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首页> 外文期刊>Nuclear physics, B >Measurement of neutrino mixing angle θ 13 and mass difference Δ m ee 2 from reactor antineutrino disappearance in the RENO experiment
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Measurement of neutrino mixing angle θ 13 and mass difference Δ m ee 2 from reactor antineutrino disappearance in the RENO experiment

机译:中微子混合角θ 13 和质量差 Δ m ee 2 实验

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RENO (Reactor Experiment for Neutrino Oscillation) made a definitive measurement of the smallest neutrino mixing angle θ 13 in 2012, based on the disappearance of reactor electron antineutrinos. The experiment has obtained a more precise value of the mixing angle and the first result on neutrino mass difference Δ m ee 2 from an energy and baseline dependent reactor neutrino disappearance using ~500 days of data. Based on the ratio of inverse-beta-decay (IBD) prompt spectra measured in two identical far and near detectors, we obtain sin 2 ? ( 2 θ 13 ) = 0.082 ± 0.009 ( stat . ) ± 0.006 ( syst . ) and | Δ m ee 2 | = [ 2.62 ? 0.23 + 0.21 ( stat . ) ? 0.13 + 0.12 ( syst . ) ] × 10 ? 3 ?eV 2 . An excess of reactor antineutrinos near 5 MeV is observed in the measured prompt spectrum with respect to the most commonly used models. The excess is found to be consistent with coming from reactors. A successful measurement of θ 13 is also made in an IBD event sample with a delayed signal of neutron capture on hydrogen. A precise value of θ 13 would provide important information on determination of the leptonic CP phase if combined with a result of an accelerator neutrino beam experiment.
机译:基于反应堆电子中微子的消失,RENO(中微子振荡反应器实验)在2012年对最小中微子混合角θ13进行了确定的测量。实验使用约500天的数据,从能量和基线相关的反应堆中微子消失,获得了更精确的混合角值和中微子质量差Δm ee 2的第一个结果。根据在两个相同的远近探测器中测得的逆β衰变(IBD)即时光谱的比率,我们得到sin 2? (2θ13)= 0.082±0.009(stat。)±0.006(syst。)和| Δm ee 2 | = [2.62吗? 0.23 + 0.21(统计)? 0.13 + 0.12(系统)]×10? 3?eV 2。相对于最常用的模型,在测得的即时光谱中观察到了接近5 MeV的反应堆抗中微子过量。发现过量与来自反应堆的一致。在IBD事件样本中也成功完成了θ13的测量,并带有中子在氢气中捕获的延迟信号。如果结合加速器中微子束实验的结果,θ13的精确值将为确定轻子CP相提供重要信息。

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