Cargando…

Oscillatory modes of quarks in baryons for 3 quark flavors u,d,s

The present notes prepare the countin of 'oscillatory modes of N _fl = 3 light quarks', - u, d, s -, using the [??] broken symmetry classification, extended to the harmonic oscillator symmetry of 3 pairedoscillator modes. [??] stands for the space rotation group generated by the sum of the...

Descripción completa

Detalles Bibliográficos
Autores principales: Minkowski, Peter, Kabana, Sonia
Lenguaje:eng
Publicado: 2014
Materias:
Acceso en línea:https://dx.doi.org/10.1051/epjconf/20147100090
http://cds.cern.ch/record/2026248
_version_ 1780947331412131840
author Minkowski, Peter
Kabana, Sonia
author_facet Minkowski, Peter
Kabana, Sonia
author_sort Minkowski, Peter
collection CERN
description The present notes prepare the countin of 'oscillatory modes of N _fl = 3 light quarks', - u, d, s -, using the [??] broken symmetry classification, extended to the harmonic oscillator symmetry of 3 pairedoscillator modes. [??] stands for the space rotation group generated by the sum of the 3 individual angular momenta of quarks in their c.m. system . The motivation arises from modeling the yields of hadrons in heavy ion collisions at RHIC and LHC, necessitating at the respective highest c.m. energies per nucleon pairs an increase of heavy hadron resonances relative to e.g. SPS energies, whence the included hadrons are treated as a noninteracting gas.
id oai-inspirehep.net-1294326
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2014
record_format invenio
spelling oai-inspirehep.net-12943262022-08-10T20:02:24Zdoi:10.1051/epjconf/20147100090http://cds.cern.ch/record/2026248engMinkowski, PeterKabana, SoniaOscillatory modes of quarks in baryons for 3 quark flavors u,d,sParticle Physics - PhenomenologyThe present notes prepare the countin of 'oscillatory modes of N _fl = 3 light quarks', - u, d, s -, using the [??] broken symmetry classification, extended to the harmonic oscillator symmetry of 3 pairedoscillator modes. [??] stands for the space rotation group generated by the sum of the 3 individual angular momenta of quarks in their c.m. system . The motivation arises from modeling the yields of hadrons in heavy ion collisions at RHIC and LHC, necessitating at the respective highest c.m. energies per nucleon pairs an increase of heavy hadron resonances relative to e.g. SPS energies, whence the included hadrons are treated as a noninteracting gas.oai:inspirehep.net:12943262014
spellingShingle Particle Physics - Phenomenology
Minkowski, Peter
Kabana, Sonia
Oscillatory modes of quarks in baryons for 3 quark flavors u,d,s
title Oscillatory modes of quarks in baryons for 3 quark flavors u,d,s
title_full Oscillatory modes of quarks in baryons for 3 quark flavors u,d,s
title_fullStr Oscillatory modes of quarks in baryons for 3 quark flavors u,d,s
title_full_unstemmed Oscillatory modes of quarks in baryons for 3 quark flavors u,d,s
title_short Oscillatory modes of quarks in baryons for 3 quark flavors u,d,s
title_sort oscillatory modes of quarks in baryons for 3 quark flavors u,d,s
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1051/epjconf/20147100090
http://cds.cern.ch/record/2026248
work_keys_str_mv AT minkowskipeter oscillatorymodesofquarksinbaryonsfor3quarkflavorsuds
AT kabanasonia oscillatorymodesofquarksinbaryonsfor3quarkflavorsuds