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Fermions on the electroweak string
We construct a simple class of exact solutions of the electroweak theory including the naked Z--string and fermion fields. It consists in the Z--string configuration (\phi,Z_\theta), the {\it time} and z components of the neutral gauge bosons (Z_{0,3},A_{0,3}) and a fermion condensate (lepton or qua...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
1994
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/0370-2693(95)00074-U http://cds.cern.ch/record/272835 |
_version_ | 1780887284554399744 |
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author | Moreno, J.M. Oaknin, D.H. Quiros, M. |
author_facet | Moreno, J.M. Oaknin, D.H. Quiros, M. |
author_sort | Moreno, J.M. |
collection | CERN |
description | We construct a simple class of exact solutions of the electroweak theory including the naked Z--string and fermion fields. It consists in the Z--string configuration (\phi,Z_\theta), the {\it time} and z components of the neutral gauge bosons (Z_{0,3},A_{0,3}) and a fermion condensate (lepton or quark) zero mode. The Z--string is not altered (no feed back from the rest of fields on the Z--string) while fermion condensates are zero modes of the Dirac equation in the presence of the Z--string background (no feed back from the {\it time} and z components of the neutral gauge bosons on the fermion fields). For the case of the n--vortex Z--string the number of zero modes found for charged leptons and quarks is (according to previous results by Jackiw and Rossi) equal to |n|, while for (massless) neutrinos is |n|-1. The presence of fermion fields in its core make the obtained configuration a superconducting string, but their presence (as well as that of Z_{0,3},A_{0,3}) does not enhance the stability of the Z--string. |
id | cern-272835 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1994 |
record_format | invenio |
spelling | cern-2728352023-03-14T18:59:45Zdoi:10.1016/0370-2693(95)00074-Uhttp://cds.cern.ch/record/272835engMoreno, J.M.Oaknin, D.H.Quiros, M.Fermions on the electroweak stringParticle Physics - PhenomenologyWe construct a simple class of exact solutions of the electroweak theory including the naked Z--string and fermion fields. It consists in the Z--string configuration (\phi,Z_\theta), the {\it time} and z components of the neutral gauge bosons (Z_{0,3},A_{0,3}) and a fermion condensate (lepton or quark) zero mode. The Z--string is not altered (no feed back from the rest of fields on the Z--string) while fermion condensates are zero modes of the Dirac equation in the presence of the Z--string background (no feed back from the {\it time} and z components of the neutral gauge bosons on the fermion fields). For the case of the n--vortex Z--string the number of zero modes found for charged leptons and quarks is (according to previous results by Jackiw and Rossi) equal to |n|, while for (massless) neutrinos is |n|-1. The presence of fermion fields in its core make the obtained configuration a superconducting string, but their presence (as well as that of Z_{0,3},A_{0,3}) does not enhance the stability of the Z--string.We construct a simple class of exact solutions of the electroweak theory including the naked $Z$--string and fermion fields. It consists in the $Z$--string configuration ($\phi,Z_\theta$), the {\it time} and $z$ components of the neutral gauge bosons ($Z_{0,3},A_{0,3}$) and a fermion condensate (lepton or quark) zero mode. The $Z$--string is not altered (no feed back from the rest of fields on the $Z$--string) while fermion condensates are zero modes of the Dirac equation in the presence of the $Z$--string background (no feed back from the {\it time} and $z$ components of the neutral gauge bosons on the fermion fields). For the case of the $n$--vortex $Z$--string the number of zero modes found for charged leptons and quarks is (according to previous results by Jackiw and Rossi) equal to $|n|$, while for (massless) neutrinos is $|n|-1$. The presence of fermion fields in its core make the obtained configuration a superconducting string, but their presence (as well as that of $Z_{0,3},A_{0,3}$) does not enhance the stability of the $Z$--string.We construct a simple class of exact solutions of the electroweak theory including the naked Z -string and fermion fields. It consists in the Z -string configuration (φ, Z θ ), the time and z components of the neutral gauge bosons Z 0,3 , A 0,3 ) and a fermion condensate (lepton or quark) zero mode. The Z -string is not altered (no feedback from the rest of fields on the Z -string) while fermion condensates are zero modes of the Dirac equation in the presence of the Z -string background (no feedback from the time and z components of the neutral gauge bosons on the fermion fields). For the case of the n -vortex Z -string the number of zero modes found for charged leptons and quarks is (according to previous results by Jackiw and Rossi) equal to | n |, while for (massless) neutrinos it is | n | − 1. The presence of fernion fields in its core makes the obtained configuration a superconducting string, but their presence (as well as that of Z 0,3 , A 0,3 ) does not enhance the stability of the Z -string.hep-ph/9411411CERN-TH-7511-94IEM-FT-95-94ACERN-TH-7511-94IEM-FT-94oai:cds.cern.ch:2728351994-11-28 |
spellingShingle | Particle Physics - Phenomenology Moreno, J.M. Oaknin, D.H. Quiros, M. Fermions on the electroweak string |
title | Fermions on the electroweak string |
title_full | Fermions on the electroweak string |
title_fullStr | Fermions on the electroweak string |
title_full_unstemmed | Fermions on the electroweak string |
title_short | Fermions on the electroweak string |
title_sort | fermions on the electroweak string |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1016/0370-2693(95)00074-U http://cds.cern.ch/record/272835 |
work_keys_str_mv | AT morenojm fermionsontheelectroweakstring AT oaknindh fermionsontheelectroweakstring AT quirosm fermionsontheelectroweakstring |