2014Chinese Journal of PhysicsRequires access

Nonzero θ_(13), CP Violation, and Broken μ-τ Symmetry

Asan Damanik

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Abstract

Recently, evidence for a nonzero and relatively large θ_(13), as shown from the latest experimental results, has a serious implication on the well-known neutrino mixing matrix and the existence of CP violation in the neutrino sector (J_(CP)≠0). One of the well-known mixing matricies is the tribimaximal (TBM) neutrino mixing matrix that predicts the mixing angle θ_(13) = 0 and J_(CP) = 0. In order to accommodate the nonzero θ_(13) and CP violation, we modified the TBM by introducing a simple perturbation matrix into the TBM matrix that can produce θ_(13) = 7:89°, which is in agreement with the present experimental results, and the Dirac phase δ ≈ π/2, and JCP ≈ 0:0222. The obtained neutrino mass matrix from the modified TBM with both nonzero θ_(13) and δ is the complex neutrino mass matrix. If we impose μ-τ symmetry, as a constraint into the neutrino mass matrix, one finds that the J_(CP) = 0, which implies that CP violation cannot be accommodated in the μ-τ symmetry scheme. We break the μ-τ symmetry softly by introducing a small parameter x to perturb the neutrino mass matrix with the constraint that the trace of the perturbed neutrino mass matrix remains constant.

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What this paper is about

Recently, evidence for a nonzero and relatively large θ_(13), as shown from the latest experimental results, has a serious implication on the well-known neutrino mixing matrix and the existence of CP violation in the neutrino sector (J_(CP)≠0). One of the well-known mixing matricies is the tribimaximal (TBM) neutrino mixing matrix that predicts the mixing angle θ_(13) = 0 and J_(CP) = 0. In order to accommodate the nonzero θ_(13) and CP violation, we modified the TBM by introducing a simple perturbation matrix into the TBM matrix that can produce θ_(13) = 7:89°, which is in agreement with the present experimental results, and the Dirac phase δ ≈ π/2, and JCP ≈ 0:0222. The obtained neutrino mass matrix from the modified TBM with both nonzero θ_(13) and δ is the complex neutrino mass matrix. If we impose μ-τ symmetry, as a constraint into the neutrino mass matrix, one finds that the J_(CP) = 0, which implies that CP violation cannot be accommodated in the μ-τ symmetry scheme. We break the μ-τ symmetry softly by introducing a small parameter x to perturb the neutrino mass matrix with the constraint that the trace of the perturbed neutrino mass matrix remains constant.

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Available abstract

Recently, evidence for a nonzero and relatively large θ_(13), as shown from the latest experimental results, has a serious implication on the well-known neutrino mixing matrix and the existence of CP violation in the neutrino sector (J_(CP)≠0). One of the well-known mixing matricies is the tribimaximal (TBM) neutrino mixing matrix that predicts the mixing angle θ_(13) = 0 and J_(CP) = 0. In order to accommodate the nonzero θ_(13) and CP violation, we modified the TBM by introducing a simple perturbation matrix into the TBM matrix that can produce θ_(13) = 7:89°, which is in agreement with the present experimental results, and the Dirac phase δ ≈ π/2, and JCP ≈ 0:0222. The obtained neutrino mass matrix from the modified TBM with both nonzero θ_(13) and δ is the complex neutrino mass matrix. If we impose μ-τ symmetry, as a constraint into the neutrino mass matrix, one finds that the J_(CP) = 0, which implies that CP violation cannot be accommodated in the μ-τ symmetry scheme. We break the μ-τ symmetry softly by introducing a small parameter x to perturb the neutrino mass matrix with the constraint that the trace of the perturbed neutrino mass matrix remains constant.

Key concepts: Pontecorvo–Maki–Nakagawa–Sakata matrix, Neutrino, Mass matrix, Physics, CP violation, Particle physics, Mixing (physics), Matrix (chemical analysis)

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