Abstract

We present the results of a Bayesian analysis of solar and KamLAND neutrino data in the framework of three-neutrino mixing. We adopt two approaches for the prior probability distribution of the oscillation parameters $\ensuremath{\Delta}{m}_{21}^{2}$, ${sin}^{2}{\ensuremath{\vartheta}}_{12}$, ${sin}^{2}{\ensuremath{\vartheta}}_{13}$: (1) a traditional flat uninformative prior; and (2) an informative prior which describes the limits on ${sin}^{2}{\ensuremath{\vartheta}}_{13}$ obtained in atmospheric and long-baseline accelerator and reactor neutrino experiments. In both approaches, we present the allowed regions in the ${sin}^{2}{\ensuremath{\vartheta}}_{13}\mathrm{\text{\ensuremath{-}}}\ensuremath{\Delta}{m}_{21}^{2}$ and ${sin}^{2}{\ensuremath{\vartheta}}_{12}\mathrm{\text{\ensuremath{-}}}{sin}^{2}{\ensuremath{\vartheta}}_{13}$ planes, as well as the marginal posterior probability distribution of ${sin}^{2}{\ensuremath{\vartheta}}_{13}$. We confirm the $1.2\ensuremath{\sigma}$ hint of ${\ensuremath{\vartheta}}_{13}>0$ found in [G. Fogli et al., Phys. Rev. Lett. 101, 141801 (2008).] from the analysis of solar and KamLAND neutrino data. We found that the statistical significance of the hint is reduced to about $0.8\ensuremath{\sigma}$ by the constraints on ${sin}^{2}{\ensuremath{\vartheta}}_{13}$ coming from atmospheric and long-baseline accelerator and reactor neutrino data, in agreement with [T. Schwetz, M. Tortola, and J. W. F. Valle, New J. Phys. 10, 113011 (2008).].

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