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Complete Cubic and Quartic Couplings of 16 and $\bar{16}$ in SO(10) Unification
A recently derived basic theorem on the decomposition of SO(2N) vertices is used to obtain a complete analytic determination of all SO(10) invariant cubic superpotential couplings involving $16_{\pm}$ semispinors of SO(10) chirality $\pm$ and tensor representations. In addition to the superpotential...
Autores principales: | , |
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Lenguaje: | eng |
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2001
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/S0550-3213(01)00493-X http://cds.cern.ch/record/519469 |
_version_ | 1780897765378752512 |
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author | Nath, Pran Syed, Raza M. |
author_facet | Nath, Pran Syed, Raza M. |
author_sort | Nath, Pran |
collection | CERN |
description | A recently derived basic theorem on the decomposition of SO(2N) vertices is used to obtain a complete analytic determination of all SO(10) invariant cubic superpotential couplings involving $16_{\pm}$ semispinors of SO(10) chirality $\pm$ and tensor representations. In addition to the superpotential couplings computed previously using the basic theorem involving the 10, 120 and $\bar{126}$ tensor representations we compute here couplings involving the 1, 45 and 210 dimensional tensor representations, i.e., we compute the $\bar{16}_{\mp}16_{\pm}1$,$\bar{16}_{\mp}16_{\pm}45$ and $\bar{16}_{\mp}16_{\pm}210$ Higgs couplings in the superpotential. A complete determination of dimension five operators in the superpotential arising from the mediation of the 1, 45 and 210 dimensional representations is also given. The vector couplings $\bar{16}_{\pm}16_{\pm}1$, $\bar{16}_{\pm}16_{\pm}45$ and $\bar{16}_{\pm}16_{\pm}210$ are also analyzed. The role of large tensor representations and the possible application of results derived here in model building are discussed. |
id | cern-519469 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2001 |
record_format | invenio |
spelling | cern-5194692023-03-14T18:46:15Zdoi:10.1016/S0550-3213(01)00493-Xhttp://cds.cern.ch/record/519469engNath, PranSyed, Raza M.Complete Cubic and Quartic Couplings of 16 and $\bar{16}$ in SO(10) UnificationParticle Physics - TheoryA recently derived basic theorem on the decomposition of SO(2N) vertices is used to obtain a complete analytic determination of all SO(10) invariant cubic superpotential couplings involving $16_{\pm}$ semispinors of SO(10) chirality $\pm$ and tensor representations. In addition to the superpotential couplings computed previously using the basic theorem involving the 10, 120 and $\bar{126}$ tensor representations we compute here couplings involving the 1, 45 and 210 dimensional tensor representations, i.e., we compute the $\bar{16}_{\mp}16_{\pm}1$,$\bar{16}_{\mp}16_{\pm}45$ and $\bar{16}_{\mp}16_{\pm}210$ Higgs couplings in the superpotential. A complete determination of dimension five operators in the superpotential arising from the mediation of the 1, 45 and 210 dimensional representations is also given. The vector couplings $\bar{16}_{\pm}16_{\pm}1$, $\bar{16}_{\pm}16_{\pm}45$ and $\bar{16}_{\pm}16_{\pm}210$ are also analyzed. The role of large tensor representations and the possible application of results derived here in model building are discussed.A recently derived basic theorem on the decomposition of SO(2N) vertices is used to obtain a complete analytic determination of all SO(10) invariant cubic superpotential couplings involving $16_{\pm}$ semispinors of SO(10) chirality $\pm$ and tensor representations. In addition to the superpotential couplings computed previously using the basic theorem involving the 10, 120 and $\bar{126}$ tensor representations we compute here couplings involving the 1, 45 and 210 dimensional tensor representations, i.e., we compute the $\bar{16}_{\mp}16_{\pm}1$,$\bar{16}_{\mp}16_{\pm}45$ and $\bar{16}_{\mp}16_{\pm}210$ Higgs couplings in the superpotential. A complete determination of dimension five operators in the superpotential arising from the mediation of the 1, 45 and 210 dimensional representations is also given. The vector couplings $\bar{16}_{\pm}16_{\pm}1$, $\bar{16}_{\pm}16_{\pm}45$ and $\bar{16}_{\pm}16_{\pm}210$ are also analyzed. The role of large tensor representations and the possible application of results derived here in model building are discussed.hep-th/0109116CERN-TH-2001-237NUB-3220CERN-TH-2001-237oai:cds.cern.ch:5194692001 |
spellingShingle | Particle Physics - Theory Nath, Pran Syed, Raza M. Complete Cubic and Quartic Couplings of 16 and $\bar{16}$ in SO(10) Unification |
title | Complete Cubic and Quartic Couplings of 16 and $\bar{16}$ in SO(10) Unification |
title_full | Complete Cubic and Quartic Couplings of 16 and $\bar{16}$ in SO(10) Unification |
title_fullStr | Complete Cubic and Quartic Couplings of 16 and $\bar{16}$ in SO(10) Unification |
title_full_unstemmed | Complete Cubic and Quartic Couplings of 16 and $\bar{16}$ in SO(10) Unification |
title_short | Complete Cubic and Quartic Couplings of 16 and $\bar{16}$ in SO(10) Unification |
title_sort | complete cubic and quartic couplings of 16 and $\bar{16}$ in so(10) unification |
topic | Particle Physics - Theory |
url | https://dx.doi.org/10.1016/S0550-3213(01)00493-X http://cds.cern.ch/record/519469 |
work_keys_str_mv | AT nathpran completecubicandquarticcouplingsof16andbar16inso10unification AT syedrazam completecubicandquarticcouplingsof16andbar16inso10unification |