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Power Law in Hadron Production
In high energy p+p interactions the mean multiplicity of neutral mesons (from eta to Upsilon) and the transverse mass spectra of pions (m_T= 1 - 15 GeV/c^2) reveal a remarkable universal behaviour: they follow, over 10 orders of magnitude, the same power law function: C m_(T)^(-P). This scaling is r...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
2001
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/S0370-2693(01)01013-9 http://cds.cern.ch/record/489523 |
_version_ | 1780897015798956032 |
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author | Gazdzicki, Marek Gorenstein, Mark I. |
author_facet | Gazdzicki, Marek Gorenstein, Mark I. |
author_sort | Gazdzicki, Marek |
collection | CERN |
description | In high energy p+p interactions the mean multiplicity of neutral mesons (from eta to Upsilon) and the transverse mass spectra of pions (m_T= 1 - 15 GeV/c^2) reveal a remarkable universal behaviour: they follow, over 10 orders of magnitude, the same power law function: C m_(T)^(-P). This scaling is rather similar to that expected in the statistical description of hadron production: the parameter P plays the role of a temperature and the normalisation constant C is analogous to the system volume. The fundamental difference is, however, in the form of the distribution function. In order to reproduce the experimental results and preserve the basic structure of the statistical approach the Boltzmann factor e^(-E^*/T) appearing in standard statistical mechanics has to be substituted by a power law factor (E^*/\Lambda)^(-P). |
id | cern-489523 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2001 |
record_format | invenio |
spelling | cern-4895232023-03-14T18:42:12Zdoi:10.1016/S0370-2693(01)01013-9http://cds.cern.ch/record/489523engGazdzicki, MarekGorenstein, Mark I.Power Law in Hadron ProductionParticle Physics - PhenomenologyIn high energy p+p interactions the mean multiplicity of neutral mesons (from eta to Upsilon) and the transverse mass spectra of pions (m_T= 1 - 15 GeV/c^2) reveal a remarkable universal behaviour: they follow, over 10 orders of magnitude, the same power law function: C m_(T)^(-P). This scaling is rather similar to that expected in the statistical description of hadron production: the parameter P plays the role of a temperature and the normalisation constant C is analogous to the system volume. The fundamental difference is, however, in the form of the distribution function. In order to reproduce the experimental results and preserve the basic structure of the statistical approach the Boltzmann factor e^(-E^*/T) appearing in standard statistical mechanics has to be substituted by a power law factor (E^*/\Lambda)^(-P).In high energy p+p(bar) interactions the mean multiplicity and transverse mass spectra of neutral mesons from eta to Upsilon (m = 0.5 - 10 GeV/c^2) and the transverse mass spectra of pions (m_T > 1 GeV/c^2) reveal a remarkable behaviour: they follow, over more than 10 orders of magnitude, the power-law function:The parameters C and P are energy dependent, but similar for all mesons produced at the same collision energy. This scaling resembles that expected in the statistical description of hadron production: the parameter P plays the role of a temperature and the normalisation constant C is analogous to the system volume. The fundamental difference is, however, in the form of the distribution function. In order to reproduce the experimental results and preserve the basic structure of the statistical approach the Boltzmann factor e^(-E/T) appearing in standard statistical mechanics has to be substituted by a power-law factor (E/Lambda)^(-P).In high energy p ( p )+ p interactions the mean multiplicity and transverse mass spectra of neutral mesons from η to ϒ ( m ≅0.5–10 GeV/ c 2 ) and the transverse mass spectra of pions ( m T > 1 GeV/ c 2 ) reveal a remarkable behaviour: they follow, over more than 10 orders of magnitude, the power-law function: Cm ( T ) − P . The parameters C and P are energy dependent, but similar for all mesons produced at the same collision energy. This scaling resembles that expected in the statistical description of hadron production: the parameter P plays the role of a temperature and the normalisation constant C is analogous to the system volume. The fundamental difference is, however, in the form of the distribution function. In order to reproduce the experimental results and preserve the basic structure of the statistical approach the Boltzmann factor e −E ∗ /T appearing in standard statistical mechanics has to be substituted by a power-law factor (E ∗ /Λ) −P .hep-ph/0103010oai:cds.cern.ch:4895232001 |
spellingShingle | Particle Physics - Phenomenology Gazdzicki, Marek Gorenstein, Mark I. Power Law in Hadron Production |
title | Power Law in Hadron Production |
title_full | Power Law in Hadron Production |
title_fullStr | Power Law in Hadron Production |
title_full_unstemmed | Power Law in Hadron Production |
title_short | Power Law in Hadron Production |
title_sort | power law in hadron production |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1016/S0370-2693(01)01013-9 http://cds.cern.ch/record/489523 |
work_keys_str_mv | AT gazdzickimarek powerlawinhadronproduction AT gorensteinmarki powerlawinhadronproduction |