Generalized μ-τ symmetry and discrete subgroups of O(3)

被引:58
作者
Joshipura, Anjan S. [1 ]
Patel, Ketan M. [2 ]
机构
[1] Phys Res Lab, Ahmadabad 380009, Gujarat, India
[2] Ist Nazl Fis Nucl, Sez Padova, I-35131 Padua, Italy
关键词
FLAVOR SYMMETRIES; NEUTRINO; LEPTONS;
D O I
10.1016/j.physletb.2015.07.062
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
The generalized mu-tau interchange symmetry in the leptonic mixing matrix U corresponds to the relations: vertical bar U-mu i vertical bar=vertical bar U-tau i vertical bar with i = 1, 2, 3. It predicts maximal atmospheric mixing and maximal Dirac CP violation given theta(13) not equal 0. We show that the generalized mu-tau symmetry can arise if the charged lepton and neutrino mass matrices are invariant under specific residual symmetries contained in the finite discrete subgroups of O (3). The groups A(4), S-4 and A(5) are the only such groups which can entirely fix U at the leading order. The neutrinos can be (a) non-degenerate or (b) partially degenerate depending on the choice of their residual symmetries. One obtains either vanishing or very large theta(13) in case of (a) while only A(5) can provide theta(13) close to its experimental value in the case (b). We provide an explicit model based on A(5) and discuss a class of perturbations which can generate fully realistic neutrino masses and mixing maintaining the generalized mu-tau symmetry in U. Our approach provides generalization of some of the ideas proposed earlier in order to obtain the predictions,theta(23)=pi/4 and delta(CP)=+/-pi/2. (C) 2015 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY license
引用
收藏
页码:159 / 166
页数:8
相关论文
共 59 条
[1]   Observation of Electron Neutrino Appearance in a Muon Neutrino Beam [J].
Abe, K. ;
Adam, J. ;
Aihara, H. ;
Akiri, T. ;
Andreopoulos, C. ;
Aoki, S. ;
Ariga, A. ;
Ariga, T. ;
Assylbekov, S. ;
Autiero, D. ;
Barbi, M. ;
Barker, G. J. ;
Barr, G. ;
Bass, M. ;
Batkiewicz, M. ;
Bay, F. ;
Bentham, S. W. ;
Berardi, V. ;
Berger, B. E. ;
Berkman, S. ;
Bertram, I. ;
Bhadra, S. ;
Blaszczyk, F. D. M. ;
Blondel, A. ;
Bojechko, C. ;
Bordoni, S. ;
Boyd, S. B. ;
Brailsford, D. ;
Bravar, A. ;
Bronner, C. ;
Buchanan, N. ;
Calland, R. G. ;
Caravaca Rodriguez, J. ;
Cartwright, S. L. ;
Castillo, R. ;
Catanesi, M. G. ;
Cervera, A. ;
Cherdack, D. ;
Christodoulou, G. ;
Clifton, A. ;
Coleman, J. ;
Coleman, S. J. ;
Collazuol, G. ;
Connolly, K. ;
Cremonesi, L. ;
Dabrowska, A. ;
Danko, I. ;
Das, R. ;
Davis, S. ;
de Perio, P. .
PHYSICAL REVIEW LETTERS, 2014, 112 (06)
[2]   Tri-bimaximal neutrino mixing and discrete flavour symmetries [J].
Altarelli, Guido ;
Feruglio, Ferruccio ;
Merlo, Luca .
FORTSCHRITTE DER PHYSIK-PROGRESS OF PHYSICS, 2013, 61 (4-5) :507-534
[3]   Discrete flavor symmetries and models of neutrino mixing [J].
Altarelli, Guido ;
Feruglio, Ferruccio .
REVIEWS OF MODERN PHYSICS, 2010, 82 (03) :2701-2729
[4]  
[Anonymous], 2015, ARXIV150408331HEPPH
[5]   Underlying A4 symmetry for the neutrino mass matrix and the quark mixing matrix [J].
Babu, KS ;
Ma, E ;
Valle, JWF .
PHYSICS LETTERS B, 2003, 552 (3-4) :207-213
[6]  
Ballett P., 2015, ARXIV150307543HEPPH
[7]   Status of three-neutrino oscillation parameters, circa 2013 [J].
Capozzi, F. ;
Fogli, G. L. ;
Lisi, E. ;
Marrone, A. ;
Montanino, D. ;
Palazzo, A. .
PHYSICAL REVIEW D, 2014, 89 (09)
[8]   A golden A5 model of leptons with a minimal NLO correction [J].
Cooper, Iain K. ;
King, Stephen F. ;
Stuart, Alexander J. .
NUCLEAR PHYSICS B, 2013, 875 (03) :650-677
[9]  
Dev A., 2015, ARXIV150404034HEPPH
[10]  
Di Iura A., 2015, ARXIV150304140HEPPH