introduction to spontaneous symmetry breaking : some examples]]></dcterms:title>
    <dcterms:subject><![CDATA[PHYSIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYMETRIE BRISEE]]></dcterms:subject>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:source><![CDATA[P/85/27]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[04/1984]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[14 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_85_27.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1985]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_85_48.pdf">
    <dcterms:title><![CDATA[Symmetry and conservation laws in particle physics in the fifties]]></dcterms:title>
    <dcterms:subject><![CDATA[PARTICULES]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE NUCLEAIRE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYMETRIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[LOIS DE CONSERVATION]]></dcterms:subject>
    <dcterms:subject><![CDATA[ANNEES 1950]]></dcterms:subject>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:source><![CDATA[P/85/48]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[08/1985]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[10 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_85_48.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1985]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_85_68.pdf">
    <dcterms:title><![CDATA[What is a Crystal ?]]></dcterms:title>
    <dcterms:subject><![CDATA[CRISTAUX]]></dcterms:subject>
    <dcterms:subject><![CDATA[MATHEMATIQUES]]></dcterms:subject>
    <dcterms:subject><![CDATA[PAVAGE]]></dcterms:subject>
    <dcterms:subject><![CDATA[FONCTIONS]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : An historical survey of our knowledge of crystal structure and of the mathematical problem of paving space with one or a few types of stones show that a crystal has not necessarily a translation lattice. The recently discovered crystals of alloys Al with 14% Mn have an ecosahedral symetry (incompatible qith translation lattice). Their electron micrographs show a structure similar to a Penrose tiling. It seems that long range order characterizing crystals can be obtained from projection of a thin slab of genuine crystal in higher dimension so that crystal physical properties can be described by quasi-periodic functions (as generalizing periodic ones) or may be almost periodic functions.]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:source><![CDATA[P/85/68]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[12/1985]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[8 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_85_68.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1985]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_86_35.pdf">
    <dcterms:title><![CDATA[Structure and classification of band representations]]></dcterms:title>
    <dcterms:subject><![CDATA[CRISTALLOGRAPHIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SOLIDES]]></dcterms:subject>
    <dcterms:subject><![CDATA[ASTRONOMIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[ORBITE]]></dcterms:subject>
    <dcterms:subject><![CDATA[ETOILES]]></dcterms:subject>
    <dcterms:subject><![CDATA[MODELISATION]]></dcterms:subject>
    <dcterms:subject><![CDATA[ENERGIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[ATOMES]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : Band representaitons in solids are investigated in the general framework of induced representations by using the concepts of orbits (stars) and strata (Wyckoff positions) in their construction and classification. The connection between band representations and irreducible representations of space groups is established by reducing the former in the basis of quasi-Bloch functions wich are eigenfunctions of translations but ar not, in general, eigenfunctions of the Hamiltonian. While irreducible representations of space group ar fnite-dimensional and are induced from infinite-order little groups Gk for vectors K in the Brillouin zone, band representations are infinite-dimensional adn are induced from finite-order little groups Gr for vectors r in the Wigner-Seitz cell. This connection between irreductible representations and band representations of space groups shedd new light on the duality properties of the Brillouin zone and the Wigner-Seitz cell. As an introduction to band representations the induced representations of point groups wich id applied to the investigation of th equivalency of band representations. Based on this connection and on the properties of the crystallographic point groups a necessary condition id established for the inequivalency of band representations induced from maximal isotropy groups. For using this condition there is need fro the induced representaitons of oint groups and a full list of them is given in the paper. One is especially interested in irreducible-band representations which form the elementary building bricks for band representations. From the point of view of the physics, irreducible-band representations correspond to energy bands with minimal numbers of branches. A method id developped for finding all the inequivalent irreducible-band representations of space groups by using the induction from maximal isotropy groups. As a rule the latter leads to inequivalent irreducible-band representations. There are, however, few exceptions to this rule. A full list of such exceptions is tabulated in the paper. With this list at hand one can construct all the different irreducible-band representations of 2-dimensional space groups. For them we list the continuity chords of all their irreducible-band representations.]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:creator><![CDATA[BACRY]]></dcterms:creator>
