<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_75_104.pdf">
    <dcterms:title><![CDATA[Generalized zeta-functions for axiom : a basic sets]]></dcterms:title>
    <dcterms:subject><![CDATA[FONCTIONS ZETA]]></dcterms:subject>
    <dcterms:subject><![CDATA[AXIOMES]]></dcterms:subject>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/75/104]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[03/1975]]></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_75_104.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1975]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/M_74_84.pdf">
    <dcterms:title><![CDATA[Currents, flows, and diffeomorphisms]]></dcterms:title>
    <dcterms:subject><![CDATA[DIFFEOMORPHISMES]]></dcterms:subject>
    <dcterms:subject><![CDATA[TOPOLOGIE DIFFERENTIELLE]]></dcterms:subject>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:creator><![CDATA[SULLIVAN]]></dcterms:creator>
    <dcterms:source><![CDATA[M/74/84]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[06/1974]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[24 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[PREPUBLICATION]]></dcterms:type>
    <dcterms:identifier><![CDATA[M_74_84.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1974]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[SULLIVAN]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_74_78.pdf">
    <dcterms:title><![CDATA[The Ergodic theory of axiom a flows]]></dcterms:title>
    <dcterms:subject><![CDATA[THEORIE ERGODIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[ENTROPIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[AXIOMES]]></dcterms:subject>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:creator><![CDATA[BOWEN]]></dcterms:creator>
    <dcterms:source><![CDATA[P/74/78]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[03/1974]]></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_74_78.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1974]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[BOWEN]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_72_29.pdf">
    <dcterms:title><![CDATA[Some Remarks on the location of zeroes of the partition function for lattice systems]]></dcterms:title>
    <dcterms:subject><![CDATA[RESEAUX]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES COMPLEXES]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES DYNAMIQUES]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES NON LINEAIRES]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE DES TREILLLIS]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : We use techniques which generalize the Lee-Yang circle theorem to investigate the distribution of zeroes of the partition function for various classes of classical lattice systems. ]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/72/29]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[1972]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[23 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_72_29.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1972]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_72_20.pdf">
    <dcterms:title><![CDATA[Bifurcations in the presence of a symmetry group]]></dcterms:title>
    <dcterms:subject><![CDATA[RESEAUX]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES COMPLEXES]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES DYNAMIQUES]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES NON LINEAIRES]]></dcterms:subject>
    <dcterms:subject><![CDATA[GROUPES DE SYMETRIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[ELECTROMAGNETISME]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : Let the origin O of a Banach space E be a fixed point of a diffeomorphism or a critical point of a vector, assuming equivariance under a linear group of isometries of E. Explicit techniques are presented to handle the generalization of the Hopf bifurcation to this equivariant situation.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/72/20]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[07/1972]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[33 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_72_20.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1972]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_72_08.pdf">
    <dcterms:title><![CDATA[Statistical mechanics on a compact set withe Z? action satisfying expansiveness and specification]]></dcterms:title>
    <dcterms:subject><![CDATA[MECANIQUE STATISTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE DES ENSEMBLES]]></dcterms:subject>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/72/08]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[07/1970]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[33 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_72_08.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1970]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_70_X036.pdf">
    <dcterms:title><![CDATA[On the Nature of turbulence]]></dcterms:title>
    <dcterms:subject><![CDATA[RESEAUX]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE STATISTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES COMPLEXES]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES DYNAMIQUES]]></dcterms:subject>
    <dcterms:subject><![CDATA[INFORMATIQUE QUANTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES NON LINEAIRES]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : A mechanism for the genetration of turbulence and related phenomena in dissipative systems is proposed.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:creator><![CDATA[TAKENS]]></dcterms:creator>
    <dcterms:source><![CDATA[P/70/X036]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[05/1970]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[16 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_X036.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1970]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[TAKENS]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_70_X035.pdf">
    <dcterms:title><![CDATA[Analiticity of Green&#039;s functions of dilute quantum gases]]></dcterms:title>
    <dcterms:subject><![CDATA[FONCTIONS DE GREEN]]></dcterms:subject>
    <dcterms:subject><![CDATA[GAZ]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE QUANTIQUE DES CHAMPS]]></dcterms:subject>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/70/X035]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[1970]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[5 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_X035.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1970]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_70_X033.pdf">
    <dcterms:title><![CDATA[Superstable interactions in classical statistical mechanics]]></dcterms:title>
