<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://archives.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://archives.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://archives.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://archives.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://archives.ihes.fr/document/P_97_54.pdf">
    <dcterms:title><![CDATA[Rydberg states of atoms and molecules. Basic group theoretical and topological analysis]]></dcterms:title>
    <dcterms:subject><![CDATA[ETATS DE RYDBERG]]></dcterms:subject>
    <dcterms:subject><![CDATA[ATOMES]]></dcterms:subject>
    <dcterms:subject><![CDATA[HYDROGENE]]></dcterms:subject>
    <dcterms:subject><![CDATA[CHAMPS ELECTROMAGNETIQUES]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : Rydberg states of atoms and molecules are studied within the qualitative approach-based primarily on topological and group theoretical analysis. The correspondence between classical and quantum mechanics is explored to apply the results of qualitative (topological) approach to classical mechanics developed by Poincaré, Lyapounov and Smale to quantum problems. The study of the action of the symmetry group of the problems considered on the classical phase space enables us to predict qualitative features of the energy level patterns for quantum Rydberg operators.]]></dcterms:description>
    <dcterms:creator><![CDATA[MICHEL]]></dcterms:creator>
    <dcterms:creator><![CDATA[ZHILINSKII]]></dcterms:creator>
    <dcterms:source><![CDATA[P/97/54]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[07/1997]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[41 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_97_54.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1997]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[MICHEL]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[ZHILINSKII]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://archives.ihes.fr/document/P_69_12.pdf">
    <dcterms:title><![CDATA[Observables at Infinity and States with Short Range : Correlations in Statistical Mechanics]]></dcterms:title>
    <dcterms:subject><![CDATA[MECANIQUE STATISTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[FONCTIONS DE CORRELATION]]></dcterms:subject>
    <dcterms:subject><![CDATA[INFORMATIQUE QUANTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE DES TREILLIS]]></dcterms:subject>
    <dcterms:description><![CDATA[Abstract : We say that a representation of an algebra of local observables has short-range correlations if any observable which can be measured outside all bounded sets is a multiple of the identity, and that a state has finite range correlations if the corresponding cyclic representation does. We characterize states with short-range correlations by a cluster property. For classical lattice systems and continuous systems with hard cores, we give a definition of equilibrium state for a specific interaction, based on a local version of the grand canonical prescription; an equilibrium state need not be translation invariant. We show that every equilibrium state has a unique decomposition into equilibrium states with short-range correlations. We use the properties of equilibrium states to prove some negative results about the existence of metastable states. We show that the correlation functions for an equilibrium state satisfy the Kirkwood-Salsburg equations; thus, at low activity, there is only one equilibrium state for a given interaction, temperature, and chemical potential. Finally, we argue heuristically that equilibrium states are invariant under time-evolution.]]></dcterms:description>
    <dcterms:creator><![CDATA[LANDFORD]]></dcterms:creator>
    <dcterms:creator><![CDATA[RUELLE]]></dcterms:creator>
    <dcterms:source><![CDATA[P/69/12]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[[06/1969]]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[42 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_12.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1969]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[LANFORD]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[RUELLE]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://archives.ihes.fr/document/P_00_44.pdf">
    <dcterms:title><![CDATA[Return to equilibrium]]></dcterms:title>
    <dcterms:subject><![CDATA[GROUPE DE RENORMALISATION]]></dcterms:subject>
    <dcterms:subject><![CDATA[EQUILIBRE THERMODYNAMIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[RAYONNEMENT DU CORPS NOIR]]></dcterms:subject>
    <dcterms:subject><![CDATA[KMS]]></dcterms:subject>
    <dcterms:creator><![CDATA[FROHLICH]]></dcterms:creator>
    <dcterms:creator><![CDATA[BACH]]></dcterms:creator>
    <dcterms:creator><![CDATA[SIGAL]]></dcterms:creator>
