The calculus of thermodynamical formalism
Autor(a) principal: | |
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Data de Publicação: | 2018 |
Outros Autores: | , , |
Tipo de documento: | Artigo |
Idioma: | eng |
Título da fonte: | Repositório Institucional da UFRGS |
Texto Completo: | http://hdl.handle.net/10183/182431 |
Resumo: | Given an onto map T acting on a metric space and an appropriate Banach space of functions X./, one classically constructs for each potential A 2 X a transfer operator LA acting on X./. Under suitable hypotheses, it is well-known that LA has a maximal eigenvalue A, has a spectral gap and defines a unique Gibbs measure A. Moreover there is a unique normalized potential of the form B D ACf f T Cc acting as a representative of the class of all potentials defining the same Gibbs measure. The goal of the present article is to study the geometry of the set N of normalized potentials, of the normalization map A 7! B, and of the Gibbs map A 7! A. We give an easy proof of the fact that N is an analytic submanifold of X and that the normalization map is analytic; we compute the derivative of the Gibbs map; and we endow N with a natural weak Riemannian metric (derived from the asymptotic variance) with respect to which we compute the gradient flow induced by the pressure with respect to a given potential, e.g. the metric entropy functional. We also apply these ideas to recover in a wide setting existence and uniqueness of equilibrium states, possibly under constraints. |
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Giulietti, PaoloKloeckner, Benoît R.Lopes, Artur OscarFarias, Diego Marcon2018-09-22T03:01:36Z20181435-9855http://hdl.handle.net/10183/182431001077339Given an onto map T acting on a metric space and an appropriate Banach space of functions X./, one classically constructs for each potential A 2 X a transfer operator LA acting on X./. Under suitable hypotheses, it is well-known that LA has a maximal eigenvalue A, has a spectral gap and defines a unique Gibbs measure A. Moreover there is a unique normalized potential of the form B D ACf f T Cc acting as a representative of the class of all potentials defining the same Gibbs measure. The goal of the present article is to study the geometry of the set N of normalized potentials, of the normalization map A 7! B, and of the Gibbs map A 7! A. We give an easy proof of the fact that N is an analytic submanifold of X and that the normalization map is analytic; we compute the derivative of the Gibbs map; and we endow N with a natural weak Riemannian metric (derived from the asymptotic variance) with respect to which we compute the gradient flow induced by the pressure with respect to a given potential, e.g. the metric entropy functional. We also apply these ideas to recover in a wide setting existence and uniqueness of equilibrium states, possibly under constraints.application/pdfengJournal of the European Mathematical Society, JEMS. Zurique, Suíça, European Mathematical Society, 2018. Vol. 20, no. 10 (July 2018), p. 2357–2412Estados de equilibrioEntropiaRegularização entrópicaTransfer operatorsEquilibrium statesEntropyRegularityWasserstein spaceThe calculus of thermodynamical formalismEstrangeiroinfo:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/openAccessreponame:Repositório Institucional da UFRGSinstname:Universidade Federal do Rio Grande do Sul (UFRGS)instacron:UFRGSORIGINAL001077339.pdfTexto completo (inglês)application/pdf412888http://www.lume.ufrgs.br/bitstream/10183/182431/1/001077339.pdfa1772de02af2f5d42d0f5e8220012460MD51TEXT001077339.pdf.txt001077339.pdf.txtExtracted Texttext/plain133709http://www.lume.ufrgs.br/bitstream/10183/182431/2/001077339.pdf.txt2eb622ac7814858e39c9efb3ebde6bd3MD52THUMBNAIL001077339.pdf.jpg001077339.pdf.jpgGenerated Thumbnailimage/jpeg1375http://www.lume.ufrgs.br/bitstream/10183/182431/3/001077339.pdf.jpgc421bc9ea1f3a2283cb814ed41084bd5MD5310183/1824312018-10-05 07:55:30.309oai:www.lume.ufrgs.br:10183/182431Repositório de PublicaçõesPUBhttps://lume.ufrgs.br/oai/requestopendoar:2018-10-05T10:55:30Repositório Institucional da UFRGS - Universidade Federal do Rio Grande do Sul (UFRGS)false |
dc.title.pt_BR.fl_str_mv |
The calculus of thermodynamical formalism |
title |
The calculus of thermodynamical formalism |
spellingShingle |
The calculus of thermodynamical formalism Giulietti, Paolo Estados de equilibrio Entropia Regularização entrópica Transfer operators Equilibrium states Entropy Regularity Wasserstein space |
title_short |
The calculus of thermodynamical formalism |
title_full |
The calculus of thermodynamical formalism |
title_fullStr |
The calculus of thermodynamical formalism |
title_full_unstemmed |
The calculus of thermodynamical formalism |
title_sort |
The calculus of thermodynamical formalism |
author |
Giulietti, Paolo |
author_facet |
Giulietti, Paolo Kloeckner, Benoît R. Lopes, Artur Oscar Farias, Diego Marcon |
author_role |
author |
author2 |
Kloeckner, Benoît R. Lopes, Artur Oscar Farias, Diego Marcon |
author2_role |
author author author |
dc.contributor.author.fl_str_mv |
Giulietti, Paolo Kloeckner, Benoît R. Lopes, Artur Oscar Farias, Diego Marcon |
dc.subject.por.fl_str_mv |
Estados de equilibrio Entropia Regularização entrópica |
topic |
Estados de equilibrio Entropia Regularização entrópica Transfer operators Equilibrium states Entropy Regularity Wasserstein space |
dc.subject.eng.fl_str_mv |
Transfer operators Equilibrium states Entropy Regularity Wasserstein space |
description |
Given an onto map T acting on a metric space and an appropriate Banach space of functions X./, one classically constructs for each potential A 2 X a transfer operator LA acting on X./. Under suitable hypotheses, it is well-known that LA has a maximal eigenvalue A, has a spectral gap and defines a unique Gibbs measure A. Moreover there is a unique normalized potential of the form B D ACf f T Cc acting as a representative of the class of all potentials defining the same Gibbs measure. The goal of the present article is to study the geometry of the set N of normalized potentials, of the normalization map A 7! B, and of the Gibbs map A 7! A. We give an easy proof of the fact that N is an analytic submanifold of X and that the normalization map is analytic; we compute the derivative of the Gibbs map; and we endow N with a natural weak Riemannian metric (derived from the asymptotic variance) with respect to which we compute the gradient flow induced by the pressure with respect to a given potential, e.g. the metric entropy functional. We also apply these ideas to recover in a wide setting existence and uniqueness of equilibrium states, possibly under constraints. |
publishDate |
2018 |
dc.date.accessioned.fl_str_mv |
2018-09-22T03:01:36Z |
dc.date.issued.fl_str_mv |
2018 |
dc.type.driver.fl_str_mv |
Estrangeiro info:eu-repo/semantics/article |
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info:eu-repo/semantics/publishedVersion |
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article |
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publishedVersion |
dc.identifier.uri.fl_str_mv |
http://hdl.handle.net/10183/182431 |
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1435-9855 |
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001077339 |
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http://hdl.handle.net/10183/182431 |
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eng |
language |
eng |
dc.relation.ispartof.pt_BR.fl_str_mv |
Journal of the European Mathematical Society, JEMS. Zurique, Suíça, European Mathematical Society, 2018. Vol. 20, no. 10 (July 2018), p. 2357–2412 |
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openAccess |
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