SU(3)c⊗SU(3)L⊗U(1)x as an SU(6)⊗U(1)x subgroup
ABSTRACT: An extension of the standard model to the local gauge group SU(3) c ^ SU(3)L ^ U(1)X as a family independent model is presented. The mass scales, the gauge boson masses, and the masses for the spin 1/2 particles in the model are studied. The mass differences between the up and down quark s...
- Autores:
-
Martínez Martínez, Roberto
Ponce Gutiérrez, William Antonio
Sánchez Duque, Luis Alberto
- Tipo de recurso:
- Article of investigation
- Fecha de publicación:
- 2002
- Institución:
- Universidad de Antioquia
- Repositorio:
- Repositorio UdeA
- Idioma:
- eng
- OAI Identifier:
- oai:bibliotecadigital.udea.edu.co:10495/13358
- Acceso en línea:
- http://hdl.handle.net/10495/13358
- Palabra clave:
- Fermion
Gauge boson
Gauge field theory
Interpretation of experime
Mass spectrum
Mixing angle
Numerical calculations
SU(3)xSU(2)xU(1)
Cálculos numericos
Espectro de masas
- Rights
- openAccess
- License
- Atribución-NoComercial-SinDerivadas 2.5 Colombia
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| dc.title.spa.fl_str_mv |
SU(3)c⊗SU(3)L⊗U(1)x as an SU(6)⊗U(1)x subgroup |
| title |
SU(3)c⊗SU(3)L⊗U(1)x as an SU(6)⊗U(1)x subgroup |
| spellingShingle |
SU(3)c⊗SU(3)L⊗U(1)x as an SU(6)⊗U(1)x subgroup Fermion Gauge boson Gauge field theory Interpretation of experime Mass spectrum Mixing angle Numerical calculations SU(3)xSU(2)xU(1) Cálculos numericos Espectro de masas |
| title_short |
SU(3)c⊗SU(3)L⊗U(1)x as an SU(6)⊗U(1)x subgroup |
| title_full |
SU(3)c⊗SU(3)L⊗U(1)x as an SU(6)⊗U(1)x subgroup |
| title_fullStr |
SU(3)c⊗SU(3)L⊗U(1)x as an SU(6)⊗U(1)x subgroup |
| title_full_unstemmed |
SU(3)c⊗SU(3)L⊗U(1)x as an SU(6)⊗U(1)x subgroup |
| title_sort |
SU(3)c⊗SU(3)L⊗U(1)x as an SU(6)⊗U(1)x subgroup |
| dc.creator.fl_str_mv |
Martínez Martínez, Roberto Ponce Gutiérrez, William Antonio Sánchez Duque, Luis Alberto |
| dc.contributor.author.none.fl_str_mv |
Martínez Martínez, Roberto Ponce Gutiérrez, William Antonio Sánchez Duque, Luis Alberto |
| dc.subject.none.fl_str_mv |
Fermion Gauge boson Gauge field theory Interpretation of experime Mass spectrum Mixing angle Numerical calculations SU(3)xSU(2)xU(1) Cálculos numericos Espectro de masas |
| topic |
Fermion Gauge boson Gauge field theory Interpretation of experime Mass spectrum Mixing angle Numerical calculations SU(3)xSU(2)xU(1) Cálculos numericos Espectro de masas |
| description |
ABSTRACT: An extension of the standard model to the local gauge group SU(3) c ^ SU(3)L ^ U(1)X as a family independent model is presented. The mass scales, the gauge boson masses, and the masses for the spin 1/2 particles in the model are studied. The mass differences between the up and down quark sectors, between the quarks and leptons, and between the charged and neutral leptons in one family are analyzed. The existence of two Dirac neutrinos for each family, one light and one very heavy, is predicted. By using experimental results from CERN LEP, SLC and atomic parity violation we constrain the mixing angle between the two neutral currents and the mass of the additional neutral gauge boson to be 20.00015<sin u<0 and 1.5 TeV<MZ2 at 95% C.L. |
| publishDate |
2002 |
| dc.date.issued.none.fl_str_mv |
2002 |
| dc.date.accessioned.none.fl_str_mv |
2020-01-18T03:36:01Z |
| dc.date.available.none.fl_str_mv |
2020-01-18T03:36:01Z |
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info:eu-repo/semantics/article |
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http://purl.org/coar/version/c_970fb48d4fbd8a85 http://purl.org/coar/version/c_71e4c1898caa6e32 |
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http://purl.org/coar/resource_type/c_2df8fbb1 |
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https://purl.org/redcol/resource_type/ART |
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Artículo de investigación |
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http://purl.org/coar/resource_type/c_2df8fbb1 |
| dc.identifier.citation.spa.fl_str_mv |
Martínez-Martínez, R., Ponce-Gutiérrez, W. A., & Sánchez-Duque, L. A. (2001). SU(3)c⊗SU(3)L⊗U(1)x as an SU(6)⊗U(1)x subgroup. Physical Review D, 65,(5), 1-9. doi: 10.1103/PhysRevD.65.055013 |
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2470-0010 |
| dc.identifier.uri.none.fl_str_mv |
http://hdl.handle.net/10495/13358 |
| dc.identifier.doi.none.fl_str_mv |
10.1103/PhysRevD.65.055013 |
| dc.identifier.eissn.none.fl_str_mv |
2470-0029 |
