Cargando…
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...
Autor principal: | |
---|---|
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 |
_version_ | 1780890987209424896 |
---|---|
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. |
id | cern-327547 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1997 |
record_format | invenio |
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 AT caravagliosfrancesco scenarioforcontactinteractionsathera |