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Non-perturbative quarkonium dissociation in hadronic matter

We calculate the dissociation rates of quarkonium ground states by tunnelling and direct thermal activation to the continuum. For hadronic matter at temperatures T \leq 0.2 GeV, neither of these mechanisms leads to a sufficiently large dissociation to explain the experimentally observed suppression...

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Detalles Bibliográficos
Autores principales: Kharzeev, D., McLerran, Larry D., Satz, H.
Lenguaje:eng
Publicado: 1995
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0370-2693(95)00695-H
http://cds.cern.ch/record/280497
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author Kharzeev, D.
McLerran, Larry D.
Satz, H.
author_facet Kharzeev, D.
McLerran, Larry D.
Satz, H.
author_sort Kharzeev, D.
collection CERN
description We calculate the dissociation rates of quarkonium ground states by tunnelling and direct thermal activation to the continuum. For hadronic matter at temperatures T \leq 0.2 GeV, neither of these mechanisms leads to a sufficiently large dissociation to explain the experimentally observed suppression of charmonium. Dissociation by sequential excitation to excited energy levels, although OZI-forbidden requires further analysis.
id cern-280497
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1995
record_format invenio
spelling cern-2804972020-07-23T02:50:29Zdoi:10.1016/0370-2693(95)00695-Hhttp://cds.cern.ch/record/280497engKharzeev, D.McLerran, Larry D.Satz, H.Non-perturbative quarkonium dissociation in hadronic matterParticle Physics - PhenomenologyWe calculate the dissociation rates of quarkonium ground states by tunnelling and direct thermal activation to the continuum. For hadronic matter at temperatures T \leq 0.2 GeV, neither of these mechanisms leads to a sufficiently large dissociation to explain the experimentally observed suppression of charmonium. Dissociation by sequential excitation to excited energy levels, although OZI-forbidden requires further analysis.We calculate the dissociation rates of quarkonium ground states by tunnelling and direct thermal activation to the continuum. For hadronic matter at temperatures $T \leq 0.2$ GeV, neither of these mechanisms leads to a sufficiently large dissociation to explain the experimentally observed suppression of charmonium. Dissociation by sequential excitation to excited energy levels, although OZI-forbidden, requires further analysis.We calculate the dissociation rates of quarkonium ground states by tunnelling and direct thermal activation to the continuum. For hadronic matter at temperatures TWe calculate the dissociation rates of quarkonium ground states by tunnelling and direct thermal activation to the continuum. For hadronic matter at temperatures Thep-ph/9504338CERN-TH-95-27CERN-TH-95-027BI-TP-95-15TPI-MINN-95-07BI-TP-95-15CERN-TH-95-27TPI-MINN-95-07oai:cds.cern.ch:2804971995-04-19
spellingShingle Particle Physics - Phenomenology
Kharzeev, D.
McLerran, Larry D.
Satz, H.
Non-perturbative quarkonium dissociation in hadronic matter
title Non-perturbative quarkonium dissociation in hadronic matter
title_full Non-perturbative quarkonium dissociation in hadronic matter
title_fullStr Non-perturbative quarkonium dissociation in hadronic matter
title_full_unstemmed Non-perturbative quarkonium dissociation in hadronic matter
title_short Non-perturbative quarkonium dissociation in hadronic matter
title_sort non-perturbative quarkonium dissociation in hadronic matter
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/0370-2693(95)00695-H
http://cds.cern.ch/record/280497
work_keys_str_mv AT kharzeevd nonperturbativequarkoniumdissociationinhadronicmatter
AT mclerranlarryd nonperturbativequarkoniumdissociationinhadronicmatter
AT satzh nonperturbativequarkoniumdissociationinhadronicmatter