| identifier_str_mv |
Martínez-Martínez, R., Ponce-Gutiérrez, W. A., & Sánchez-Duque, L. A. (2001). SU(3)c⊗SU(3)L⊗U(1)x as an SU(6)⊗U(1)x subgroup. Physical Review D, 65,(5), 1-9. doi: 10.1103/PhysRevD.65.055013 2470-0010 10.1103/PhysRevD.65.055013 2470-0029 |
| url |
http://hdl.handle.net/10495/13358 |
| dc.language.iso.spa.fl_str_mv |
eng |
| language |
eng |
| dc.relation.ispartofjournalabbrev.spa.fl_str_mv |
Phys. Rev. D |
| dc.rights.*.fl_str_mv |
Atribución-NoComercial-SinDerivadas 2.5 Colombia |
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info:eu-repo/semantics/openAccess |
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http://creativecommons.org/licenses/by-nc-nd/2.5/co/ |
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http://purl.org/coar/access_right/c_abf2 |
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Atribución-NoComercial-SinDerivadas 2.5 Colombia http://creativecommons.org/licenses/by-nc-nd/2.5/co/ http://purl.org/coar/access_right/c_abf2 https://creativecommons.org/licenses/by-nc-nd/4.0/ |
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openAccess |
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application/pdf |
| dc.publisher.spa.fl_str_mv |
American Physical Society |
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Estados Unidos |
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Universidad de Antioquia |
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Martínez Martínez, RobertoPonce Gutiérrez, William AntonioSánchez Duque, Luis Alberto2020-01-18T03:36:01Z2020-01-18T03:36:01Z2002Martínez-Martínez, R., Ponce-Gutiérrez, W. A., & Sánchez-Duque, L. A. (2001). SU(3)c⊗SU(3)L⊗U(1)x as an SU(6)⊗U(1)x subgroup. Physical Review D, 65,(5), 1-9. doi: 10.1103/PhysRevD.65.0550132470-0010http://hdl.handle.net/10495/1335810.1103/PhysRevD.65.0550132470-0029ABSTRACT: An extension of the standard model to the local gauge group SU(3) c ^ SU(3)L ^ U(1)X as a family independent model is presented. The mass scales, the gauge boson masses, and the masses for the spin 1/2 particles in the model are studied. The mass differences between the up and down quark sectors, between the quarks and leptons, and between the charged and neutral leptons in one family are analyzed. The existence of two Dirac neutrinos for each family, one light and one very heavy, is predicted. By using experimental results from CERN LEP, SLC and atomic parity violation we constrain the mixing angle between the two neutral currents and the mass of the additional neutral gauge boson to be 20.00015<sin u<0 and 1.5 TeV<MZ2 at 95% C.L.application/pdfengAmerican Physical SocietyEstados Unidosinfo:eu-repo/semantics/articlehttp://purl.org/coar/resource_type/c_2df8fbb1https://purl.org/redcol/resource_type/ARTArtículo de investigaciónhttp://purl.org/coar/version/c_970fb48d4fbd8a85http://purl.org/coar/version/c_71e4c1898caa6e32Atribución-NoComercial-SinDerivadas 2.5 Colombiainfo:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by-nc-nd/2.5/co/http://purl.org/coar/access_right/c_abf2https://creativecommons.org/licenses/by-nc-nd/4.0/FermionGauge bosonGauge field theoryInterpretation of experimeMass spectrumMixing angleNumerical calculationsSU(3)xSU(2)xU(1)Cálculos numericosEspectro de masasSU(3)c⊗SU(3)L⊗U(1)x as an SU(6)⊗U(1)x subgroupPhys. Rev. DPhysical Review D1165CC-LICENSElicense_urllicense_urlArtículo de investigacióntext/plain; charset=utf-849http://bibliotecadigital.udea.edu.co/bitstream/10495/13358/2/license_url4afdbb8c545fd630ea7db775da747b2fMD52license_textlicense_texttext/html; charset=utf-80http://bibliotecadigital.udea.edu.co/bitstream/10495/13358/3/license_textd41d8cd98f00b204e9800998ecf8427eMD53license_rdflicense_rdfapplication/rdf+xml; charset=utf-80http://bibliotecadigital.udea.edu.co/bitstream/10495/13358/4/license_rdfd41d8cd98f00b204e9800998ecf8427eMD54LICENSElicense.txtlicense.txttext/plain; charset=utf-81748http://bibliotecadigital.udea.edu.co/bitstream/10495/13358/5/license.txt8a4605be74aa9ea9d79846c1fba20a33MD55ORIGINALPonceWilliam_2002_ subgroup.pdfPonceWilliam_2002_ subgroup.pdfArtículo de investigaciónapplication/pdf141841http://bibliotecadigital.udea.edu.co/bitstream/10495/13358/1/PonceWilliam_2002_%20subgroup.pdf0be9c7ce7aa08afe963e2f8573e0ecedMD5110495/13358oai:bibliotecadigital.udea.edu.co:10495/133582021-05-16 11:48:15.04Repositorio Institucional Universidad de Antioquiaandres.perez@udea.edu.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 |