Neutrino mass matrices with Mee=0

被引:12
|
作者
BenTov, Yoni [1 ]
Zee, A. [1 ,2 ]
机构
[1] Univ Calif Santa Barbara, Dept Phys, Santa Barbara, CA 93106 USA
[2] Univ Calif Santa Barbara, Kavli Inst Theoret Phys, Santa Barbara, CA 93106 USA
来源
PHYSICAL REVIEW D | 2011年 / 84卷 / 07期
基金
美国国家科学基金会;
关键词
MU-TAU SYMMETRY; PARAMETRIZATION;
D O I
10.1103/PhysRevD.84.073012
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Motivated by the possibility that the amplitude for neutrinoless double beta decay may be much smaller than the planned sensitivity of future experiments, we study Ansatze for the neutrino mass matrix with M-ee = 0. For the case in which CP is conserved, we consider two classes of real-valued mass matrices: "Class I" defined by vertical bar Me mu vertical bar = vertical bar M-e tau vertical bar, and "Class II" defined by vertical bar M-mu mu vertical bar = vertical bar M-tau tau vertical bar. The important phenomenological distinction between the two is that Class I permits only small values of V-e3 up to similar to 0.03, while Class II admits large values of V-e3 up to its empirical upper limit of 0.22. Then we introduce CP-violating complex phases into the mass matrix. We show that it is possible to have tribimaximal mixing with M-ee = 0 and vertical bar M-mu tau vertical bar = vertical bar M-mu mu vertical bar = vertical bar M-tau tau vertical bar if the Majorana phase angles are +/-pi/4. Alternatively, for smaller values of vertical bar M-mu tau vertical bar = vertical bar M-mu mu vertical bar = vertical bar M-tau tau vertical bar it is possible to obtain vertical bar V-e3 vertical bar similar to 0.2 and generate relatively large CP-violating amplitudes. To eliminate phase redundancy, we emphasize rephasing any mass matrix with M-ee = 0 into a standard form with two complex phases. The discussion alternates between analytical and numerical but remains purely phenomenological, without any attempt to derive mass matrices from a fundamental theory.
引用
收藏
页数:14
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