The inert Zee model
ABSTRACT: We study a realization of the topology of the Zee model for the generation of neutrino masses at one-loop with a minimal set of vector-like fermions. After imposing an exact Z2 symmetry to avoid tree-level Higgs-mediated avor changing neutral currents, one dark matter candidate is obtained...
- Autores:
-
Portillo Quintero, Dilia María
Restrepo Quintero, Diego Alejandro
Zapata Noreña, Óscar Alberto
- Tipo de recurso:
- Article of investigation
- Fecha de publicación:
- 2016
- Institución:
- Universidad de Antioquia
- Repositorio:
- Repositorio UdeA
- Idioma:
- eng
- OAI Identifier:
- oai:bibliotecadigital.udea.edu.co:10495/10967
- Acceso en línea:
- http://hdl.handle.net/10495/10967
- Palabra clave:
- Dark Matter
Double Beta Deca
Masas de neutrinos
Modelo inerte de Zee
- Rights
- openAccess
- License
- Atribución-NoComercial-SinDerivadas 2.5 Colombia
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The inert Zee model |
| title |
The inert Zee model |
| spellingShingle |
The inert Zee model Dark Matter Double Beta Deca Masas de neutrinos Modelo inerte de Zee |
| title_short |
The inert Zee model |
| title_full |
The inert Zee model |
| title_fullStr |
The inert Zee model |
| title_full_unstemmed |
The inert Zee model |
| title_sort |
The inert Zee model |
| dc.creator.fl_str_mv |
Portillo Quintero, Dilia María Restrepo Quintero, Diego Alejandro Zapata Noreña, Óscar Alberto |
| dc.contributor.author.none.fl_str_mv |
Portillo Quintero, Dilia María Restrepo Quintero, Diego Alejandro Zapata Noreña, Óscar Alberto |
| dc.subject.none.fl_str_mv |
Dark Matter Double Beta Deca Masas de neutrinos Modelo inerte de Zee |
| topic |
Dark Matter Double Beta Deca Masas de neutrinos Modelo inerte de Zee |
| description |
ABSTRACT: We study a realization of the topology of the Zee model for the generation of neutrino masses at one-loop with a minimal set of vector-like fermions. After imposing an exact Z2 symmetry to avoid tree-level Higgs-mediated avor changing neutral currents, one dark matter candidate is obtained from the subjacent inert doublet model, but with the presence of new co-annihilating particles. We show that the model is consistent with the constraints coming from lepton avor violation processes, oblique parameters, dark matter and neutrino oscillation data. |
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2016 |
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2016 |
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2019-05-02T19:34:30Z |
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2019-05-02T19:34:30Z |
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info:eu-repo/semantics/article |
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Artículo de investigación |
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Longas, R., Portillo Quintero, D. M., Restrepo Quintero, D. A., & Zapata Noreña, O. A. (2016). The inert Zee model. Journal of High Energy Physics. 2016, 162, 1-20. DOI:10.1007/JHEP03(2016)162 |
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1029-8479 |
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http://hdl.handle.net/10495/10967 |
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10.1007/JHEP03(2016)162 |
| dc.identifier.eissn.none.fl_str_mv |
1126-6708 |
| identifier_str_mv |
Longas, R., Portillo Quintero, D. M., Restrepo Quintero, D. A., & Zapata Noreña, O. A. (2016). The inert Zee model. Journal of High Energy Physics. 2016, 162, 1-20. DOI:10.1007/JHEP03(2016)162 1029-8479 10.1007/JHEP03(2016)162 1126-6708 |
| url |
http://hdl.handle.net/10495/10967 |
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eng |
| language |
eng |
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JHEP |
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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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openAccess |
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application/pdf |
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Springer Verlag |
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Grupo de Fisica y Astrofisica Computacional (FACOM) |
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Reino Unido |
| institution |
Universidad de Antioquia |
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Portillo Quintero, Dilia MaríaRestrepo Quintero, Diego AlejandroZapata Noreña, Óscar Alberto2019-05-02T19:34:30Z2019-05-02T19:34:30Z2016Longas, R., Portillo Quintero, D. M., Restrepo Quintero, D. A., & Zapata Noreña, O. A. (2016). The inert Zee model. Journal of High Energy Physics. 2016, 162, 1-20. DOI:10.1007/JHEP03(2016)1621029-8479http://hdl.handle.net/10495/1096710.1007/JHEP03(2016)1621126-6708ABSTRACT: We study a realization of the topology of the Zee model for the generation of neutrino masses at one-loop with a minimal set of vector-like fermions. After imposing an exact Z2 symmetry to avoid tree-level Higgs-mediated avor changing neutral currents, one dark matter candidate is obtained from the subjacent inert doublet model, but with the presence of new co-annihilating particles. We show that the model is consistent with the constraints coming from lepton avor violation processes, oblique parameters, dark matter and neutrino oscillation data.application/pdfengSpringer VerlagGrupo de Fisica y Astrofisica Computacional (FACOM)Reino Unidoinfo: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/Dark MatterDouble Beta DecaMasas de neutrinosModelo inerte de ZeeThe inert Zee modelJHEPJournal of High Energy Physics1202016162ORIGINALRestrepoDiego_2016_InertZeeModel.pdfRestrepoDiego_2016_InertZeeModel.pdfArtículo de investigaciónapplication/pdf1019754http://bibliotecadigital.udea.edu.co/bitstream/10495/10967/1/RestrepoDiego_2016_InertZeeModel.pdf99644aec54ce5a669bca6568860201aeMD51LICENSElicense.txtlicense.txttext/plain; charset=utf-81748http://bibliotecadigital.udea.edu.co/bitstream/10495/10967/5/license.txt8a4605be74aa9ea9d79846c1fba20a33MD55CC-LICENSElicense_urllicense_urltext/plain; charset=utf-849http://bibliotecadigital.udea.edu.co/bitstream/10495/10967/2/license_url4afdbb8c545fd630ea7db775da747b2fMD52license_textlicense_texttext/html; charset=utf-80http://bibliotecadigital.udea.edu.co/bitstream/10495/10967/3/license_textd41d8cd98f00b204e9800998ecf8427eMD53license_rdflicense_rdfLicenciaapplication/rdf+xml; charset=utf-80http://bibliotecadigital.udea.edu.co/bitstream/10495/10967/4/license_rdfd41d8cd98f00b204e9800998ecf8427eMD5410495/10967oai:bibliotecadigital.udea.edu.co:10495/109672021-05-16 11:49:07.957Repositorio Institucional Universidad de Antioquiaandres.perez@udea.edu.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 |