    <dcterms:source><![CDATA[P/00/44]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[06/2000]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[53 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_00_44.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[2000]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[FROHLICH]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[BACH]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[SIGAL]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://archives.ihes.fr/document/P_93_59.pdf">
    <dcterms:title><![CDATA[Conformal field theory and geometry of strings]]></dcterms:title>
    <dcterms:subject><![CDATA[QUANTIFICATION GEOMETRIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE DES CHAMPS]]></dcterms:subject>
    <dcterms:subject><![CDATA[GEOMETRIE DIFFERENTIELLE NON COMMUTATIVE]]></dcterms:subject>
    <dcterms:subject><![CDATA[PRINCIPE DE DUALITE]]></dcterms:subject>
    <dcterms:subject><![CDATA[SYMETRIE MIROIR]]></dcterms:subject>
    <dcterms:creator><![CDATA[FROHLICH]]></dcterms:creator>
    <dcterms:creator><![CDATA[GAWEDZKI]]></dcterms:creator>
    <dcterms:source><![CDATA[P/93/59]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[11/1993]]></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_93_59.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1993]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[FROHLICH]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[GAWEDZKI]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://archives.ihes.fr/document/P_78_243.pdf">
    <dcterms:title><![CDATA[The Charge sectors of quantum electrodynamics in a framework of local observables]]></dcterms:title>
    <dcterms:subject><![CDATA[ELECTRODYNAMIQUE QUANTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[ALGEBRE]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE DES CHAMPS]]></dcterms:subject>
    <dcterms:subject><![CDATA[THEORIE DES JAUGES]]></dcterms:subject>
    <dcterms:subject><![CDATA[GROUPES DE LORENTZ]]></dcterms:subject>
    <dcterms:creator><![CDATA[FROHLICH]]></dcterms:creator>
    <dcterms:source><![CDATA[P/78/243]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[10/1978]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[36 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_243.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1978]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[FROHLICH]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://archives.ihes.fr/document/P_99_54.pdf">
    <dcterms:title><![CDATA[Self-gravitating fundamental strings and black holes]]></dcterms:title>
    <dcterms:subject><![CDATA[MODELES DES CORDES VIBRANTES]]></dcterms:subject>
    <dcterms:subject><![CDATA[TROUS NOIRS]]></dcterms:subject>
    <dcterms:subject><![CDATA[GRAVITATION]]></dcterms:subject>
    <dcterms:creator><![CDATA[DAMOUR]]></dcterms:creator>
    <dcterms:creator><![CDATA[VENEZIANO]]></dcterms:creator>
    <dcterms:source><![CDATA[P/99/54]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[07/1999]]></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_99_54.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1999]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[DAMOUR]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[VENEZIANO]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://archives.ihes.fr/document/P_98_44.pdf">
    <dcterms:title><![CDATA[Pre-Big bang bubbles from the gravitational instability of generic string vacua]]></dcterms:title>
    <dcterms:subject><![CDATA[COSMOLOGIE]]></dcterms:subject>
    <dcterms:subject><![CDATA[MODELES DES CORDES VIBRANTES]]></dcterms:subject>
    <dcterms:subject><![CDATA[GRAVITATION]]></dcterms:subject>
    <dcterms:subject><![CDATA[STABILITE]]></dcterms:subject>
    <dcterms:subject><![CDATA[TROUS NOIRS]]></dcterms:subject>
    <dcterms:subject><![CDATA[ESPACE-TEMPS]]></dcterms:subject>
    <dcterms:subject><![CDATA[INFLATION]]></dcterms:subject>
    <dcterms:creator><![CDATA[DAMOUR]]></dcterms:creator>
    <dcterms:creator><![CDATA[BUONANNO]]></dcterms:creator>
    <dcterms:creator><![CDATA[VENEZIANO]]></dcterms:creator>
    <dcterms:source><![CDATA[P/98/44]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[06/1998]]></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_98_44.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1998]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[DAMOUR]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[BUONANNO]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[VENEZIANO]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://archives.ihes.fr/document/P_96_01.pdf">
    <dcterms:title><![CDATA[Selected themes in relativistic gravity]]></dcterms:title>
    <dcterms:subject><![CDATA[GRAVITATION]]></dcterms:subject>
    <dcterms:subject><![CDATA[RELATIVITE GENERALE]]></dcterms:subject>