    <dcterms:creator><![CDATA[ZAK]]></dcterms:creator>
    <dcterms:source><![CDATA[P/86/35]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[06/1986]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[46 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_86_35.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1986]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[BACRY]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[ZAK]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_87_42.pdf">
    <dcterms:title><![CDATA[Symmetry and classification of energy bands in crystals]]></dcterms:title>
    <dcterms:subject><![CDATA[SOLIDES]]></dcterms:subject>
    <dcterms:subject><![CDATA[CLASSIFICATION]]></dcterms:subject>
    <dcterms:subject><![CDATA[ENERGIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[GROUPES SPATIAUX]]></dcterms:subject>
    <dcterms:description><![CDATA[To appear in Proceedings XVth International Colloquium on Group Theretical Methods in Physics (Varna, June 1987)<br />
<br />
Abstract : An energy band in a solid contains an infinite number of states which transform linearly as a space group representation induced from a finite dimensional representation of the isotropy group of a point in space. A band representation is elementary if it cannot be decomposed as a direct sum of band representations; it describes a single band. We give a complete classification of the inequivalent elementary band representations.]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:creator><![CDATA[BACRY]]></dcterms:creator>
    <dcterms:creator><![CDATA[ZAK]]></dcterms:creator>
    <dcterms:source><![CDATA[P/87/42]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[10/1987]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[11 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_87_42.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1987]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[BACRY]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[ZAK]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_88_58.pdf">
    <dcterms:title><![CDATA[Les Concepts fondamentaux de la cristallographie]]></dcterms:title>
    <dcterms:subject><![CDATA[CRISTALLOGRAPHIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[MATHEMATIQUES]]></dcterms:subject>
    <dcterms:description><![CDATA[Résumé : Nous introduisons un nouvel ensemble de définitions des concepts de la cristallographie en dimension n. Il est basé sur les propriétés générales des actions de groupe. Enfin nous précison comment on détermine le systèmes cristallographique et la classe de Bravais d&#039;un groupe cristallographique.<br />
<br />
Abstract : We introduce a new set of definitions of the fundamental concepts of n-dimensional crystallography. It is based on general properties of group actions. We also show how to determine the crystallographic system and the Bravais class of a cristallographic group.]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:creator><![CDATA[MOZRZYMAS]]></dcterms:creator>
    <dcterms:source><![CDATA[P/88/58]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[11/1988]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[7 f.]]></dcterms:format>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_88_58.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1988]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MOZRZYMAS]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_89_73.pdf">
    <dcterms:title><![CDATA[Covariant symmetric non-associative algebras on group representations]]></dcterms:title>
    <dcterms:subject><![CDATA[REPRESENTATIONS DE GROUPES]]></dcterms:subject>
    <dcterms:subject><![CDATA[ALGEBRES NON ASSOCIATIVES]]></dcterms:subject>
    <dcterms:subject><![CDATA[ANALYSE DE COVARIANCE]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : When the vector space ? carries a representation p of the group G, if the decomposition of the symmetrized tensor product representation contains p, there exists a symmetrical non-associative algebra on ? with G a group of automorphisms. We give explicitly for dimension 2 (two maximal algebras). We also give several examples of th use of these algebras in physics and in mathematics.<br />
<br />
