Fractionalized time reversal, parity and charge conjugation symmetry in topological superconductor: a possible origin of three generations of neutrinos and mass mixing

preprint2016arXivOpen access

Abstract

The existence of three generations of neutrinos(charged leptons/quarks) and their mass mixing are deep mysteries of our universe. Recently, Majorana's spirit returns in modern condensed matter physics -- in the context of topological Majorana zero modes in certain classes of topological superconductors(TSCs). In this paper, we attempt to investigate the topological nature of the neutrino by assuming that a relativistic Majorana fermion can be divided into four topological Majorana zero modes at cutoff energy scale, e.g. planck scale. We begin with an exactly solvable 11D lattice model which realizes a T2=−1T^2=-1 time reversal symmetry protected TSC, and show that a pair of topological Majorana zero modes can realize a T4=−1T^4=-1 time reversal symmetry.Moreover, we find that a pair of topological Majorana zero modes can also realize a P4=−1P^4=-1 parity symmetry and even a nontrivial C‾4=−1\overline C^4=-1 charge conjugation symmetry. Next, we argue that the origin of three generations of neutrinos(charged leptons and quarks) can be naturally explained as three distinguishable ways of forming a pair of complex fermions(with opposite spin polarizations) out of four topological Majorana zero modes, characterized by the T4=−1T^4=-1, (TP)4=−1(TP)^4=-1 and (TC‾)4=−1(T \overline C)^4=-1 fractionalized symmetries that each complex fermion carries at cutoff energy scale. Finally, we use a semiclassical approach to compute the neutrino mass mixing matrix at leading order(LO), e.g., in the absence of CPCP violation correction. We obtain θ12=31.7∘,θ23=45∘θ_{12}=31.7^\circ, θ_{23}=45^\circ and θ13=0∘θ_{13}=0^\circ(the golden ratio pattern), which is consistent with an A5A_5 flavor symmetry pattern. We further predict an exact mass ratio of the three mass eigenstates of neutrinos with m1/m3=m2/m3=3/5m_1/m_3=m_2/m_3=3/\sqrt{5} and an effective mass of neutrinoless double beta decay m0νββ=m1/5m_{0νββ}=m_1/\sqrt{5}.

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