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Dive into the research topics where Emilio Torrente-Lujan is active.

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Featured researches published by Emilio Torrente-Lujan.


Physical Review D | 2004

Neutrino mass parameters from Kamland, SNO, and other solar evidence

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

The general gaugings of maximal d = 9 supergravity

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

KamLAND, solar antineutrinos, and the solar magnetic field

Bhag C. Chauhan; Joao Pulido; Emilio Torrente-Lujan

The overall effect of the measured observed ratio


Journal of High Energy Physics | 2003

KamLAND bounds on solar antineutrinos and neutrino transition magnetic moments

Emilio Torrente-Lujan

R\ensuremath{\sim}0.6


Journal of High Energy Physics | 2003

KamLAND, solar antineutrinos and their magnetic moment

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

Predictions from non trivial Quark-Lepton complementarity

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

Maximal Nine Dimensional Supergravity, General gaugings and the Embedding Tensor

J.J. Fernandez-Melgarejo; Tomas Ortin; Emilio Torrente-Lujan

A second solution (LMAII) appears for values


Physics of Atomic Nuclei | 2004

KamLAND and solar antineutrino spectrum

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

Toward minimal renormalizable SUSY SU(5) Grand Unified Model with tribimaximal mixing from A(4) Flavor symmetry

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

Hamevol1.0: a C++ code for differential equations based on Runge-Kutta algorithm. An application to matter enhanced neutrino oscillation

P. Aliani; V. Antonelli; M. Picariello; Emilio Torrente-Lujan

{\ensuremath{\chi}}^{2}

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Bhag C. Chauhan

Instituto Superior Técnico

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Joao Pulido

Instituto Superior Técnico

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Tomas Ortin

Spanish National Research Council

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Alfredo Urbano

International School for Advanced Studies

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M. Picariello

Istituto Nazionale di Fisica Nucleare

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