    <dcterms:subject><![CDATA[RESEAUX]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE STATISTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[FONCTIONS CONTINUES]]></dcterms:subject>
    <dcterms:subject><![CDATA[FONCTIONS DE CORRELATION]]></dcterms:subject>
    <dcterms:subject><![CDATA[EQUILIBRE]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : We consider classical systems of particles inv dimensions. For a very large class of pair potentials (superstable lower regular potentials) it is shown that the correlation functions have bounds of the form ?(x1,...,xn)??n. Using these and further inequalities one can extend various results obtained by Dobrushin and Minlos [3] for the case of potentials which are non-integrably divergent at the origin. In particular it is shown that the pressure is a continuous function of the density. Infinite system equilibrium states are also defined and studied by analogy with the work of Dobrushin [2a] and of Lanford and Ruelle [11] for lattice gases.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/70/X033]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[1970]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[23 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_X033.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1970]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_70_X029.pdf">
    <dcterms:title><![CDATA[Integral representation of states on a C*-algebras]]></dcterms:title>
    <dcterms:subject><![CDATA[RESEAUX]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE STATISTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES COMPLEXES]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES DYNAMIQUES]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : Let E be the compact set of states on a C?-algebra U with identity. We discuss the representations of a state ? as barycenter of a probability measure ? on E. Examples of such representations are the central decomposition and the ergodic decomposition. They are associated with an Abelian von Neumann algebra B in the commutant ?(U)? of the image of U in the representation canonically associated with ?. This situation is studied in general and a number of applications are discussed.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/70/X029]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[1970]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[30 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_X029.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1970]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_69_30.pdf">
    <dcterms:title><![CDATA[Symmetry breakdown in statistical mechanics]]></dcterms:title>
    <dcterms:subject><![CDATA[SYMETRIE BRISEE]]></dcterms:subject>
    <dcterms:subject><![CDATA[MECANIQUE STATISTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[CONGRES ET CONFERENCES]]></dcterms:subject>
    <dcterms:description><![CDATA[Lecture given at the Ecole d&#039;Eté de Physique Théorique. Cargèse, Corsica, 1969.<br />
<br />
Abstract : We discuss the general problem of symmetry beakdown in the algebraic approach to statistical mechanics. We consider in particular the case of classical quantum lattice systems.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/69/30]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[1969]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[24 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_30.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1969]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_68_X022.pdf">
    <dcterms:title><![CDATA[Some Remarks on the ground state of infinite systems in statistical mechanics]]></dcterms:title>
    <dcterms:subject><![CDATA[MECANIQUE STATISTIQUE]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : We investigate the ground states of infinite quantum lattice systems. It is shown in particular that a positive energy operator is associated with these states. ]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/68/X022]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[1968]]></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_68_X022.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1968]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_67_X016.pdf">
    <dcterms:title><![CDATA[Statistical mechanics of a one-dimensional lattice gas]]></dcterms:title>
    <dcterms:subject><![CDATA[MECANIQUE STATISTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[RESEAUX]]></dcterms:subject>
    <dcterms:subject><![CDATA[GAZ]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : We study the statistical mechanics of an infinite one-dimensional classical lattice gas. Extending a result of Van Hove we show that, for a large class of interactions, such a system has no phase transition. The equilibrium state of the system is represented by a measure which is invariant under the effect of lattice translations. The dynamical system defined by this invariant measure is shown to be a K-system. ]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/67/X016]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[1967]]></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_67_X016.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1967]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_67_X015.pdf">
    <dcterms:title><![CDATA[Almost periodic states on C*-algebras *)]]></dcterms:title>
    <dcterms:subject><![CDATA[C*-ALGEBRES]]></dcterms:subject>
    <dcterms:subject><![CDATA[GROUPES D&#039;AUTOMORSPHISME]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : Given a C*-algebra O with a group of automorphisms, we define and study almost periodic states on O. A natural decomposition of such states is introduced and discussed. <br />
<br />
*) These notes are a result of discussions between S. Dpolicher, G. Gallavotti and D. Ruelle, they are not intended for publication.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/67/X015]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[1967]]></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_67_X015.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1967]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_67_X012.pdf">
    <dcterms:title><![CDATA[A Variational formulation of equilibrium statistical mechanics and the Gibbs phase rule]]></dcterms:title>
    <dcterms:subject><![CDATA[ENTROPIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[RESEAUX]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE STATISTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES COMPLEXES]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : It is shown that for an infinite lattice system, thermodynamic equilibrium is the solution of a variational problem involving a mean entropy of states introduced earlier [2]. As an application, a version of the Gibbs phase rule is proved.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/67/X012]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[1967]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[6 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_67_X012.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1967]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_66_X005.pdf">