    <dcterms:creator><![CDATA[DAMOUR]]></dcterms:creator>
    <dcterms:source><![CDATA[P/96/01]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[01/1996]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[19 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_96_01.pdf]]></dcterms:identifier>
    <dcterms:coverage><![CDATA[1996]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
    <dcterms:rightsHolder><![CDATA[IHES]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[DAMOUR]]></dcterms:rightsHolder>
</rdf:Description><rdf:Description rdf:about="https://archives.ihes.fr/document/P_95_101.pdf">
    <dcterms:title><![CDATA[Theoretical aspects of gravitational radiation]]></dcterms:title>
    <dcterms:subject><![CDATA[RAYONNEMENT GRAVITATIONNEL]]></dcterms:subject>
    <dcterms:subject><![CDATA[CALCULS NUMERIQUES]]></dcterms:subject>
    <dcterms:subject><![CDATA[DETECTEURS]]></dcterms:subject>
    <dcterms:subject><![CDATA[DETECTEURS DE RAYONNEMENT]]></dcterms:subject>
    <dcterms:subject><![CDATA[TROUS NOIRS]]></dcterms:subject>
    <dcterms:creator><![CDATA[DAMOUR]]></dcterms:creator>
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    <dcterms:title><![CDATA[Gravitational waves and cosmology]]></dcterms:title>
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    <dcterms:date><![CDATA[06/1995]]></dcterms:date>
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    <dcterms:title><![CDATA[Conservation laws for sysmems of extended  bodies in the first post-Newtonian approximation]]></dcterms:title>
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    <dcterms:subject><![CDATA[CALCULS NUMERIQUES]]></dcterms:subject>
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    <dcterms:creator><![CDATA[VOKROUHLICKY]]></dcterms:creator>
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</rdf:Description><rdf:Description rdf:about="https://archives.ihes.fr/document/P_92_87.pdf">
    <dcterms:title><![CDATA[General relativistic celestial mechanics. III - Rotational equations of motion]]></dcterms:title>
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    <dcterms:subject><![CDATA[EQUATIONS DU MOUVEMENT]]></dcterms:subject>
    <dcterms:subject><![CDATA[RELATIVITE GENERALE]]></dcterms:subject>
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    <dcterms:creator><![CDATA[SOFFEL]]></dcterms:creator>
    <dcterms:creator><![CDATA[XU]]></dcterms:creator>
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    <dcterms:date><![CDATA[11/1992]]></dcterms:date>
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    <dcterms:format><![CDATA[13 f.]]></dcterms:format>
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</rdf:Description><rdf:Description rdf:about="https://archives.ihes.fr/document/P_92_42.pdf">
    <dcterms:title><![CDATA[Hereditary effects in gravitational radiation]]></dcterms:title>
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    <dcterms:creator><![CDATA[BLANCHET]]></dcterms:creator>
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    <dcterms:date><![CDATA[07/1992]]></dcterms:date>
    <dcterms:format><![CDATA[A4]]></dcterms:format>
    <dcterms:format><![CDATA[17 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
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    <dcterms:coverage><![CDATA[1992]]></dcterms:coverage>
    <dcterms:provenance><![CDATA[IHES]]></dcterms:provenance>
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    <dcterms:title><![CDATA[General relativistic celestial mechanics. II - Translational equations of motion]]></dcterms:title>
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    <dcterms:subject><![CDATA[RELATIVITE GENERALE]]></dcterms:subject>
    <dcterms:subject><![CDATA[EQUATIONS DU MOUVEMENT]]></dcterms:subject>
    <dcterms:creator><![CDATA[DAMOUR]]></dcterms:creator>
    <dcterms:creator><![CDATA[SOFFEL]]></dcterms:creator>
    <dcterms:creator><![CDATA[XU]]></dcterms:creator>
    <dcterms:source><![CDATA[P/91/72]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[10/1991]]></dcterms:date>
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    <dcterms:format><![CDATA[40 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
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    <dcterms:coverage><![CDATA[1991]]></dcterms:coverage>
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</rdf:Description><rdf:Description rdf:about="https://archives.ihes.fr/document/P_90_87.pdf">
    <dcterms:title><![CDATA[General relativistic celestial mechanics. I - Method and definition of reference systems]]></dcterms:title>
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    <dcterms:subject><![CDATA[RELATIVITE GENERALE]]></dcterms:subject>
    <dcterms:subject><![CDATA[METHODOLOGIE]]></dcterms:subject>
    <dcterms:creator><![CDATA[DAMOUR]]></dcterms:creator>
