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A Scenario for Contact Interactions at HERA

The four fermion contact interactions, required to explain the anomalous HERA result, could come from the exchange of new heavy (probably composite) resonances. Depending on their charges and quantum numbers, one gets different scenarios and finds that many of these configurations are unsuitable. Fo...

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Autor principal: Caravaglios, Francesco
Lenguaje:eng
Publicado: 1997
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0370-2693(98)00149-X
http://cds.cern.ch/record/327547
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author Caravaglios, Francesco
author_facet Caravaglios, Francesco
author_sort Caravaglios, Francesco
collection CERN
description The four fermion contact interactions, required to explain the anomalous HERA result, could come from the exchange of new heavy (probably composite) resonances. Depending on their charges and quantum numbers, one gets different scenarios and finds that many of these configurations are unsuitable. For example, new neutral resonances seems to be disfavored by the data coming from the TEVATRON, LEP 2 and atomic parity violation. These experiments allow only few helicity combinations that cannot arise from neutral currents in a natural way. On the contrary, a global large symmetry SU(8) * SU(8) (which is contained in SU(16)) embeds some lepto-quarks of spin 1 that could give suitable four fermion interactions (compatible with all other experiments) if these resonances are the lightest new (probably composite) states with a mass comparable to the scale of the contact interactions.
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institution Organización Europea para la Investigación Nuclear
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spelling cern-3275472023-03-14T17:14:14Zdoi:10.1016/S0370-2693(98)00149-Xhttp://cds.cern.ch/record/327547engCaravaglios, FrancescoA Scenario for Contact Interactions at HERAParticle Physics - PhenomenologyThe four fermion contact interactions, required to explain the anomalous HERA result, could come from the exchange of new heavy (probably composite) resonances. Depending on their charges and quantum numbers, one gets different scenarios and finds that many of these configurations are unsuitable. For example, new neutral resonances seems to be disfavored by the data coming from the TEVATRON, LEP 2 and atomic parity violation. These experiments allow only few helicity combinations that cannot arise from neutral currents in a natural way. On the contrary, a global large symmetry SU(8) * SU(8) (which is contained in SU(16)) embeds some lepto-quarks of spin 1 that could give suitable four fermion interactions (compatible with all other experiments) if these resonances are the lightest new (probably composite) states with a mass comparable to the scale of the contact interactions.The four fermion contact interactions, required to explain the anomalous HERA result, could come from the exchange of new heavy (probably composite) resonances. Depending on their charges and quantum numbers, one gets different scenarios and finds that many of these configurations are unsuitable. For example, new neutral resonances seems to be disfavored by the data coming from the TEVATRON, LEP 2 and atomic parity violation. These experiments allow only few helicity combinations that cannot arise from neutral currents in a natural way. On the contrary, a global large symmetry SU(8) * SU(8) (which is contained in SU(16)) embeds some lepto-quarks of spin 1 that could give suitable four fermion interactions (compatible with all other experiments) if these resonances are the lightest new (probably composite) states with a mass comparable to the scale of the contact interactions.The four-fermion contact interactions, required to explain the anomalous HERA result, could come from the exchange of new heavy (probably composite) resonances. Depending on their charges and quantum numbers, one gets different scenarios and finds that many of these configurations are unsuitable. For example, new neutral resonances seem to be disfavoured by the data coming from the TEVATRON, LEP 2 and atomic parity violation. These experiments allow only few helicity combinations, and these cannot arise from neutral currents in a natural way. On the contrary, a global large symmetry SU (8)× SU (8) (which is contained in SU (16)) embeds some leptoquarks of spin 1 that could give suitable four-fermion interactions (compatible with all other experiments) if these resonances were the lightest new (probably composite) states with a mass comparable to the scale of the contact interactions.hep-ph/9706288CERN-TH-97-104CERN-TH-97-104oai:cds.cern.ch:3275471997-06-10
spellingShingle Particle Physics - Phenomenology
Caravaglios, Francesco
A Scenario for Contact Interactions at HERA
title A Scenario for Contact Interactions at HERA
title_full A Scenario for Contact Interactions at HERA
title_fullStr A Scenario for Contact Interactions at HERA
title_full_unstemmed A Scenario for Contact Interactions at HERA
title_short A Scenario for Contact Interactions at HERA
title_sort scenario for contact interactions at hera
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0370-2693(98)00149-X
http://cds.cern.ch/record/327547
work_keys_str_mv AT caravagliosfrancesco ascenarioforcontactinteractionsathera
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