Proceedings of the XIth International Conference on Heavy Quarks and Leptons — PoS(HQL 2012) 2012
DOI: 10.22323/1.166.0051
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Observation of electron-antineutrino disappearance at Daya Bay.

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Cited by 6 publications
(6 citation statements)
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“…We can broadly categorize the reactor experiments into (i) short baseline (~1 km) and (ii) long baseline (~100-1000 km) reactor experiments. Three short baseline reactor neutrino experiments which looked for antineutrino disappearance with the main objective to measure last unknown neutrino oscillation angle θ 13 are Double Chooz in France [114], RENO in South Korea [115], and Daya Bay in China [116]. All three experiments used detectors which included liquid scintillator target loaded with 0.1% of Gadolinium.…”
Section: Reactor Neutrino Experimentmentioning
confidence: 99%
“…We can broadly categorize the reactor experiments into (i) short baseline (~1 km) and (ii) long baseline (~100-1000 km) reactor experiments. Three short baseline reactor neutrino experiments which looked for antineutrino disappearance with the main objective to measure last unknown neutrino oscillation angle θ 13 are Double Chooz in France [114], RENO in South Korea [115], and Daya Bay in China [116]. All three experiments used detectors which included liquid scintillator target loaded with 0.1% of Gadolinium.…”
Section: Reactor Neutrino Experimentmentioning
confidence: 99%
“…The discovery of neutrino flavor oscillation is a tremendous achievement in particle physics during the last two decades [1][2][3], which manifests that neutrinos have masses, and the leptonic mixing matrix is nontrivial. However, the origin of the flavor mixing is elusive for theorists.…”
Section: Introductionmentioning
confidence: 99%
“…These patterns, especially the TBM, derived from flavor groups such as A 4 [15,16] and S 4 [16,17], are compatible with previous published data of atmospheric neutrino and solar neutrino. The discovery of a relatively large reactor mixing angle θ 13 [3,[18][19][20][21] and the remarkable progress of measurements of neutrino oscillation parameters, however, strictly constrain or exclude the above patterns. Hence, diverse methods to generate a nonzero reactor mixing angle θ 13 have been proposed.…”
Section: Introductionmentioning
confidence: 99%
“…Neutrino oscillations have been very well established by measuring the neutrino-mixing parameters θ 12 , θ 23 , θ 13 , Δ m 2 21 , and Δm 2 31 [1]. One of the promising candidates for explaining the observed Pontecorvo-Maki-Nakagawa-Sakata (PMNS) mixing matrix is the tribimaximal (TBM) [2] which is ruled out due to the discovery of the nonzero value of θ 13 [3][4][5][6][7][8][9]. Hence, in order to accommodate θ 13 ≠ 0, the PMNS matrix is reproduced using the next-to-TBM (NTBM) [10,11] which predicts the correlations among the phase and mixing angles.…”
Section: Introductionmentioning
confidence: 99%