On the phenomenological analysis of the S-matrix in multiple production

Detalhes bibliográficos
Autor(a) principal: Ito, D.
Data de Publicação: 1961
Outros Autores: Zimerman, A. H., Ragusa, S., Miyazima, T.
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Repositório Institucional da UNESP
Texto Completo: http://dx.doi.org/10.1007/BF02733443
http://hdl.handle.net/11449/231174
Resumo: An attempt is made to analyse the structure of S-matrix elements for multiple production by phenomenological considerations based upon the two center model. We start from two assumptions: 1) the momentum distributions of pions emitted in the for- and backward cones are isotropic in each center-of-mass system (the fire ball rest system) and the average values e{open}0 of the pion energies in this system do not depend on the details of collisions; 2) the mean value of the momentum transfer Δ is always of the order of the nucleon mass M. From these assumptions the following results are derived in Sect. 2: 1) the multiplicity is given by n{reversed tilde equals}ξ√2 E0|Δ|/e{open}0, where ξ is the ratio ℳ/ℳmax of the fire ball mass ℳ and its maximum value ℳmax. Experimentally, ξ{reversed tilde equals}0.5 at 1013 eV; 2) the lower limit of the inelasticity K is given by K≥ξ2. At 1013 eV we have K≥ξ2{reversed tilde equals}0.2 which is consistent with experiments. The relation between multiplicity and inelasticity is discussed; 3) in the center-of-mass system of the fire ball and the recoil nucleon (« isobar system » IBS), the ratio |M|/ℳ of the momentum of the nucleon M and the fire ball mass ℳ is also expressed by the parameter ξ as |N|/ℳ=(1-ξ2)/2ξ. At 1013 eV we have |M|/ℳ{reversed tilde equals}1. This means that an equipartition of energy is approximately valid for the three possible degrees of freedom: the motion of the recoil nucleon, the translational and internal motion of the fire ball. |M|≪ℳ is excluded, unless K is unity, contrary to experiments; 4) when the equipartition holds, the mean value of the transverse momentum is constant and its value is of the order of e{open}0. In Sect. 3, the ℳ and n-dependence of the S-matrix is discussed. And by using the corresponding results we estimate the asymmetry in numbers of particles n1 and n2 emitted in the for- and backward cones. The parameter [〈(n1-n2)2〉/〈(n1+n2)2〉]1/2, a measure of the asymmetry, becomes 1/3 due to statistical fluctuation alone. It becomes larger if the energy transfer Δ0 is not zero. Discussion is also made of the condition by which the average value e{open}0 of the pion energy in the fire ball is constant. The properties of the fire ball seem to be independent from the mechanism of its production. Extending this point of view, the similarity between the multiple production in N-N collisions and N-N annihilation is discussed in Sect. 4. Conclusions are given in Sect. 5. © 1961 Società Italiana di Fisica.
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spelling On the phenomenological analysis of the S-matrix in multiple productionAn attempt is made to analyse the structure of S-matrix elements for multiple production by phenomenological considerations based upon the two center model. We start from two assumptions: 1) the momentum distributions of pions emitted in the for- and backward cones are isotropic in each center-of-mass system (the fire ball rest system) and the average values e{open}0 of the pion energies in this system do not depend on the details of collisions; 2) the mean value of the momentum transfer Δ is always of the order of the nucleon mass M. From these assumptions the following results are derived in Sect. 2: 1) the multiplicity is given by n{reversed tilde equals}ξ√2 E0|Δ|/e{open}0, where ξ is the ratio ℳ/ℳmax of the fire ball mass ℳ and its maximum value ℳmax. Experimentally, ξ{reversed tilde equals}0.5 at 1013 eV; 2) the lower limit of the inelasticity K is given by K≥ξ2. At 1013 eV we have K≥ξ2{reversed tilde equals}0.2 which is consistent with experiments. The relation between multiplicity and inelasticity is discussed; 3) in the center-of-mass system of the fire ball and the recoil nucleon (« isobar system » IBS), the ratio |M|/ℳ of the momentum of the nucleon M and the fire ball mass ℳ is also expressed by the parameter ξ as |N|/ℳ=(1-ξ2)/2ξ. At 1013 eV we have |M|/ℳ{reversed tilde equals}1. This means that an equipartition of energy is approximately valid for the three possible degrees of freedom: the motion of the recoil nucleon, the translational and internal motion of the fire ball. |M|≪ℳ is excluded, unless K is unity, contrary to experiments; 4) when the equipartition holds, the mean value of the transverse momentum is constant and its value is of the order of e{open}0. In Sect. 3, the ℳ and n-dependence of the S-matrix is discussed. And by using the corresponding results we estimate the asymmetry in numbers of particles n1 and n2 emitted in the for- and backward cones. The parameter [〈(n1-n2)2〉/〈(n1+n2)2〉]1/2, a measure of the asymmetry, becomes 1/3 due to statistical fluctuation alone. It becomes larger if the energy transfer Δ0 is not zero. Discussion is also made of the condition by which the average value e{open}0 of the pion energy in the fire ball is constant. The properties of the fire ball seem to be independent from the mechanism of its production. Extending this point of view, the similarity between the multiple production in N-N collisions and N-N annihilation is discussed in Sect. 4. Conclusions are given in Sect. 5. © 1961 Società Italiana di Fisica.Instituto de Física Teórica, São PauloInstituto de Física TeóricaIto, D.Zimerman, A. H.Ragusa, S.Miyazima, T.2022-04-29T08:43:54Z2022-04-29T08:43:54Z1961-06-01info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/article878-902http://dx.doi.org/10.1007/BF02733443Il Nuovo Cimento Series 10, v. 20, n. 5, p. 878-902, 1961.0029-63411827-6121http://hdl.handle.net/11449/23117410.1007/BF027334432-s2.0-51649208882Scopusreponame:Repositório Institucional da UNESPinstname:Universidade Estadual Paulista (UNESP)instacron:UNESPengIl Nuovo Cimento Series 10info:eu-repo/semantics/openAccess2022-04-29T08:43:54Zoai:repositorio.unesp.br:11449/231174Repositório InstitucionalPUBhttp://repositorio.unesp.br/oai/requestopendoar:29462024-08-05T22:00:51.157801Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP)false
dc.title.none.fl_str_mv On the phenomenological analysis of the S-matrix in multiple production
title On the phenomenological analysis of the S-matrix in multiple production
spellingShingle On the phenomenological analysis of the S-matrix in multiple production
Ito, D.
