2021
DOI: 10.1103/physrevd.103.112008
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Improved constraints on neutrino mixing from the T2K experiment with3.13×1021protons on target

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Cited by 103 publications
(57 citation statements)
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References 92 publications
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“…The quark sector with three generations contains a CP violating complex phase called the Cabibbo-Kobayashi-Maskawa (CKM) phase. Recently, a nonzero phase has been hinted at in the lepton sector as well [28][29][30]. The existence of CP violation (CPV) in nature and the SUSY CP problem are reconciled by the idea of that CP is a gauge symmetry [31,32], which is broken spontaneously [33].…”
Section: Jhep09(2021)031mentioning
confidence: 99%
See 1 more Smart Citation
“…The quark sector with three generations contains a CP violating complex phase called the Cabibbo-Kobayashi-Maskawa (CKM) phase. Recently, a nonzero phase has been hinted at in the lepton sector as well [28][29][30]. The existence of CP violation (CPV) in nature and the SUSY CP problem are reconciled by the idea of that CP is a gauge symmetry [31,32], which is broken spontaneously [33].…”
Section: Jhep09(2021)031mentioning
confidence: 99%
“…There is some tension between measurements of this phase. The NOνA [29] experiment favors δ CP < π, still allowing a CP-conserving phase, while T2K [30] favors δ CP > π and disfavors CP-violation at the level of 2σ.…”
Section: The Sm Flavor Structurementioning
confidence: 99%
“…Marvelous data from several ongoing experiments such as Super-K [10], IceCube-DeepCore [11], ANTARES [12], Daya Bay [13], RENO [14], Tokai to Kamioka (T2K) [15,16], and NuMI Off-axis ν e Appearance (NOνA) [17] have been improving our knowledge about the neutrino oscillation parameters beyond expectations. Because of this fascinating progress, we have been able to build a robust, simple, three-flavor neutrino oscillation paradigm which successfully accommodate most of the data [3][4][5][6].…”
Section: Jhep11(2021)094mentioning
confidence: 99%
“…[24,25]. In 2021, T2K and NOνA updated their results with the best-fit value from T2K remaining the same, δ D = 252 •+40 • −33 • (NO) and 281 •+28 • −31 • (IO) [26] while the NOνA best fit changes to δ D = 148 •+49 • −157 • for NO [27]. The tension still remains with a difference of 104 • in the best fit values.…”
Section: Introductionmentioning
confidence: 98%