This paper will appear in part two of Symmetry in Nature, a volume in honour of Luigi Radicati di Brozolo, Sculoa Normale Superiore, Pisa, 1989]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:source><![CDATA[P/89/73]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[10/1989]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[9 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_89_73.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1989]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_70_05.pdf">
    <dcterms:title><![CDATA[Properties of the breaking of hadronic internal symmetry]]></dcterms:title>
    <dcterms:subject><![CDATA[SYMETRIE BRISEE]]></dcterms:subject>
    <dcterms:subject><![CDATA[MATHEMATIQUES]]></dcterms:subject>
    <dcterms:subject><![CDATA[HADRONS]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : The directions of breaking of the hadronic internal symmetry by the electromagnetic, semileptonic—and nonleptonic—weak and CP violating interactions are characterized by remarkable mathematical properties. These directions correspond to idempotents or nilpotents of an algebra and they are critical, i.e., every invariant function for the symmetry group, e.g., (SU(3) × SU(3)) × (1, P, C, PC) has an extremum on these directions.]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:creator><![CDATA[RADICATI]]></dcterms:creator>
    <dcterms:source><![CDATA[P/70/05]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[11/1970]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[18 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_70_05.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1970]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RADICATI]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_69_10.pdf">
    <dcterms:title><![CDATA[The Geometry of the Octet]]></dcterms:title>
    <dcterms:subject><![CDATA[SYMETRIE BRISEE]]></dcterms:subject>
    <dcterms:subject><![CDATA[GEOMETRIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[ALGEBRE]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : This is a preliminary version of chapter II and II of a paper on internal symmetries wich we are preparing. It contains a coordinate free formulation of SU(3) invariant algebras on the octet space.<br />
We calculate it now in the hope that it might be of help to the readers of the accompanying paper on SU(3)xSU(13) where the same formalism is used to discuss some physically interesting problems.<br />
We believe that the geometrical approach presented in these papers will help clarifying the relations and the properties of the fundamental interactions.<br />
It might be used for example to understand the geometrical basis of some recent attempts to compute Cabibbo&#039;s angle.]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:creator><![CDATA[RADICATI]]></dcterms:creator>
    <dcterms:source><![CDATA[P/69/10]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[[10/1969]]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[38 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_69_10.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1969]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RADICATI]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_69_11.pdf">
    <dcterms:title><![CDATA[Breaking of the SU(3) x SU(3) Symmetry in Hadronic Physics]]></dcterms:title>
    <dcterms:subject><![CDATA[SYMETRIE BRISEE]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[HADRONS]]></dcterms:subject>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:creator><![CDATA[RADICATI]]></dcterms:creator>
    <dcterms:source><![CDATA[P/69/11]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[[09/1969]]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[35 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_69_11.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1969]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RADICATI]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_69_X032.pdf">
    <dcterms:title><![CDATA[Applications of Group Theory to Quantum Physics : Algebraic Apects]]></dcterms:title>
    <dcterms:subject><![CDATA[THEORIE DES GROUPES]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE QUANTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[CONGRES ET CONFERENCES]]></dcterms:subject>
    <dcterms:subject><![CDATA[ATOMES]]></dcterms:subject>
    <dcterms:subject><![CDATA[MOLECULES]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE NUCLEAIRE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYMETRIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[HADRONS]]></dcterms:subject>
    <dcterms:description><![CDATA[Lectures given at the 1969 Battelle Summer Rencontres in Mathematics and Physics. Seattle - Washington - USA]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:source><![CDATA[P/69/X032]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[09/1969]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[97 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_69_X032.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1969]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_68_31.pdf">
    <dcterms:title><![CDATA[The Present Status of CP, T and CPT Invariance]]></dcterms:title>
