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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...

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Detalles Bibliográficos
Autores principales: Gazdzicki, Marek, Gorenstein, Mark I.
Lenguaje:eng
Publicado: 2001
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0370-2693(01)01013-9
http://cds.cern.ch/record/489523
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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).
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2001
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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