title_short On the phenomenological analysis of the S-matrix in multiple production
title_full On the phenomenological analysis of the S-matrix in multiple production
title_fullStr On the phenomenological analysis of the S-matrix in multiple production
title_full_unstemmed On the phenomenological analysis of the S-matrix in multiple production
title_sort On the phenomenological analysis of the S-matrix in multiple production
author Ito, D.
author_facet Ito, D.
Zimerman, A. H.
Ragusa, S.
Miyazima, T.
author_role author
author2 Zimerman, A. H.
Ragusa, S.
Miyazima, T.
author2_role author
author
author
dc.contributor.none.fl_str_mv Instituto de Física Teórica
dc.contributor.author.fl_str_mv Ito, D.
Zimerman, A. H.
Ragusa, S.
Miyazima, T.
description An attempt is made to analyse the structure of S-matrix elements for multiple production by phenomenological considerations based upon the two center model. We start from two assumptions: 1) the momentum distributions of pions emitted in the for- and backward cones are isotropic in each center-of-mass system (the fire ball rest system) and the average values e{open}0 of the pion energies in this system do not depend on the details of collisions; 2) the mean value of the momentum transfer Δ is always of the order of the nucleon mass M. From these assumptions the following results are derived in Sect. 2: 1) the multiplicity is given by n{reversed tilde equals}ξ√2 E0|Δ|/e{open}0, where ξ is the ratio ℳ/ℳmax of the fire ball mass ℳ and its maximum value ℳmax. Experimentally, ξ{reversed tilde equals}0.5 at 1013 eV; 2) the lower limit of the inelasticity K is given by K≥ξ2. At 1013 eV we have K≥ξ2{reversed tilde equals}0.2 which is consistent with experiments. The relation between multiplicity and inelasticity is discussed; 3) in the center-of-mass system of the fire ball and the recoil nucleon (« isobar system » IBS), the ratio |M|/ℳ of the momentum of the nucleon M and the fire ball mass ℳ is also expressed by the parameter ξ as |N|/ℳ=(1-ξ2)/2ξ. At 1013 eV we have |M|/ℳ{reversed tilde equals}1. This means that an equipartition of energy is approximately valid for the three possible degrees of freedom: the motion of the recoil nucleon, the translational and internal motion of the fire ball. |M|≪ℳ is excluded, unless K is unity, contrary to experiments; 4) when the equipartition holds, the mean value of the transverse momentum is constant and its value is of the order of e{open}0. In Sect. 3, the ℳ and n-dependence of the S-matrix is discussed. And by using the corresponding results we estimate the asymmetry in numbers of particles n1 and n2 emitted in the for- and backward cones. The parameter [〈(n1-n2)2〉/〈(n1+n2)2〉]1/2, a measure of the asymmetry, becomes 1/3 due to statistical fluctuation alone. It becomes larger if the energy transfer Δ0 is not zero. Discussion is also made of the condition by which the average value e{open}0 of the pion energy in the fire ball is constant. The properties of the fire ball seem to be independent from the mechanism of its production. Extending this point of view, the similarity between the multiple production in N-N collisions and N-N annihilation is discussed in Sect. 4. Conclusions are given in Sect. 5. © 1961 Società Italiana di Fisica.
publishDate 1961
dc.date.none.fl_str_mv 1961-06-01
2022-04-29T08:43:54Z
2022-04-29T08:43:54Z
dc.type.status.fl_str_mv info:eu-repo/semantics/publishedVersion
dc.type.driver.fl_str_mv info:eu-repo/semantics/article
format article
status_str publishedVersion
dc.identifier.uri.fl_str_mv http://dx.doi.org/10.1007/BF02733443
Il Nuovo Cimento Series 10, v. 20, n. 5, p. 878-902, 1961.
0029-6341
1827-6121
http://hdl.handle.net/11449/231174
10.1007/BF02733443
2-s2.0-51649208882
url http://dx.doi.org/10.1007/BF02733443
http://hdl.handle.net/11449/231174
identifier_str_mv Il Nuovo Cimento Series 10, v. 20, n. 5, p. 878-902, 1961.
0029-6341
1827-6121
10.1007/BF02733443
2-s2.0-51649208882
dc.language.iso.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv Il Nuovo Cimento Series 10
dc.rights.driver.fl_str_mv info:eu-repo/semantics/openAccess
eu_rights_str_mv openAccess
dc.format.none.fl_str_mv 878-902
dc.source.none.fl_str_mv Scopus
reponame:Repositório Institucional da UNESP
instname:Universidade Estadual Paulista (UNESP)
instacron:UNESP
instname_str Universidade Estadual Paulista (UNESP)
instacron_str UNESP
institution UNESP
reponame_str Repositório Institucional da UNESP
collection Repositório Institucional da UNESP
repository.name.fl_str_mv Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP)
repository.mail.fl_str_mv
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