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Bilarge neutrino mixing and Abelian flavor symmetry

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Bilarge neutrino mixing and Abelian flavor symmetry

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dc.contributor.author Ding, G.J.
dc.contributor.author Morisi, S.
dc.contributor.author Furtado Valle, José Wagner
dc.date.accessioned 2013-11-18T12:04:46Z
dc.date.available 2013-11-18T12:04:46Z
dc.date.issued 2013
dc.identifier.citation Ding, G.J. Morisi, S. Furtado Valle, José Wagner 2013 Bilarge neutrino mixing and Abelian flavor symmetry Physical Review D 87 5 053013-1 053013-13
dc.identifier.uri http://hdl.handle.net/10550/31108
dc.description.abstract We explore two bilarge neutrino mixing Anzatze within the context of Abelian flavor symmetry theories: (BL1) sin theta(12) similar to lambda, sin theta(13) similar to lambda, sin theta(23) similar to lambda, and (BL2) sin theta(12) similar to lambda, sin theta(13) similar to lambda, sin theta(23) similar to 1 ¿ lambda. The first pattern is proposed by two of us and is favored if the atmospheric mixing angle theta(23) lies in the first octant, while the second one is preferred for the second octant of theta(23). In order to reproduce the second texture, we find that the flavor symmetry should be U(1) x Z(m), while for the first pattern the flavor symmetry should be extended to U(1) x Z(m) x Z(n) with m and n of different parity. Explicit models for both mixing patterns are constructed based on the flavor symmetries U(1) x Z(3) x Z(4) and U(1) x Z(2). The models are extended to the quark sector within the framework of SU(5) grand unified theory in order to give a successful description of quark and lepton masses and mixing simultaneously. Phenomenological implications are discussed.
dc.relation.ispartof Physical Review D, 2013, vol. 87, num. 5, p. 053013-1-053013-13
dc.subject Física
dc.title Bilarge neutrino mixing and Abelian flavor symmetry
dc.type journal article es_ES
dc.date.updated 2013-11-18T12:04:46Z
dc.identifier.doi 10.1103/PhysRevD.87.053013
dc.identifier.idgrec 091607
dc.rights.accessRights open access es_ES
dc.identifier.url 10.1103/PhysRevD.87.053013

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