Tri-bimaximal Neutrino Mixing and Flavor-dependent Resonant Leptogenesis

Jul, 2006
18 pages
Published in:
  • Phys.Lett.B 653 (2007) 278-287
e-Print:

Citations per year

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Abstract:
We propose a particularly economical neutrino mass model, in which there are only two right-handed Majorana neutrinos of O(1){\cal O}(1) TeV and their masses are highly degenerate. Its novel Yukawa-coupling texture together with the seesaw mechanism allows us to achieve the normal neutrino mass hierarchy with m1=0m^{}_1 = 0 and a nearly tri-bimaximal neutrino mixing pattern with the maximal CP-violating phase: θ23=π/4\theta^{}_{23} = \pi/4, δ=π/2|\delta| = \pi/2 and sin2θ12=(12tan2θ13)/3\sin^2 \theta^{}_{12} = (1 - 2 \tan^2 \theta^{}_{13})/3. One may also obtain the inverted neutrino mass hierarchy with m3=0m^{}_3 = 0 and the corresponding neutrino mixing pattern with θ23=π/4\theta^{}_{23} =\pi/4 and θ13=δ=0\theta^{}_{13} = \delta = 0. In both cases, the cosmological baryon number asymmetry ηB6.1×1010\eta^{}_{\rm B} \approx 6.1 \times 10^{-10} can naturally be interpreted through the resonant leptogenesis mechanism. After taking into account the flavor effects, we find that the prediction for ηB\eta^{}_{\rm B} is enhanced by a factor 4\sim 4. An experimental test of this TeV-scale neutrino model might be possible at LHC and ILC in the future.
  • 11.30.Fs
  • 14.60.Pq
  • 14.60.St
  • neutrino: mass
  • neutrino: mixing angle
  • seesaw model: minimal
  • mass: hierarchy
  • matter: asymmetry
  • leptogenesis
  • baryon number: asymmetry
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