Combined Analysis of Two- and Three-Particle Correlations in q,p-Bose Gas Model

q-deformed oscillators and the q-Bose gas model enable effective description of the observed non-Bose type behavior of the intercept (''strength'') λ⁽²⁾ ≡ C⁽²⁾(K,K) - 1 of two-particle correlation function C⁽²⁾(p1,p2) of identical pions produced in heavy-ion collisions. Three- an...

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Дата:2006
Автор: Gavrilik, A.M.
Формат: Стаття
Мова:English
Опубліковано: Інститут математики НАН України 2006
Назва видання:Symmetry, Integrability and Geometry: Methods and Applications
Онлайн доступ:http://dspace.nbuv.gov.ua/handle/123456789/146107
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Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Цитувати:Combined Analysis of Two- and Three-Particle Correlations in q,p-Bose Gas Model / A.M. Gavrilik // Symmetry, Integrability and Geometry: Methods and Applications. — 2006. — Т. 2. — Бібліогр.: 43 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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spelling irk-123456789-1461072019-02-08T01:23:37Z Combined Analysis of Two- and Three-Particle Correlations in q,p-Bose Gas Model Gavrilik, A.M. q-deformed oscillators and the q-Bose gas model enable effective description of the observed non-Bose type behavior of the intercept (''strength'') λ⁽²⁾ ≡ C⁽²⁾(K,K) - 1 of two-particle correlation function C⁽²⁾(p1,p2) of identical pions produced in heavy-ion collisions. Three- and n-particle correlation functions of pions (or kaons) encode more information on the nature of the emitting sources in such experiments. And so, the q-Bose gas model was further developed: the intercepts of n-th order correlators of q-bosons and the n-particle correlation intercepts within the q,p-Bose gas model have been obtained, the result useful for quantum optics, too. Here we present the combined analysis of two- and three-pion correlation intercepts for the q-Bose gas model and its q,p-extension, and confront with empirical data (from CERN SPS and STAR/RHIC) on pion correlations. Similar to explicit dependence of λ⁽²⁾ on mean momenta of particles (pions, kaons) found earlier, here we explore the peculiar behavior, versus mean momentum, of the 3-particle correlation intercept λ⁽³⁾(K). The whole approach implies complete chaoticity of sources, unlike other joint descriptions of two- and three-pion correlations using two phenomenological parameters (e.g., core-halo fraction plus partial coherence of sources). 2006 Article Combined Analysis of Two- and Three-Particle Correlations in q,p-Bose Gas Model / A.M. Gavrilik // Symmetry, Integrability and Geometry: Methods and Applications. — 2006. — Т. 2. — Бібліогр.: 43 назв. — англ. 1815-0659 2000 Mathematics Subject Classification: 81R50; 81V99; 82B99 http://dspace.nbuv.gov.ua/handle/123456789/146107 en Symmetry, Integrability and Geometry: Methods and Applications Інститут математики НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
description q-deformed oscillators and the q-Bose gas model enable effective description of the observed non-Bose type behavior of the intercept (''strength'') λ⁽²⁾ ≡ C⁽²⁾(K,K) - 1 of two-particle correlation function C⁽²⁾(p1,p2) of identical pions produced in heavy-ion collisions. Three- and n-particle correlation functions of pions (or kaons) encode more information on the nature of the emitting sources in such experiments. And so, the q-Bose gas model was further developed: the intercepts of n-th order correlators of q-bosons and the n-particle correlation intercepts within the q,p-Bose gas model have been obtained, the result useful for quantum optics, too. Here we present the combined analysis of two- and three-pion correlation intercepts for the q-Bose gas model and its q,p-extension, and confront with empirical data (from CERN SPS and STAR/RHIC) on pion correlations. Similar to explicit dependence of λ⁽²⁾ on mean momenta of particles (pions, kaons) found earlier, here we explore the peculiar behavior, versus mean momentum, of the 3-particle correlation intercept λ⁽³⁾(K). The whole approach implies complete chaoticity of sources, unlike other joint descriptions of two- and three-pion correlations using two phenomenological parameters (e.g., core-halo fraction plus partial coherence of sources).
format Article
author Gavrilik, A.M.
spellingShingle Gavrilik, A.M.
Combined Analysis of Two- and Three-Particle Correlations in q,p-Bose Gas Model
Symmetry, Integrability and Geometry: Methods and Applications
author_facet Gavrilik, A.M.
author_sort Gavrilik, A.M.
title Combined Analysis of Two- and Three-Particle Correlations in q,p-Bose Gas Model
title_short Combined Analysis of Two- and Three-Particle Correlations in q,p-Bose Gas Model
title_full Combined Analysis of Two- and Three-Particle Correlations in q,p-Bose Gas Model
title_fullStr Combined Analysis of Two- and Three-Particle Correlations in q,p-Bose Gas Model
title_full_unstemmed Combined Analysis of Two- and Three-Particle Correlations in q,p-Bose Gas Model
title_sort combined analysis of two- and three-particle correlations in q,p-bose gas model
publisher Інститут математики НАН України
publishDate 2006
url http://dspace.nbuv.gov.ua/handle/123456789/146107
citation_txt Combined Analysis of Two- and Three-Particle Correlations in q,p-Bose Gas Model / A.M. Gavrilik // Symmetry, Integrability and Geometry: Methods and Applications. — 2006. — Т. 2. — Бібліогр.: 43 назв. — англ.
series Symmetry, Integrability and Geometry: Methods and Applications
work_keys_str_mv AT gavrilikam combinedanalysisoftwoandthreeparticlecorrelationsinqpbosegasmodel
first_indexed 2023-05-20T17:23:50Z
last_indexed 2023-05-20T17:23:50Z
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