    <dcterms:title><![CDATA[Condensation of lattice gases]]></dcterms:title>
    <dcterms:subject><![CDATA[RESEAUX]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE STATISTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES COMPLEXES]]></dcterms:subject>
    <dcterms:subject><![CDATA[CONDENSATION]]></dcterms:subject>
    <dcterms:subject><![CDATA[GAZ]]></dcterms:subject>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:creator><![CDATA[GINIBRE]]></dcterms:creator>
    <dcterms:creator><![CDATA[GROSSMANN]]></dcterms:creator>
    <dcterms:source><![CDATA[P/66/X005]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[1966]]></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_66_X005.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1966]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[GINIBRE]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[GROSSMANN]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_66_04.pdf">
    <dcterms:title><![CDATA[Mean entropy of States in classical statistical mechanics]]></dcterms:title>
    <dcterms:subject><![CDATA[ENTROPIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[RESEAUX]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE STATISTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES COMPLEXES]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : The equilibrium states for an infinite system of classical mechanics may be represented by states over Abelian C* algebras. We consider here continuous and lattice systems and define a mean entropy for their states. The properties of this mean entropy are investigated : linearity, upper semi-continuity, integral representations. In the lattice case, it is found that our mean entropy coincides with the KOLMOGOROV-SINAI invariant of ergodic theory.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:creator><![CDATA[ROBINSON]]></dcterms:creator>
    <dcterms:source><![CDATA[P/66/04]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[1966]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[25 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_66_04.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1966]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[ROBINSON]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_66_03.pdf">
    <dcterms:title><![CDATA[Integral représentations of invariant states on B*-algebras]]></dcterms:title>
    <dcterms:subject><![CDATA[INVARIANTS]]></dcterms:subject>
    <dcterms:subject><![CDATA[ALGEBRES]]></dcterms:subject>
    <dcterms:subject><![CDATA[GROUPES D&#039;AUTOMORPHISMES]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : Let ?? be a B* algebra with a group G of automorphisms and K be the set of G?invariant states on ??. We discuss conditions under which a G?invariant state has a unique integral representation in terms of extremal points of K, i.e., extremal invariant states.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:creator><![CDATA[LANFORD]]></dcterms:creator>
    <dcterms:source><![CDATA[P/66/03]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[1966]]></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_66_03.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1966]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[LANFORD]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_66_02.pdf">
    <dcterms:title><![CDATA[The States of classical statistical mechanics]]></dcterms:title>
    <dcterms:subject><![CDATA[MECANIQUE STATISTIQUE]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : a state of an infinite system in classical statistical mechanics is usually described by its correlation functions. We discuss here other description in particular as 1) a state on a B*-algebras, 2) a collection of density distributions, 3) a field theory 4) a mesure on a space of configurations of infitely many particles. We consier the relations between these various descriptions and prove under very general conditions an integral representation of a state as superposition of extremal invariant states corresponding to pure thermodynamical phases.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/66/02]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[1966]]></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_66_02.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1966]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_66_01.pdf">
    <dcterms:title><![CDATA[Extremal invariant states]]></dcterms:title>
    <dcterms:subject><![CDATA[INVARIANTS]]></dcterms:subject>
    <dcterms:subject><![CDATA[C*-ALGEBRES]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYMETRIE]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : A number of results are derived which are pertinent to the description of physical systems by states on C*-algebras invariants under a symmetry group. In particular an integral decomposition relevant to the study of lower symmetry is obtained which is occur in equilibrium statistical mechanics as existence of crystals, ferromagnetic states, etc... A characterization is given of strongly clustering euclidean invariant states, and it is shown that they cannot be decomposed into states of lower symmetry.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:creator><![CDATA[ROBINSON]]></dcterms:creator>
    <dcterms:source><![CDATA[P/66/01]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[1966]]></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_66_01.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1966]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[ROBINSON]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_65_03.pdf">
    <dcterms:title><![CDATA[The Stability of many-particle systems]]></dcterms:title>
    <dcterms:subject><![CDATA[THEORIE QUANTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[STABILITE]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : It is shown that a quantal or classical system of N particles of distinct species ?,? = 1, 2, … ? interacting through pair potentials ???(r) are stable, in the sense that the total energy is always bounded below by ?NB, provided ???(r) exceeds some ???(2)(r) whose Fourier transform ????(p)????(p) corresponds to a positive semidefinite ? × ? matrix for all p.<br />
