Nonextensive Statistical Mechanics: Some Links with Astronomical Phenomena
- Autores
- Tsallis, Constantino; Prato, Domingo; Plastino, Ángel Ricardo
- Año de publicación
- 2004
- Idioma
- inglés
- Tipo de recurso
- artículo
- Estado
- versión publicada
- Descripción
- A variety of astronomical phenomena appear to not satisfy the ergodic hypothesis in the relevant stationary state, if any. As such, there is no reason for expecting the applicability of Boltzmann–Gibbs (BG) statistical mechanics. Some of these phenomena appear to follow, instead, nonextensive statistical mechanics. In the same manner that the BG formalism is based on the entropy SBG = −k∑ipi ln pi, the nonextensive one is based on the form Sq = k(1 −∑ipiq)/(q− 1) (with S₁ = SBG). The stationary states of the former are characterized by an exponential dependence on the energy, whereas those of the latter are characterized by an (asymptotic) power law. A brief review of this theory is given here, as well as of some of its applications, such as the solar neutrino problem, polytropic self-gravitating systems, galactic peculiar velocities, cosmic rays and some cosmological aspects. In addition to these, an analogy with the Keplerian elliptic orbits versus the Ptolemaic epicycles is developed, where we show that optimizing Sq with a few constraints is equivalent to optimizing SBG with an infinite number of constraints.
Facultad de Ciencias Astronómicas y Geofísicas - Materia
-
Astronomía
Física
nonextensive statistical mechanics
Tsallis entropy
solar neutrino problem
cosmic rays
polytropes - Nivel de accesibilidad
- acceso abierto
- Condiciones de uso
- http://creativecommons.org/licenses/by-nc-sa/4.0/
- Repositorio
- Institución
- Universidad Nacional de La Plata
- OAI Identificador
- oai:sedici.unlp.edu.ar:10915/130646
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Nonextensive Statistical Mechanics: Some Links with Astronomical PhenomenaTsallis, ConstantinoPrato, DomingoPlastino, Ángel RicardoAstronomíaFísicanonextensive statistical mechanicsTsallis entropysolar neutrino problemcosmic rayspolytropesA variety of astronomical phenomena appear to not satisfy the ergodic hypothesis in the relevant stationary state, if any. As such, there is no reason for expecting the applicability of Boltzmann–Gibbs (BG) statistical mechanics. Some of these phenomena appear to follow, instead, nonextensive statistical mechanics. In the same manner that the BG formalism is based on the entropy S<sub>BG</sub> = −k∑<sub>i</sub>p<sub>i</sub> ln p<sub>i</sub>, the nonextensive one is based on the form S<sub>q</sub> = k(1 −∑<sub>i</sub>p<sub>i</sub><sup>q</sup>)/(q− 1) (with S₁ = S<sub>BG</sub>). The stationary states of the former are characterized by an exponential dependence on the energy, whereas those of the latter are characterized by an (asymptotic) power law. A brief review of this theory is given here, as well as of some of its applications, such as the solar neutrino problem, polytropic self-gravitating systems, galactic peculiar velocities, cosmic rays and some cosmological aspects. In addition to these, an analogy with the Keplerian elliptic orbits versus the Ptolemaic epicycles is developed, where we show that optimizing S<sub>q</sub> with a few constraints is equivalent to optimizing S<sub>BG</sub> with an infinite number of constraints.Facultad de Ciencias Astronómicas y Geofísicas2004-03info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionArticulohttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdf259-274http://sedici.unlp.edu.ar/handle/10915/130646enginfo:eu-repo/semantics/altIdentifier/issn/0004-640Xinfo:eu-repo/semantics/altIdentifier/issn/1572-946Xinfo:eu-repo/semantics/altIdentifier/arxiv/cond-mat/0301590info:eu-repo/semantics/altIdentifier/doi/10.1023/b:astr.0000032528.99179.4finfo:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by-nc-sa/4.0/Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International (CC BY-NC-SA 4.0)reponame:SEDICI (UNLP)instname:Universidad Nacional de La Platainstacron:UNLP2025-10-15T11:23:08Zoai:sedici.unlp.edu.ar:10915/130646Institucionalhttp://sedici.unlp.edu.ar/Universidad públicaNo correspondehttp://sedici.unlp.edu.ar/oai/snrdalira@sedici.unlp.edu.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:13292025-10-15 11:23:08.761SEDICI (UNLP) - Universidad Nacional de La Platafalse |
dc.title.none.fl_str_mv |
Nonextensive Statistical Mechanics: Some Links with Astronomical Phenomena |
title |
Nonextensive Statistical Mechanics: Some Links with Astronomical Phenomena |
spellingShingle |
Nonextensive Statistical Mechanics: Some Links with Astronomical Phenomena Tsallis, Constantino Astronomía Física nonextensive statistical mechanics Tsallis entropy solar neutrino problem cosmic rays polytropes |
