Emilio Torrente-Lujan
University of Murcia
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Publication
Featured researches published by Emilio Torrente-Lujan.
Physical Review D | 2004
Paola Aliani; Vito Antonelli; Marco Picariello; Emilio Torrente-Lujan
An updated analysis of all available neutrino oscillation evidence in reactor (Kamland, first 145 days of data) and solar experiments (SK day and night spectra, global rates from Homestake, SAGE, and GALLEX) including the SNOCC and NC data is presented. In the framework of two active neutrino oscillations we determine the allowed regions in neutrino parameter space; we obtain, from the Kamland spectral shape and global signal, the following antineutrino best solution parameters:
Journal of High Energy Physics | 2011
J.J. Fernandez-Melgarejo; Tomas Ortin; Emilio Torrente-Lujan
\ensuremath{\Delta}{m}_{\mathrm{kl}}^{2}=7.7\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}5}{\mathrm{eV}}^{2},{\mathrm{tan}}^{2}{\ensuremath{\theta}}_{\mathrm{kl}}=0.98.
Physical Review D | 2003
Bhag C. Chauhan; Joao Pulido; Emilio Torrente-Lujan
The overall effect of the measured observed ratio
Journal of High Energy Physics | 2003
Emilio Torrente-Lujan
R\ensuremath{\sim}0.6
Journal of High Energy Physics | 2003
Paola Aliani; Vito Antonelli; Marco Picariello; Emilio Torrente-Lujan
is that the large mixing angle (LMA) region remains the only one that is still favored. Combining Kamland and solar data and assuming CPT invariance, i.e., the same mass matrix for neutrinos and antineutrinos, we obtain the following antineutrino best solution parameters (LMAI solution):
International Journal of Modern Physics A | 2007
Marco Picariello; Bhag C. Chauhan; Joao Pulido; Emilio Torrente-Lujan
\ensuremath{\Delta}{m}^{2}=7.1\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}5}{\mathrm{eV}}^{2},{\mathrm{tan}}^{2}\ensuremath{\theta}=0.47.
Protein Science | 2012
J.J. Fernandez-Melgarejo; Tomas Ortin; Emilio Torrente-Lujan
A second solution (LMAII) appears for values
Physics of Atomic Nuclei | 2004
Bhag C. Chauhan; Joao Pulido; Emilio Torrente-Lujan
\ensuremath{\Delta}{m}^{2}=1.5\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}4}{\mathrm{eV}}^{2},{\mathrm{tan}}^{2}\ensuremath{\theta}=0.48.
Physical Review D | 2010
Paolo Ciafaloni; Marco Picariello; Emilio Torrente-Lujan; Alfredo Urbano
We determine additionally individual neutrino mixing parameters and their errors from fits to marginal likelihood distributions; the values are compatible with previous results. In both methods,
arXiv: Computational Engineering, Finance, and Science | 2003
P. Aliani; V. Antonelli; M. Picariello; Emilio Torrente-Lujan
{\ensuremath{\chi}}^{2}