This result is applied to discuss charged systems and stability is proved for Coulomb interactions if the charges are somewhat smeared rather than concentrated at points. For a large class of potentials it is shown that classical instability implies quantum instability in the case of bosons and, in three or more dimensions, also of fermions. Quantum systems with Coulomb interactions (point charges) are discussed and it is shown in particular that their stability cannot depend on the ratios between the masses of the particles.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:creator><![CDATA[FISHER]]></dcterms:creator>
    <dcterms:source><![CDATA[P/65/03]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[1965]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[17 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_65_03.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1965]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[FISHER]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_02_44.pdf">
    <dcterms:title><![CDATA[Seiberg-Witten prepotential from instanton counting]]></dcterms:title>
    <dcterms:subject><![CDATA[INVARIANTS DE SEIBERG-WITTEN]]></dcterms:subject>
    <dcterms:subject><![CDATA[CHAMPS DE JAUGE]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE DES CHAMPS]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : Direct evaluation of the Seiberg-Witten prepotential is accomplished following the localization programme suggested some time ago. Our results agree with all low-instanton calculations available in the literature. We present a two-parameter generalization of the Seiberg-Witten prepotential, which is rather natural from the M-theory/five dimensional perspective, and conjecture its relation to the tau-functions of KP/Toda hierarchy.<br />
<br />
To Arkady Vainshtein on his 60th anniversary<br />
]]></dcterms:description>
    <dcterms:creator><![CDATA[NEKRASOV]]></dcterms:creator>
    <dcterms:source><![CDATA[P/02/44]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[06/2002]]></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_02_44.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:Description rdf:about="https://omeka.ihes.fr/document/P_02_20.pdf">
    <dcterms:title><![CDATA[Target space symmetries in topological theories I.]]></dcterms:title>
    <dcterms:subject><![CDATA[TOPOLOGIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYMETRIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[ESPACE]]></dcterms:subject>
    <dcterms:subject><![CDATA[DIFFEOMORPHISMES]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE DES CHAMPS]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : We study realization of the target space diffeomorphisms in the type C topological string. We found that the charges, which generate transformations of the boundary observables, form an algebra, which differs from that of bulk charges by the contribution of the bubbled disks. We discuss applications to noncommutative field theories.]]></dcterms:description>
    <dcterms:creator><![CDATA[NEKRASOV]]></dcterms:creator>
    <dcterms:creator><![CDATA[BAULIEU]]></dcterms:creator>
    <dcterms:creator><![CDATA[LOSEV]]></dcterms:creator>
    <dcterms:source><![CDATA[P/02/20]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[03/2002]]></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_02_20.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>
    <dcterms:rightsHolder><![CDATA[BAULIEU]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[LOSEV]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/P_02_19.pdf">
    <dcterms:title><![CDATA[Noncommutative instantons revisited]]></dcterms:title>
    <dcterms:subject><![CDATA[INSTANTONS]]></dcterms:subject>
    <dcterms:subject><![CDATA[CHAMPS DE JAUGE]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : We find a new gauge in which U(1) noncommutative instantons are explicitly non-singular on noncommutative R^4. We also present a pedagogical introduction to the noncommutative gauge theories.]]></dcterms:description>
    <dcterms:creator><![CDATA[NEKRASOV]]></dcterms:creator>
    <dcterms:source><![CDATA[P/02/19]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[03/2002]]></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_02_19.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:Description rdf:about="https://omeka.ihes.fr/document/P_02_18.pdf">
    <dcterms:title><![CDATA[Trieste lectures on solitons in noncommutative Gauge theories]]></dcterms:title>
    <dcterms:subject><![CDATA[CHAMPS DE JAUGE]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SOLITONS]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : We present a pedagogical introduction into noncommutative gauge theories, their stringy origin, and non-perturbative effects, including monopole and instanton solutions.]]></dcterms:description>
    <dcterms:creator><![CDATA[NEKRASOV]]></dcterms:creator>
    <dcterms:source><![CDATA[P/02/18]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[03/2002]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[34 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_18.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:Description rdf:about="https://omeka.ihes.fr/document/P_02_14.pdf">
    <dcterms:title><![CDATA[Lectures on open strings, and noncommutative Gauge theories]]></dcterms:title>
    <dcterms:subject><![CDATA[CHAMPS DE JAUGE]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[MODELES DES CORDES VIBRANTES]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract :The background independent formulation of the gauge theories on D-branes in flat space-time is considered, some examples of the solutions of their equations of motion are presented, the solutions of Dirac equation in these backgrounds are analyzed, and the generalizations to the curved spaces, like orbifolds, conifolds, and K3 surfaces are discussed.]]></dcterms:description>
    <dcterms:creator><![CDATA[NEKRASOV]]></dcterms:creator>
    <dcterms:source><![CDATA[P/02/14]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[03/2002]]></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_02_14.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: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: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/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/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/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_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_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_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_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_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_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_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_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_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:RDF>
