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Transverse momentum bounds and scaling in the hydrodynamical model
It is shown that the equation of state of an ideal relativistic gas, as applied in the hydrodynamical model, leads not only to deviations from scaling in longitudinal rapidity distributions, but also to an average transverse momentum increasing asymptotically as a power of the incident energy. To pr...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
1974
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/0370-2693(74)90691-1 http://cds.cern.ch/record/873651 |
_version_ | 1780907703317561344 |
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author | Chaichian, Masud Satz, Helmut Suhonen, E |
author_facet | Chaichian, Masud Satz, Helmut Suhonen, E |
author_sort | Chaichian, Masud |
collection | CERN |
description | It is shown that the equation of state of an ideal relativistic gas, as applied in the hydrodynamical model, leads not only to deviations from scaling in longitudinal rapidity distributions, but also to an average transverse momentum increasing asymptotically as a power of the incident energy. To prevent such an increase, one must use the equation of state of an interacting gas, in which the velocity of sound becomes asymptotically equal to that of light. This then also restores scaling (up to logarithmic terms) in longitudinal rapidity. (25 refs). |
id | cern-873651 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1974 |
record_format | invenio |
spelling | cern-8736512019-09-30T06:29:59Zdoi:10.1016/0370-2693(74)90691-1http://cds.cern.ch/record/873651engChaichian, MasudSatz, HelmutSuhonen, ETransverse momentum bounds and scaling in the hydrodynamical modelParticle Physics - PhenomenologyIt is shown that the equation of state of an ideal relativistic gas, as applied in the hydrodynamical model, leads not only to deviations from scaling in longitudinal rapidity distributions, but also to an average transverse momentum increasing asymptotically as a power of the incident energy. To prevent such an increase, one must use the equation of state of an interacting gas, in which the velocity of sound becomes asymptotically equal to that of light. This then also restores scaling (up to logarithmic terms) in longitudinal rapidity. (25 refs).CERN-TH-1862oai:cds.cern.ch:8736511974-04-19 |
spellingShingle | Particle Physics - Phenomenology Chaichian, Masud Satz, Helmut Suhonen, E Transverse momentum bounds and scaling in the hydrodynamical model |
title | Transverse momentum bounds and scaling in the hydrodynamical model |
title_full | Transverse momentum bounds and scaling in the hydrodynamical model |
title_fullStr | Transverse momentum bounds and scaling in the hydrodynamical model |
title_full_unstemmed | Transverse momentum bounds and scaling in the hydrodynamical model |
title_short | Transverse momentum bounds and scaling in the hydrodynamical model |
title_sort | transverse momentum bounds and scaling in the hydrodynamical model |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1016/0370-2693(74)90691-1 http://cds.cern.ch/record/873651 |
work_keys_str_mv | AT chaichianmasud transversemomentumboundsandscalinginthehydrodynamicalmodel AT satzhelmut transversemomentumboundsandscalinginthehydrodynamicalmodel AT suhonene transversemomentumboundsandscalinginthehydrodynamicalmodel |