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Particle Physics Booklet - Particle Data Group - Lawrence Berkeley ...

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198 13. Neutrino mixing<br />

Figure 13.10: The regions of squared-mass splitting and mixing<br />

angle favored or excluded by various experiments. The figure was<br />

contributed by H. Murayama (University of California, <strong>Berkeley</strong>, and<br />

IPMU, University of Tokyo).<br />

averaging over the region of neutrino production in the Sun. The νe<br />

undergo transitions into (νμ + ντ )/ √ 2. As a consequence of the effects<br />

of the solar matter, the solar νe transitions observed by the Super-<br />

Kamiokande and SNO experiments exhibit a characteristic dependence<br />

on sin 2 θ12: P 3ν<br />

⊙ (νe → νe) ∼ = |Ue3| 4 +(1−|Ue3| 2 ) 2 sin 2 θ12. The data<br />

show that P 3ν<br />

⊙ ∼ = 0.3, which is a strong evidence for solar matter<br />

effects in the transitions [85] since in the case of transitions in vacuum<br />

P 3ν<br />

⊙ ∼ = |Ue3| 4 +(1−|Ue3| 2 ) 2 (1 − 0.5sin 2 2θ12) � 0.48,whereweusedthe<br />

experimental limits |Ue3| 2 < 0.056 and sin 2 2θ12 � 0.93.<br />

IV. The evidence for flavour neutrino oscillations. The evidence<br />

for flavour neutrino oscillations/transitions is compelling. We discuss the<br />

relevant data in the full edition. The regions of the oscillation parameter<br />

space favored or excluded by various neutrino oscillation experiments are<br />

shown in Fig. 13.10.

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