    <dcterms:subject><![CDATA[PHYSIQUE NUCLEAIRE]]></dcterms:subject>
    <dcterms:subject><![CDATA[PARTICULES]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYMETRIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[INVARIANTS]]></dcterms:subject>
    <dcterms:description><![CDATA[Introduction : <br />
Last time I came to Sweden, cars were drivent on the left side of the roads. This week most cars I saw were driven on the right side. I am very grateful to the Nobel Foundation for this opportunity to observe this P violation. I may have found the cause of this P violation by looking at buses or trucks with the same inscription on both sides ; they are not symmetrically written.<br />
I have also made a couter-experiment to verify this theory. In Tokyo I found an equal probability for cars to be driven on the left side or the right side of the streets and I did observe that identical texts were placed symmetrically on buses and trucks : the first character is near the front part on both sides so the same text must be read from left to right on one side and from right to left on the other side.<br />
Since I have never been yet in a car undergoing a spontaneous CP transformation, I will be able to give you today my report on CP, T and CPT invariance.]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:source><![CDATA[P/68/31]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[[06/1968]]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[18 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_68_31.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1968]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_67_30.pdf">
    <dcterms:title><![CDATA[Matrices densité de polarisation]]></dcterms:title>
    <dcterms:subject><![CDATA[THEORIE QUANTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[MATRICES]]></dcterms:subject>
    <dcterms:subject><![CDATA[DENSITE]]></dcterms:subject>
    <dcterms:subject><![CDATA[CONGRES ET CONFERENCES]]></dcterms:subject>
    <dcterms:subject><![CDATA[POLARISATION]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE NUCLEAIRE]]></dcterms:subject>
    <dcterms:description><![CDATA[Ce manuscrit est un anti-résumé de la communication qui sera faite par l&#039;auteur à la rencontre des 17 et 18 novembre 1967, du groupe d&#039;étude du problème à 2 corps]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:source><![CDATA[P/67/30]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[[11/1967]]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[17 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_67_30.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1967]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/A3_1_3_7_5.pdf">
    <dcterms:title><![CDATA[Lettre du Ministère de l&#039;Education nationale demandant à Monsieur Motchane de signer la convention jointe concernant une subvention, avril 1968]]></dcterms:title>
    <dcterms:subject><![CDATA[SUBVENTION]]></dcterms:subject>
    <dcterms:subject><![CDATA[MINISTERE DE L&#039;EDUCATION NATIONALE]]></dcterms:subject>
    <dcterms:creator><![CDATA[MINISTERE DE L&#039;EDUCATION NATIONALE]]></dcterms:creator>
    <dcterms:source><![CDATA[A3.1.3.7.5]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[16/04/1968]]></dcterms:date>
    <dcterms:format><![CDATA[21x27]]></dcterms:format>
    <dcterms:format><![CDATA[3 f.]]></dcterms:format>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[CORRESPONDANCE]]></dcterms:type>
    <dcterms:identifier><![CDATA[A3_1_3_7_5.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1968]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/6H_NASH_1.pdf">
    <dcterms:title><![CDATA[Lettre de John Nash à Léon Motchane (1959)]]></dcterms:title>
    <dcterms:description><![CDATA[L.a.s. de John Nash à Léon Motchane acceptant son offre de venir à l&#039;IHES pour le 1er semestre 1960. Il décrit ensuite sa situation personnelle qui l&#039;a conduit à Genève.]]></dcterms:description>
    <dcterms:creator><![CDATA[MOTCHANE]]></dcterms:creator>
    <dcterms:source><![CDATA[6H/NASH/1]]></dcterms:source>
    <dcterms:date><![CDATA[1959]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[1 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[CORRESPONDANCE]]></dcterms:type>
    <dcterms:identifier><![CDATA[6H_NASH_1.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1959]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/6H_NASH_2.pdf">
    <dcterms:title><![CDATA[Lettre de Léon Motchane à John Nash (1959)]]></dcterms:title>
    <dcterms:description><![CDATA[Copie carbone de la lettre d&#039;invitation officielle de Léon Motchane à John Nash pour le premier semestre 1960.]]></dcterms:description>
    <dcterms:creator><![CDATA[MOTCHANE]]></dcterms:creator>
    <dcterms:source><![CDATA[6H/NASH/2]]></dcterms:source>
    <dcterms:date><![CDATA[04/12/1959]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[1 f.]]></dcterms:format>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[CORRESPONDANCE]]></dcterms:type>
    <dcterms:identifier><![CDATA[6H_NASH_2.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1959]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/6H_NASH_3.pdf">