    <dcterms:creator><![CDATA[SOFFEL]]></dcterms:creator>
    <dcterms:creator><![CDATA[XU]]></dcterms:creator>
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    <dcterms:date><![CDATA[11/1990]]></dcterms:date>
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    <dcterms:format><![CDATA[41 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
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    <dcterms:coverage><![CDATA[1990]]></dcterms:coverage>
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    <dcterms:title><![CDATA[Post-Newtonian generation of gravitational waves II. The Spin moments]]></dcterms:title>
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    <dcterms:subject><![CDATA[SPIN]]></dcterms:subject>
    <dcterms:subject><![CDATA[CHAMPS GRAVITATIONNELS]]></dcterms:subject>
    <dcterms:subject><![CDATA[CALCUL TENSORIEL]]></dcterms:subject>
    <dcterms:creator><![CDATA[DAMOUR]]></dcterms:creator>
    <dcterms:creator><![CDATA[IYER]]></dcterms:creator>
    <dcterms:source><![CDATA[P/90/85]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[10/1990]]></dcterms:date>
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    <dcterms:format><![CDATA[32 f.]]></dcterms:format>
    <dcterms:language><![CDATA[EN]]></dcterms:language>
    <dcterms:language><![CDATA[FR]]></dcterms:language>
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    <dcterms:title><![CDATA[Levi-Civita and the general relativistic problem of motion]]></dcterms:title>
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    <dcterms:subject><![CDATA[RELATIVITE GENERALE]]></dcterms:subject>
    <dcterms:subject><![CDATA[MECANIQUE ANALYTIQUE]]></dcterms:subject>
    <dcterms:subject><![CDATA[MOUVEMENT]]></dcterms:subject>
    <dcterms:creator><![CDATA[DAMOUR]]></dcterms:creator>
    <dcterms:creator><![CDATA[SCHAFER]]></dcterms:creator>
    <dcterms:source><![CDATA[P/90/60]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[07/1990]]></dcterms:date>
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    <dcterms:format><![CDATA[7 f.]]></dcterms:format>
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    <dcterms:coverage><![CDATA[1990]]></dcterms:coverage>
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    <dcterms:title><![CDATA[Post-Newtonian generation of gravitational waves]]></dcterms:title>
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    <dcterms:subject><![CDATA[RELATIVITE GENERALE]]></dcterms:subject>
    <dcterms:subject><![CDATA[CHAMPS GRAVITATIONNELS]]></dcterms:subject>
    <dcterms:creator><![CDATA[DAMOUR]]></dcterms:creator>
    <dcterms:creator><![CDATA[BLANCHET]]></dcterms:creator>
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    <dcterms:date><![CDATA[03/1989]]></dcterms:date>
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    <dcterms:language><![CDATA[FR]]></dcterms:language>
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    <dcterms:title><![CDATA[Characterizing volume forms]]></dcterms:title>
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    <dcterms:subject><![CDATA[THEORIE QUANTIQUE DES CHAMPS]]></dcterms:subject>
    <dcterms:subject><![CDATA[GEOMETRIE DIFFERENTIELLE]]></dcterms:subject>
    <dcterms:creator><![CDATA[CARTIER]]></dcterms:creator>
    <dcterms:creator><![CDATA[BERG]]></dcterms:creator>
    <dcterms:creator><![CDATA[DEWITT-MORETTE]]></dcterms:creator>
    <dcterms:creator><![CDATA[WURM]]></dcterms:creator>
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    <dcterms:date><![CDATA[04/2001]]></dcterms:date>
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    <dcterms:rightsHolder><![CDATA[DEWITT-MORETTE]]></dcterms:rightsHolder>
    <dcterms:rightsHolder><![CDATA[WURM]]></dcterms:rightsHolder>
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    <dcterms:title><![CDATA[Scaling and functional integration. Suivi de Brydges&#039; operator in renormalization theory]]></dcterms:title>
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    <dcterms:subject><![CDATA[RENORMALISATION]]></dcterms:subject>
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    <dcterms:subject><![CDATA[ESPACE-TEMPS]]></dcterms:subject>
    <dcterms:subject><![CDATA[EQUATIONS AUX DERIVEES PARTIELLES]]></dcterms:subject>
    <dcterms:subject><![CDATA[ESPACES GENERALISES]]></dcterms:subject>
    <dcterms:creator><![CDATA[CARTIER]]></dcterms:creator>
    <dcterms:creator><![CDATA[DEWITT-MORETTE]]></dcterms:creator>
    <dcterms:source><![CDATA[M/99/51]]></dcterms:source>
    <dcterms:publisher><![CDATA[IHES]]></dcterms:publisher>
    <dcterms:date><![CDATA[07/1999]]></dcterms:date>
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    <dcterms:rightsHolder><![CDATA[DEWITT-MORETTE]]></dcterms:rightsHolder>
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