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Thermal hadron production in Si-Au collisions

The most abundantly produced hadron species in Si\!-\!Au collisions at the BNL-AGS (nucleons, pions, kaons, antikaons and hyperons) are shown to be in accord with emission from a thermal resonance gas source of temperature T\simeq 110 MeV and baryochemical potential \mu_B \simeq 540 MeV, correspondi...

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Detalles Bibliográficos
Autores principales: Cleymans, J., Elliott, D., Satz, H., Thews, R.L.
Lenguaje:eng
Publicado: 1996
Materias:
Acceso en línea:https://dx.doi.org/10.1007/s002880050393
http://cds.cern.ch/record/299500
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author Cleymans, J.
Elliott, D.
Satz, H.
Thews, R.L.
author_facet Cleymans, J.
Elliott, D.
Satz, H.
Thews, R.L.
author_sort Cleymans, J.
collection CERN
description The most abundantly produced hadron species in Si\!-\!Au collisions at the BNL-AGS (nucleons, pions, kaons, antikaons and hyperons) are shown to be in accord with emission from a thermal resonance gas source of temperature T\simeq 110 MeV and baryochemical potential \mu_B \simeq 540 MeV, corresponding to about 1/3 standard nuclear density. Our analysis takes the isopin asymmetry of the initial state fully into account.
id cern-299500
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1996
record_format invenio
spelling cern-2995002023-03-14T18:08:59Zdoi:10.1007/s002880050393http://cds.cern.ch/record/299500engCleymans, J.Elliott, D.Satz, H.Thews, R.L.Thermal hadron production in Si-Au collisionsNuclear Physics - TheoryThe most abundantly produced hadron species in Si\!-\!Au collisions at the BNL-AGS (nucleons, pions, kaons, antikaons and hyperons) are shown to be in accord with emission from a thermal resonance gas source of temperature T\simeq 110 MeV and baryochemical potential \mu_B \simeq 540 MeV, corresponding to about 1/3 standard nuclear density. Our analysis takes the isopin asymmetry of the initial state fully into account.The most abundantly produced hadron species in $Si\!-\!Au$ collisions at the BNL-AGS (nucleons, pions, kaons, antikaons and hyperons) are shown to be in accord with emission from a thermal resonance gas source of temperature $T\simeq 110$ MeV and baryochemical potential $\mu_B \simeq 540$ MeV, corresponding to about 1/3 standard nuclear density. Our analysis takes the isopin asymmetry of the initial state fully into account.nucl-th/9603004CERN-TH-95-298AZPH-TH-95-26BI-TP-95-35UCT-TP-95-225AZPH-TH-95-26BI-TP-95-35CERN-TH-95-298UCT-TP-225oai:cds.cern.ch:2995001996-03-06
spellingShingle Nuclear Physics - Theory
Cleymans, J.
Elliott, D.
Satz, H.
Thews, R.L.
Thermal hadron production in Si-Au collisions
title Thermal hadron production in Si-Au collisions
title_full Thermal hadron production in Si-Au collisions
title_fullStr Thermal hadron production in Si-Au collisions
title_full_unstemmed Thermal hadron production in Si-Au collisions
title_short Thermal hadron production in Si-Au collisions
title_sort thermal hadron production in si-au collisions
topic Nuclear Physics - Theory
url https://dx.doi.org/10.1007/s002880050393
http://cds.cern.ch/record/299500
work_keys_str_mv AT cleymansj thermalhadronproductioninsiaucollisions
AT elliottd thermalhadronproductioninsiaucollisions
AT satzh thermalhadronproductioninsiaucollisions
AT thewsrl thermalhadronproductioninsiaucollisions