Relating large Ue3 to the ratio of neutrino mass-squared differences

[1]  P. Machado,et al.  Combining accelerator and reactor measurements of θ13: the first result , 2011, 1111.3330.

[2]  S. King,et al.  Trimaximal mixing with predicted theta_13 from a new type of constrained sequential dominance , 2011, 1108.4278.

[3]  N. Chamoun,et al.  One-zero textures of Majorana neutrino mass matrix and current experimental tests , 2011, 1108.4010.

[4]  M. Toups,et al.  Indication for the disappearance of reactor electron antineutrinos in the Double Chooz experiment , 2011, 1112.6353.

[5]  J. Valle,et al.  Where we are on θ13: addendum to ‘Global neutrino data and recent reactor fluxes: status of three-flavor oscillation parameters’ , 2011, 1108.1376.

[6]  J. C. Mitchell,et al.  Improved search for Muon-neutrino to electron-neutrino oscillations in MINOS. , 2011, Physical review letters.

[7]  E. Lisi,et al.  Evidence of $\theta_{13}$>0 from global neutrino data analysis , 2011, 1106.6028.

[8]  Tejpreet Singh Golan,et al.  Indication of electron neutrino appearance from an accelerator-produced off-axis muon neutrino beam. , 2011, Physical review letters.

[9]  W. Rodejohann.  NEUTRINO-LESS DOUBLE BETA DECAY AND PARTICLE PHYSICS , 2011, 1106.1334.

[10]  J. Valle,et al.  Global neutrino data and recent reactor fluxes: the status of three-flavour oscillation parameters , 2011, 1103.0734.

[11]  Tatsuo C. Kobayashi,et al.  Non-Abelian Discrete Symmetries in Particle Physics , 2010, 1003.3552.

[12]  G. Altarelli,et al.  Discrete Flavor Symmetries and Models of Neutrino Mixing , 2010, 1002.0211.

[13]  M. Gonzalez-Garcia,et al.  Updated global fit to three neutrino mixing: status of the hints of θ13 > 0 , 2010, 1001.4524.

[14]  S. Goswami,et al.  Hybrid textures in minimal seesaw mass matrices , 2008, 0811.4744.

[15]  S. Goswami,et al.  Minimal textures in seesaw mass matrices and their low and high energy phenomenology , 2009, 0905.2739.

[16]  S. Goswami,et al.  Minimal seesaw textures with two heavy neutrinos , 2008, 0807.3438.

[17]  Tatsuo C. Kobayashi,et al.  Flavor symmetry breaking and vacuum alignment on orbifolds , 2008, 0809.3064.

[18]  E. Lisi,et al.  Hints of theta13>0 from global neutrino data analysis. , 2008, Physical review letters.

[19]  M. Frigerio,et al.  Common origin of $\theta_{13}$ and Delta m**2{12} in a model of neutrino mass with quaternion symmetry , 2007, 0708.0166.

[20]  Z. Xing,et al.  Neutrino masses, lepton flavor mixing and leptogenesis in the minimal seesaw model , 2006, hep-ph/0612033.

[21]  M. Tanimoto,et al.  Flavor symmetry and vacuum aligned mass textures , 2006, hep-ph/0609220.

[22]  N. Haba,et al.  Twisted flavors and tribimaximal neutrino mixing. , 2006, Physical review letters.

[23]  A. Merle,et al.  Elements of the neutrino mass matrix : Allowed ranges and implications of texture zeros , 2006, hep-ph/0603111.

[24]  N. Haba,et al.  Discrete flavor symmetry, dynamical mass textures, and grand unification , 2005, hep-ph/0511108.

[25]  W. Rodejohann,et al.  Minimal mass matrices for Dirac neutrinos , 2005, hep-ph/0503143.

[26]  G. Branco,et al.  Removing ambiguities in the neutrino mass matrix , 2002, hep-ph/0212341.

[27]  S. Glashow,et al.  Cosmological sign of neutrino CP violation , 2002, hep-ph/0208157.

[28]  M. N. Rebelo,et al.  Linking solar and long baseline terrestrial neutrino experiments. , 1999, Physical review letters.

[29]  M. Grassi,et al.  Limits on neutrino oscillations from the CHOOZ experiment , 1999, hep-ex/9907037.

[30]  R. Gatto,et al.  Weak Selfmasses, Cabibbo Angle, and Broken SU(2) x SU(2) , 1968 .