    <dcterms:title><![CDATA[Lettre de Léon Motchane à Mme M. Lanchon (1959)]]></dcterms:title>
    <dcterms:description><![CDATA[Copie carbone d&#039;une lettre de Léon Motchane à Mme M. Lanchon (Direction des Affaires Culturelles, Quai d&#039;Orsay) lui demandant de délivrer un visa pour Nash depuis la Suisse.]]></dcterms:description>
    <dcterms:creator><![CDATA[MOTCHANE]]></dcterms:creator>
    <dcterms:source><![CDATA[6H/NASH/3]]></dcterms:source>
    <dcterms:date><![CDATA[04/12/1959]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[1 f.]]></dcterms:format>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[CORRESPONDANCE]]></dcterms:type>
    <dcterms:identifier><![CDATA[6H_NASH_3.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1959]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/6H_NASH_10.pdf">
    <dcterms:title><![CDATA[Lettre de Léon Motchane à John Nash (1964)]]></dcterms:title>
    <dcterms:description><![CDATA[Copie carbone d&#039;une lettre de Léon Motchane à John Nash l&#039;invitant pour un an à l&#039;IHES de septembre 1964 à août 1965.]]></dcterms:description>
    <dcterms:creator><![CDATA[MOTCHANE]]></dcterms:creator>
    <dcterms:source><![CDATA[6H/NASH/10]]></dcterms:source>
    <dcterms:date><![CDATA[11/06/1964]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[1 f.]]></dcterms:format>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[CORRESPONDANCE]]></dcterms:type>
    <dcterms:identifier><![CDATA[6H_NASH_10.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1964]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/M_77_167.pdf">
    <dcterms:title><![CDATA[Un Problème de topologie générale : le problème de Souslin]]></dcterms:title>
    <dcterms:subject><![CDATA[TOPOLOGIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE DES ENSEMBLES]]></dcterms:subject>
    <dcterms:subject><![CDATA[ENSEMBLES ORDONNES]]></dcterms:subject>
    <dcterms:creator><![CDATA[MOTCHANE]]></dcterms:creator>
    <dcterms:source><![CDATA[M/77/167]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[03/1977]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[32 f.]]></dcterms:format>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[M_77_167.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1977]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MOTCHANE]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/6H_NASH_4.pdf">
    <dcterms:title><![CDATA[Lettre de John Nash à Léon Motchane (1959-1960)]]></dcterms:title>
    <dcterms:description><![CDATA[L.a.s. de John Nash à Léon Motchane disant qu&#039;il a perdu sa lettre d&#039;invitation. Il explique qu&#039;il ne veut pas être associé officiellement avec l&#039;IHES.]]></dcterms:description>
    <dcterms:creator><![CDATA[NASH]]></dcterms:creator>
    <dcterms:source><![CDATA[6H/NASH/4]]></dcterms:source>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[1 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[CORRESPONDANCE]]></dcterms:type>
    <dcterms:identifier><![CDATA[6H_NASH_4.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1959-1960]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/6H_NASH_5.pdf">
    <dcterms:title><![CDATA[Lettre de John Nash à  Léon Motchane (1962)]]></dcterms:title>
    <dcterms:description><![CDATA[L.a.s. de John Nash à Léon Motchane disant qu&#039;il est prêt à accepter la demande de visite, que Leray a proposé à Motchane. Il ajoute avoir postulé sans succès à la NSF et attend la réponse de la Fondation Guggenheim.]]></dcterms:description>
    <dcterms:creator><![CDATA[NASH]]></dcterms:creator>
    <dcterms:source><![CDATA[6H/NASH/5]]></dcterms:source>
    <dcterms:date><![CDATA[13/03/1962]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[1 f.]]></dcterms:format>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[CORRESPONDANCE]]></dcterms:type>
    <dcterms:identifier><![CDATA[6H_NASH_5.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1962]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/6H_NASH_6.pdf">
    <dcterms:title><![CDATA[Lettre de Léon Motchane à John Nash (1962)]]></dcterms:title>
    <dcterms:description><![CDATA[Copie carbone d&#039;une lettre de Léon Motchane à John Nash expliquant qu&#039;il le recontactera s&#039;il peut l&#039;inviter en 1963.]]></dcterms:description>
    <dcterms:creator><![CDATA[NASH]]></dcterms:creator>
    <dcterms:source><![CDATA[6H/NASH/6]]></dcterms:source>
    <dcterms:date><![CDATA[22/03/1962]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[1 f.]]></dcterms:format>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[CORRESPONDANCE]]></dcterms:type>
    <dcterms:identifier><![CDATA[6H_NASH_6.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1962]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/6H_NASH_9.pdf">
    <dcterms:title><![CDATA[Lettre de John Nash à Alexandre Grothendieck (1964)]]></dcterms:title>
    <dcterms:description><![CDATA[L.a.s. de Nash à Alexandre Grothendieck le remerciant pour son invitation.]]></dcterms:description>
