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<rdf:Description rdf:about="https://omeka.ihes.fr/document/ZP6_1_7.jpg">
    <dcterms:title><![CDATA[Robert Oppenheimer et Léon Motchane lors de la conférece de presse]]></dcterms:title>
    <dcterms:subject><![CDATA[EVENEMENT OFFICIEL]]></dcterms:subject>
    <dcterms:subject><![CDATA[PERSONNALITE]]></dcterms:subject>
    <dcterms:creator><![CDATA[RAOUL-DUVAL]]></dcterms:creator>
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    <dcterms:date><![CDATA[16/05/1963]]></dcterms:date>
    <dcterms:rights><![CDATA[F. Raoul-Duval - Pleine Page]]></dcterms:rights>
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    <dcterms:coverage><![CDATA[1963]]></dcterms:coverage>
    <dcterms:rightsHolder><![CDATA[F. R. Duval - Pleine Page]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/ZP6_1_8.jpg">
    <dcterms:title><![CDATA[Robert Oppenheimer et Léon Motchane et deux administrateurs de l&#039;IHES, lors de la conférence de presse.]]></dcterms:title>
    <dcterms:subject><![CDATA[EVENEMENT OFFICIEL]]></dcterms:subject>
    <dcterms:subject><![CDATA[PERSONNALITE]]></dcterms:subject>
    <dcterms:subject><![CDATA[PAVILLON DE MUSIQUE]]></dcterms:subject>
    <dcterms:description><![CDATA[Ils font face aux journalistes]]></dcterms:description>
    <dcterms:creator><![CDATA[RAOUL-DUVAL]]></dcterms:creator>
    <dcterms:source><![CDATA[ZP6.1 (8)]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[16/05/1963]]></dcterms:date>
    <dcterms:rights><![CDATA[F. Raoul-Duval - Pleine Page]]></dcterms:rights>
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    <dcterms:coverage><![CDATA[1963]]></dcterms:coverage>
    <dcterms:rightsHolder><![CDATA[F. R. Duval - Pleine Page]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/ZP6_1_9.jpg">
    <dcterms:title><![CDATA[Robert Oppenheimer, Léon Motchane et deux administrateurs de l&#039;IHES lors de la conférence de presse]]></dcterms:title>
    <dcterms:subject><![CDATA[EVENEMENT OFFICIEL]]></dcterms:subject>
    <dcterms:subject><![CDATA[PERSONNALITE]]></dcterms:subject>
    <dcterms:subject><![CDATA[PAVILLON DE MUSIQUE]]></dcterms:subject>
    <dcterms:creator><![CDATA[RAOUL-DUVAL]]></dcterms:creator>
    <dcterms:source><![CDATA[ZP6.1 (9)]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[16/05/1963]]></dcterms:date>
    <dcterms:rights><![CDATA[F. Raoul-Duval - Pleine Page]]></dcterms:rights>
    <dcterms:accessRights><![CDATA[Autorisation à demander]]></dcterms:accessRights>
    <dcterms:license><![CDATA[BY]]></dcterms:license>
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    <dcterms:identifier><![CDATA[ZP6_1_9.jpg]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1963]]></dcterms:coverage>
    <dcterms:rightsHolder><![CDATA[F. R. Duval - Pleine Page]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://omeka.ihes.fr/document/H1_1_2_5_2_6.pdf">
    <dcterms:title><![CDATA[Rapport de David Ruelle sur son activité scientifique pour l&#039;année 1970-1971, novembre 1971]]></dcterms:title>
    <dcterms:subject><![CDATA[CONSEIL SCIENTIFIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[ACTIVITE SCIENTIFIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[PROFESSEUR PERMANENT]]></dcterms:subject>
    <dcterms:subject><![CDATA[SEMINAIRE]]></dcterms:subject>
    <dcterms:subject><![CDATA[PUBLICATION]]></dcterms:subject>
    <dcterms:subject><![CDATA[MECANIQUE STATISTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[CONFERENCE]]></dcterms:subject>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[H1.1.2.5.2/6]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:format><![CDATA[21x29,7]]></dcterms:format>
    <dcterms:format><![CDATA[2 f.]]></dcterms:format>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
    <dcterms:type><![CDATA[TEXTE]]></dcterms:type>
    <dcterms:type><![CDATA[RAPPORT]]></dcterms:type>
    <dcterms:identifier><![CDATA[H1_1_2_5_2_6.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1971]]></dcterms:coverage>
    <dcterms:rightsHolder><![CDATA[IHES]]></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_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_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_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_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_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_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_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_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_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_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_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_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_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_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_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_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_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_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/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_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/MP_75_106.pdf">
    <dcterms:title><![CDATA[Zeta-functions for expanding maps and Anosov flows]]></dcterms:title>
    <dcterms:subject><![CDATA[FONCTIONS ZETA]]></dcterms:subject>
    <dcterms:subject><![CDATA[FLOTS D&#039;ANOSOV]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : Given a real-analytic expanding endomorphism of a compact manifold M, a meromorphic zeta function is defined on the complex-valued real-analytic functions on M. A zeta function for Anosov flows is shown to be meromorphic if the flow and its stable-unstable foliations are real-analytic. ]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[MP/75/106]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[05/1975]]></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[MP_75_106.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/P_75_128.pdf">
    <dcterms:title><![CDATA[On Manifolds of phase coexistence]]></dcterms:title>
    <dcterms:subject><![CDATA[PHYSIQUE THEORIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE MATHEMATIQUE]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : Using a theorem on convex functions due to Israel, it is shown that a point of coexistence of n+1n+1 phases cannot be isolated in the space of interactions, but lies on some infinite dimensional manifold.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/75/128]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[12/1975]]></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_75_128.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/P_75_129.pdf">
