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Some information from nucleon-antinucleon annihilation at rest: e+e- annihilation, hadronic fragmentation, and deep inelastic scattering structure function
The experimental spectra of charged pions in NN annihilation at rest are described in a model of quasi-two-body decays. The same model predicts the pi /sup 0/, s, rho 's and omega 's spectra. These calculations are used to determine, in the vector dominance model, the pion spectra in the e...
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Lenguaje: | eng |
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CERN
1974
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Acceso en línea: | https://dx.doi.org/10.5170/CERN-1974-018.43 http://cds.cern.ch/record/867129 |
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author | Pelaquier, E |
author_facet | Pelaquier, E |
author_sort | Pelaquier, E |
collection | CERN |
description | The experimental spectra of charged pions in NN annihilation at rest are described in a model of quasi-two-body decays. The same model predicts the pi /sup 0/, s, rho 's and omega 's spectra. These calculations are used to determine, in the vector dominance model, the pion spectra in the e/sup +/e/sup -/ annihilation at the same energy. The NN system is then used as a heavy hadron in order to describe, in a model-independent way: the projectile fragmentation part in inclusive reactions; the valence part of the deep inelastic structure function. (0 refs). |
id | cern-867129 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1974 |
publisher | CERN |
record_format | invenio |
spelling | cern-8671292019-09-30T06:29:59Zdoi:10.5170/CERN-1974-018.43http://cds.cern.ch/record/867129engPelaquier, ESome information from nucleon-antinucleon annihilation at rest: e+e- annihilation, hadronic fragmentation, and deep inelastic scattering structure functionParticle Physics - PhenomenologyThe experimental spectra of charged pions in NN annihilation at rest are described in a model of quasi-two-body decays. The same model predicts the pi /sup 0/, s, rho 's and omega 's spectra. These calculations are used to determine, in the vector dominance model, the pion spectra in the e/sup +/e/sup -/ annihilation at the same energy. The NN system is then used as a heavy hadron in order to describe, in a model-independent way: the projectile fragmentation part in inclusive reactions; the valence part of the deep inelastic structure function. (0 refs).CERNoai:cds.cern.ch:8671291974 |
spellingShingle | Particle Physics - Phenomenology Pelaquier, E Some information from nucleon-antinucleon annihilation at rest: e+e- annihilation, hadronic fragmentation, and deep inelastic scattering structure function |
title | Some information from nucleon-antinucleon annihilation at rest: e+e- annihilation, hadronic fragmentation, and deep inelastic scattering structure function |
title_full | Some information from nucleon-antinucleon annihilation at rest: e+e- annihilation, hadronic fragmentation, and deep inelastic scattering structure function |
title_fullStr | Some information from nucleon-antinucleon annihilation at rest: e+e- annihilation, hadronic fragmentation, and deep inelastic scattering structure function |
title_full_unstemmed | Some information from nucleon-antinucleon annihilation at rest: e+e- annihilation, hadronic fragmentation, and deep inelastic scattering structure function |
title_short | Some information from nucleon-antinucleon annihilation at rest: e+e- annihilation, hadronic fragmentation, and deep inelastic scattering structure function |
title_sort | some information from nucleon-antinucleon annihilation at rest: e+e- annihilation, hadronic fragmentation, and deep inelastic scattering structure function |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.5170/CERN-1974-018.43 http://cds.cern.ch/record/867129 |
work_keys_str_mv | AT pelaquiere someinformationfromnucleonantinucleonannihilationatresteeannihilationhadronicfragmentationanddeepinelasticscatteringstructurefunction |