    <dcterms:creator><![CDATA[NASH]]></dcterms:creator>
    <dcterms:source><![CDATA[6H/NASH/9]]></dcterms:source>
    <dcterms:date><![CDATA[05/06/1964]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[1 f.]]></dcterms:format>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[CORRESPONDANCE]]></dcterms:type>
    <dcterms:identifier><![CDATA[6H_NASH_9.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1964]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/6H_NASH_11.pdf">
    <dcterms:title><![CDATA[Lettre de John Nash à Léon Motchane (1964)]]></dcterms:title>
    <dcterms:description><![CDATA[L.a.s. de  John Nash à Léon Motchane le remerciant pour son invitation. ]]></dcterms:description>
    <dcterms:creator><![CDATA[NASH]]></dcterms:creator>
    <dcterms:source><![CDATA[6H/NASH/11]]></dcterms:source>
    <dcterms:date><![CDATA[29/06/1964]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[1 f.]]></dcterms:format>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[CORRESPONDANCE]]></dcterms:type>
    <dcterms:identifier><![CDATA[6H_NASH_11.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1964]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/6H_NASH_12.pdf">
    <dcterms:title><![CDATA[Lettre de John Nash à Alexandre Grothendieck (1964)]]></dcterms:title>
    <dcterms:description><![CDATA[L.a.s. de John Nash à Alexandre Grothendieck disant qu&#039;il a eu son passeport et son ticket à bord du Queen Mary. Il pense aussi habiter chez une famille, plutôt qu&#039;à l&#039;IHES, afin d&#039;améliorer son français.]]></dcterms:description>
    <dcterms:creator><![CDATA[NASH]]></dcterms:creator>
    <dcterms:source><![CDATA[6H/NASH/12]]></dcterms:source>
    <dcterms:date><![CDATA[08/07/1964]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[1 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[CORRESPONDANCE]]></dcterms:type>
    <dcterms:identifier><![CDATA[6H_NASH_12.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1964]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_01_27.pdf">
    <dcterms:title><![CDATA[Noncommutative Field Theory]]></dcterms:title>
    <dcterms:subject><![CDATA[THEORIE QUANTIQUE DES CHAMPS]]></dcterms:subject>
    <dcterms:subject><![CDATA[ESPACE-TEMPS]]></dcterms:subject>
    <dcterms:subject><![CDATA[CINEMATIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[MODELES DES CORDES VIBRANTES]]></dcterms:subject>
    <dcterms:subject><![CDATA[SOLITONS]]></dcterms:subject>
    <dcterms:subject><![CDATA[INSTANTONS]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : We review the generalization of field theory to space-time with noncommuting coordinates, starting with the basics and covering most of the active directions of research. Such theories are now known to emerge from limits of M theory and string theory, and to describe quantum Hall states. In the last few years they have been studied intensively, and many qualitatively new phenomena have been discovered, both on the classical and quantum level. <br />
To appear in Reviews of Modern Physics.]]></dcterms:description>
    <dcterms:creator><![CDATA[NEKRASOV]]></dcterms:creator>
    <dcterms:creator><![CDATA[DOUGLAS]]></dcterms:creator>
    <dcterms:source><![CDATA[P/01/27]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[06/2001]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[31 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_01_27.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[2001]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[NEKRASOV]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[DOUGLAS]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_02_13.pdf">
    <dcterms:title><![CDATA[Milne Universe, Tachyons, and quantum group]]></dcterms:title>
    <dcterms:subject><![CDATA[MILNE]]></dcterms:subject>
    <dcterms:subject><![CDATA[TACHYONS]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE QUANTIQUE DES CHAMPS]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : We analyze the spectrum of the bosonic and superstring on the orbifold of the space-time by a boost, leading to the cosmological singularity. We show that the modular invariance leads to the spectrum where the twisted sector tachyon, together with all other twisted sector fields, present in the Euclidean version of the orbifold, is absent. This makes impossible to resolve the singularity by a marginal deformation of the worldsheet CFT. We also establish a relation between the resolution of rotational orbifolds in Euclidean and Lorentzian setups, and quantum groups. The analysis confirms the impossibility of resolving the cosmological orbifold singularity.]]></dcterms:description>
    <dcterms:creator><![CDATA[NEKRASOV]]></dcterms:creator>
    <dcterms:source><![CDATA[P/02/13]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[03/2002]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[9 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[P_02_13.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[2002]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[NEKRASOV]]></dcterms:rightsHolder>
</rdf:Description></rdf:RDF>