    <dcterms:title><![CDATA[Probability estimates for continuous spin systems]]></dcterms:title>
    <dcterms:subject><![CDATA[PROBABILITES]]></dcterms:subject>
    <dcterms:subject><![CDATA[CENTRIFUGATION]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : Probability estimates for classical systems of particles with superstable interactions [1] are extended to continuous spin systems. ]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/75/129]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[12/1975]]></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_75_129.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/P_76_149.pdf">
    <dcterms:title><![CDATA[A Heuristic theory of phase transitions]]></dcterms:title>
    <dcterms:subject><![CDATA[RESEAUX]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES COMPLEXES]]></dcterms:subject>
    <dcterms:subject><![CDATA[ESPACES DE BANACH]]></dcterms:subject>
    <dcterms:subject><![CDATA[TRANSITIONS DE PHASE]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : Let Z be a suitable Banach space of interactions for a lattice spin system. If n+1 thermodynamic phases coexist for ?0 ?Z, it is shown that a manifold of codimension n of coexistence of (at least) n+1 phases passes through ?0. There are also n+1 manifolds of codimension n?1 of coexistence of (at least) n phases; these have a common boundary along the manifold of coexistence of n+1 phases. And so on for coexistence of fewer phases. This theorem is proved under a technical condition (R) which says that the pressure is a differentiable function of the interaction at ?0 when restricted to some codimensionn affine subspace of Z. The condition (R) has not been checked in any specific instance, and it is possible that our theorem is useless or vacuous. We believe however that the method of proof is physically correct and constitutes at least a heuristic proof of the Gibbs phase rule.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/76/149]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[10/1976]]></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_76_149.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1976]]></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_77_163.pdf">
    <dcterms:title><![CDATA[Applications conservant une mesure absolument continue par rapport à dx sur [0, 1]]]></dcterms:title>
    <dcterms:subject><![CDATA[FONCTIONS DIFFERENTIABLES]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE DE LA MESURE]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : Sufficient conditions are given such that a differentiable, noninvertible, map g : [0,1]~[0,1] leaves invariant a measure absolutely continuous with respect to the Lebesgue measure. In particular, this is shown to be the case for 9(x)=Rx(1- x) when R = 3,6785735 .... ]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/77/163]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[03/1977]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[6 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_77_163.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1977]]></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/PM_77_181.pdf">
    <dcterms:title><![CDATA[Integral representation of measures associated with a foliation]]></dcterms:title>
    <dcterms:subject><![CDATA[CALCUL INTEGRAL]]></dcterms:subject>
    <dcterms:subject><![CDATA[TOPOLOGIE DIFFERENTIELLE]]></dcterms:subject>
    <dcterms:subject><![CDATA[FEUILLETAGES]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE GEOMETRIQUE DES FONCTIONS]]></dcterms:subject>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[PM/77/181]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[05/1977]]></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[PM_77_181.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1977]]></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_77_189.pdf">
    <dcterms:title><![CDATA[Dynamical systems with turbulent behavior]]></dcterms:title>
    <dcterms:subject><![CDATA[CONGRES ET CONFERENCES]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES DYNAMIQUES]]></dcterms:subject>
    <dcterms:subject><![CDATA[ENTROPIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[RADON]]></dcterms:subject>
    <dcterms:description><![CDATA[[Text of a talk presented at the International Mathematical Physics Conference in Rome, 1977]]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/77/189]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[10/1977]]></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_77_189.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1977]]></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_77_190.pdf">
    <dcterms:title><![CDATA[Sensitive dependence on initial conditions and turbulent behavior of dynamical systems]]></dcterms:title>
    <dcterms:subject><![CDATA[SYSTEMES DYNAMIQUES]]></dcterms:subject>
    <dcterms:subject><![CDATA[DYNAMIQUE DIFFERENTIABLE]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : The asymptotic behavior of differentiable dynamical systems is analyzed. We discuss its descriptoin by asymptotic measures and the turbulent behavior with senditive dependence on initial condition.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/77/190]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[10/1977]]></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_77_190.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1977]]></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_77_193.pdf">
    <dcterms:title><![CDATA[Analiticity properties of the characteristic exponents of random matrix products]]></dcterms:title>
    <dcterms:subject><![CDATA[EXPOSANTS]]></dcterms:subject>
    <dcterms:subject><![CDATA[MATRICES]]></dcterms:subject>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/77/193]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[11/1977]]></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_77_193.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1977]]></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_78_214.pdf">
    <dcterms:title><![CDATA[The Multiplicative ergodic theorem]]></dcterms:title>
    <dcterms:subject><![CDATA[THEORIE ERGODIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES DYNAMIQUES]]></dcterms:subject>
