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Isospin bounds for energy partition in $\overline{\e}$ and $\overline{N}$ annihilation

In reactions such as ee to anything, NN to anything, the final state (neglecting secondary isospin violating decays) is customarily supposed to have isospin zero or one. It is shown that for such states the average fraction (X) of the energy carried away by neutral pions is bounded by X<(9+ squar...

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Detalles Bibliográficos
Autores principales: Bell, J S, Karl, G, Llewellyn Smith, Christopher Hubert
Lenguaje:eng
Publicado: 1974
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0370-2693(74)90063-X
http://cds.cern.ch/record/873533
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author Bell, J S
Karl, G
Llewellyn Smith, Christopher Hubert
author_facet Bell, J S
Karl, G
Llewellyn Smith, Christopher Hubert
author_sort Bell, J S
collection CERN
description In reactions such as ee to anything, NN to anything, the final state (neglecting secondary isospin violating decays) is customarily supposed to have isospin zero or one. It is shown that for such states the average fraction (X) of the energy carried away by neutral pions is bounded by X<(9+ square root 41)/20 approximately=0.77, when I/sub 3/=0 (e.g., for ee, pp, nn) and by X>(11- square root 41)/40 approximately=0.115, when I/sub 3/=+or-1 (e.g., for pn or np). (4 refs).
id cern-873533
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1974
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spelling cern-8735332019-09-30T06:29:59Zdoi:10.1016/0370-2693(74)90063-Xhttp://cds.cern.ch/record/873533engBell, J SKarl, GLlewellyn Smith, Christopher HubertIsospin bounds for energy partition in $\overline{\e}$ and $\overline{N}$ annihilationParticle Physics - TheoryIn reactions such as ee to anything, NN to anything, the final state (neglecting secondary isospin violating decays) is customarily supposed to have isospin zero or one. It is shown that for such states the average fraction (X) of the energy carried away by neutral pions is bounded by X<(9+ square root 41)/20 approximately=0.77, when I/sub 3/=0 (e.g., for ee, pp, nn) and by X>(11- square root 41)/40 approximately=0.115, when I/sub 3/=+or-1 (e.g., for pn or np). (4 refs).oai:cds.cern.ch:8735331974
spellingShingle Particle Physics - Theory
Bell, J S
Karl, G
Llewellyn Smith, Christopher Hubert
Isospin bounds for energy partition in $\overline{\e}$ and $\overline{N}$ annihilation
title Isospin bounds for energy partition in $\overline{\e}$ and $\overline{N}$ annihilation
title_full Isospin bounds for energy partition in $\overline{\e}$ and $\overline{N}$ annihilation
title_fullStr Isospin bounds for energy partition in $\overline{\e}$ and $\overline{N}$ annihilation
title_full_unstemmed Isospin bounds for energy partition in $\overline{\e}$ and $\overline{N}$ annihilation
title_short Isospin bounds for energy partition in $\overline{\e}$ and $\overline{N}$ annihilation
title_sort isospin bounds for energy partition in $\overline{\e}$ and $\overline{n}$ annihilation
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/0370-2693(74)90063-X
http://cds.cern.ch/record/873533
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AT karlg isospinboundsforenergypartitioninoverlineeandoverlinenannihilation
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