A B Balantekin and H Yüksel 2003 J. Phys. G: Nucl. Part. Phys. 29 665 doi:10.1088/0954-3899/29/4/305
A B Balantekin and H Yüksel
Show affiliationsA global analysis of the data from all the solar neutrino experiments combined with the recent KamLAND data is presented. A formula frequently used in the literature gives survival probability for three active solar neutrino flavours in terms of a suitably modified two-flavour survival probability. Corrections to this formula, which depend on θ13 and δm231, are calculated. For the mass scale suggested by the atmospheric neutrino experiments the contributions of δm231 to these corrections are found to be negligible. The role of θ13 in solar neutrino physics is elaborated. For electron neutrino oscillations into another active flavour, we find best fit values of tan2 θ12 ~ 0.46, tan2 θ13 ~ 0 and δm221 ~ 7.1 × 10−5 eV2. It is found that the combined solar neutrino and KamLAND data provide the limit cos4 θ13 > 0.8 at the 90% confidence level.
95.30.Cq Elementary particle processes
14.60.Pq Neutrino mass and mixing
96.60.Vg Particle emission, solar wind
97.10.Cv Stellar structure, interiors, evolution, nucleosynthesis, ages
Issue 4 (April 2003)
Received 17 January 2003
Published 6 March 2003
A B Balantekin and H Yüksel 2003 J. Phys. G: Nucl. Part. Phys. 29 665
Y Liu et al 2005 Smart Mater. Struct. 14 1163
S Denis et al 2007 Supercond. Sci. Technol. 20 192
P J Brown et al 2004 J. Phys.: Condens. Matter 16 65
Jeong Sam Han et al 2005 J. Micromech. Microeng. 15 822
H N V Temperley and D H Trevena 1987 J. Phys. D: Appl. Phys. 20 1080
A N Verma et al 1984 J. Phys. D: Appl. Phys. 17 863
F Y Wu and K Y Lin 1980 J. Phys. A: Math. Gen. 13 629
Ramon van Handel and Hideo Mabuchi 2005 J. Opt. B: Quantum Semiclass. Opt. 7 S226
H E Lomelí and J D Meiss 2003 Nonlinearity 16 1573