    <dcterms:subject><![CDATA[DYNAMIQUE DIFFERENTIABLE]]></dcterms:subject>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/78/214]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[03/1978]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[12 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_78_214.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1978]]></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_78_240.pdf">
    <dcterms:title><![CDATA[Ergodic theory of differentiable dynamical systems]]></dcterms:title>
    <dcterms:subject><![CDATA[THEORIE ERGODIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES DYNAMIQUES]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEOREME]]></dcterms:subject>
    <dcterms:subject><![CDATA[EXPOSANTS]]></dcterms:subject>
    <dcterms:subject><![CDATA[VARIETES]]></dcterms:subject>
    <dcterms:subject><![CDATA[STABILITE]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : If f is a C1+? diffeomorphism of a compact manifold M, we prove the existence of stable manifolds, almost verywhere with respect to every f-invariant probability measure on M. These stable manifolds are smooth but do not in general constitute a continuous family. The proof of this stable manifold theorem (and similar results) is through the study of random matrix products (multiplicative ergodic theorem) and perturbation of such products. ]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/78/240]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[09/1978]]></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_78_240.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1978]]></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_78_245.pdf">
    <dcterms:title><![CDATA[On the Measures which describe turbulence]]></dcterms:title>
    <dcterms:subject><![CDATA[TURBULENCE]]></dcterms:subject>
    <dcterms:subject><![CDATA[HYDRODYNAMIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE ASYMPTOTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[HEURISTIQUE]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : One expects that the average behavior (over large times) for hydordynamics and other natural phenomena is described by certain asymptotic measures on phase space. If initial conditions in a set of zero Lebesgu measure ar discarded, the asymptotic measures can be characterized on the basis of heuristic arguments. The requirement of stability under small stochastic perturbations produces measures with the same characterizations. We give here a critical discussion of the heuristic arguments and of the possible use of the characterizations of the asymptotic measures in the study of turbulence.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/78/245]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[11/1978]]></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_78_245.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1978]]></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_79_313.pdf">
    <dcterms:title><![CDATA[Measures describing a turbulent flow]]></dcterms:title>
    <dcterms:subject><![CDATA[STABILITE]]></dcterms:subject>
    <dcterms:subject><![CDATA[PERTURBATION]]></dcterms:subject>
    <dcterms:subject><![CDATA[PROCESSUS STOCHASTIQUES]]></dcterms:subject>
    <dcterms:subject><![CDATA[TEMPS]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract :Recent attempts at understanding hydrodynamic turbulence have used the ideas of strange attractors, characteristic exponents and stable manifolds for differentiable dynamical systems in finite dimensional spaces. This use was somewhat metophorical, because hydrodynamic evolution is defined in infinite dimensional functional spaces. A recent study indicates that many results in infinite dimensional Hilbert spaces under certain compactness assumptions. This is the case in particular for the time evolution defined by the Navier-Stokes equations in a bounded region of R2 or R3.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/79/313]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[11/1979]]></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_79_313.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1979]]></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_80_11.pdf">
    <dcterms:title><![CDATA[Characteristic exponents and invariant manifolds in Hilbert space]]></dcterms:title>
    <dcterms:subject><![CDATA[THEORIE ERGODIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[MATHEMATIQUES]]></dcterms:subject>
    <dcterms:subject><![CDATA[VARIETES]]></dcterms:subject>
    <dcterms:subject><![CDATA[ESPACES DE HILBERT]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEOREMES]]></dcterms:subject>
    <dcterms:subject><![CDATA[TOPOLOGIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[VALEURS PROPRES]]></dcterms:subject>
    <dcterms:subject><![CDATA[FONCTIONS]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES SYNAMIQUES]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : The multiplicative ergodic theorem and the construction almost everywhere of stable and unstable manifolds (Pesin theory) are extended to differentiable dynamical systems on Hilbert manifolds under some compactness assumptions. The results apply to partial differential equations of evolution and also to non-invertible maps of compact manifolds.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/80/11]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[03/1980]]></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_80_11.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1980]]></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_81_23.pdf">
    <dcterms:title><![CDATA[Small random perturbations of dynamical systems and the definition of attractors]]></dcterms:title>
    <dcterms:subject><![CDATA[RESEAUX]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES DYNAMIQUES]]></dcterms:subject>
    <dcterms:subject><![CDATA[PHYSIQUE STATISTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYSTEMES COMPLEXES]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIES NON LINEAIRES]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : The strange attractors plotted by computers and seen in physical experiments do not necessarily have an open basin of attraction. In view of this we study a new definition of attractors based on ideas of Conley. We argue that the attractors observed in the presence of small random perturbations correspond to this new definition.]]></dcterms:description>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/81/23]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[03/1981]]></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_81_23.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1981]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
</rdf:Description></rdf:RDF>