title_short |
Nonextensive Statistical Mechanics: Some Links with Astronomical Phenomena |
title_full |
Nonextensive Statistical Mechanics: Some Links with Astronomical Phenomena |
title_fullStr |
Nonextensive Statistical Mechanics: Some Links with Astronomical Phenomena |
title_full_unstemmed |
Nonextensive Statistical Mechanics: Some Links with Astronomical Phenomena |
title_sort |
Nonextensive Statistical Mechanics: Some Links with Astronomical Phenomena |
dc.creator.none.fl_str_mv |
Tsallis, Constantino Prato, Domingo Plastino, Ángel Ricardo |
author |
Tsallis, Constantino |
author_facet |
Tsallis, Constantino Prato, Domingo Plastino, Ángel Ricardo |
author_role |
author |
author2 |
Prato, Domingo Plastino, Ángel Ricardo |
author2_role |
author author |
dc.subject.none.fl_str_mv |
Astronomía Física nonextensive statistical mechanics Tsallis entropy solar neutrino problem cosmic rays polytropes |
topic |
Astronomía Física nonextensive statistical mechanics Tsallis entropy solar neutrino problem cosmic rays polytropes |
dc.description.none.fl_txt_mv |
A variety of astronomical phenomena appear to not satisfy the ergodic hypothesis in the relevant stationary state, if any. As such, there is no reason for expecting the applicability of Boltzmann–Gibbs (BG) statistical mechanics. Some of these phenomena appear to follow, instead, nonextensive statistical mechanics. In the same manner that the BG formalism is based on the entropy S<sub>BG</sub> = −k∑<sub>i</sub>p<sub>i</sub> ln p<sub>i</sub>, the nonextensive one is based on the form S<sub>q</sub> = k(1 −∑<sub>i</sub>p<sub>i</sub><sup>q</sup>)/(q− 1) (with S₁ = S<sub>BG</sub>). The stationary states of the former are characterized by an exponential dependence on the energy, whereas those of the latter are characterized by an (asymptotic) power law. A brief review of this theory is given here, as well as of some of its applications, such as the solar neutrino problem, polytropic self-gravitating systems, galactic peculiar velocities, cosmic rays and some cosmological aspects. In addition to these, an analogy with the Keplerian elliptic orbits versus the Ptolemaic epicycles is developed, where we show that optimizing S<sub>q</sub> with a few constraints is equivalent to optimizing S<sub>BG</sub> with an infinite number of constraints. Facultad de Ciencias Astronómicas y Geofísicas |
description |
A variety of astronomical phenomena appear to not satisfy the ergodic hypothesis in the relevant stationary state, if any. As such, there is no reason for expecting the applicability of Boltzmann–Gibbs (BG) statistical mechanics. Some of these phenomena appear to follow, instead, nonextensive statistical mechanics. In the same manner that the BG formalism is based on the entropy S<sub>BG</sub> = −k∑<sub>i</sub>p<sub>i</sub> ln p<sub>i</sub>, the nonextensive one is based on the form S<sub>q</sub> = k(1 −∑<sub>i</sub>p<sub>i</sub><sup>q</sup>)/(q− 1) (with S₁ = S<sub>BG</sub>). The stationary states of the former are characterized by an exponential dependence on the energy, whereas those of the latter are characterized by an (asymptotic) power law. A brief review of this theory is given here, as well as of some of its applications, such as the solar neutrino problem, polytropic self-gravitating systems, galactic peculiar velocities, cosmic rays and some cosmological aspects. In addition to these, an analogy with the Keplerian elliptic orbits versus the Ptolemaic epicycles is developed, where we show that optimizing S<sub>q</sub> with a few constraints is equivalent to optimizing S<sub>BG</sub> with an infinite number of constraints. |
publishDate |
2004 |
dc.date.none.fl_str_mv |
2004-03 |
dc.type.none.fl_str_mv |
info:eu-repo/semantics/article info:eu-repo/semantics/publishedVersion Articulo http://purl.org/coar/resource_type/c_6501 info:ar-repo/semantics/articulo |
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article |
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publishedVersion |
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http://sedici.unlp.edu.ar/handle/10915/130646 |
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http://sedici.unlp.edu.ar/handle/10915/130646 |
dc.language.none.fl_str_mv |
eng |
language |
eng |
dc.relation.none.fl_str_mv |
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http://creativecommons.org/licenses/by-nc-sa/4.0/ Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International (CC BY-NC-SA 4.0) |
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application/pdf 259-274 |
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