Measurement of Neutrino and Antineutrino Oscillations Using Beam and Atmospheric Data in MINOS

Adamson, P.; Anghel, I. M.; Backhouse, C.; Barr, G.; Bishai, M.; Blake, A.; Bock, G. J.; Bogert, D.; Cao, S.; Castromonte, C.; Childress, S.; Coelho, J. A. B.; Corwin, L. A.; Cronin-Hennessy, D.; Jong, J. K. De; Devan, A. V.; Devenish, N. E.; Diwan, M.; Escobar, C. O.; Evans, Justin J.; Falk, E.; Feldman, G. J.; Frohne, M. V.; Gallagher, H.; Gomes, R. A.; Goodman, M. C.; Gouffon, P.; Graf, N.; Gran, R.; Grzelak, K.; Habig, A.; Hahn, S.; Hartnell, J.; Hatcher, R.; Himmel, A.; Holin, A.; Hylen, J.; Irwin, G. M.; Isvan, Z.; James, C.; Jensen, D.; Kafka, T.; Kasahara, S. M S; Koizumi, G.; Kordosky, M.; Kreymer, A.; Lang, K.; Ling, Jiajie; Litchfield, P. J.; Lucas, P.; Mann, W. A.; Маршак, М. Л.; Mathis, M.; Mayer, N.; McGowan, A. M.; Medeiros, M. M.; Mehdiyev, R.; Meier, J. R.; Messier, M. D.; Michael, D. G.; Miller, William H.; Mishra, S. R.; Sher, Shlomi; Moore, C. D.; Mualem, L.; Musser, J.; Naples, D.; Nelson, J. K.; Newman, H. B.; Nichol, R. J.; Nowak, J.; O’Connor, J. Michael; Oliver, W. P.; Orchanian, M.; Pahlka, R. B.; Paley, J.; Patterson, R. B.; Pawloski, G.; Phan-Budd, S.; Plunkett, R.; Qiu, X.; Radovic, A.; Rebel, B.; Rosenfeld, C.; Rubin, H. A.; Sanchez, M. C.; Schneps, J.; Schreckenberger, A.; Schreiner, P.; Sharma, R.; Sousa, A.; Tagg, N.; Talaga, R. L.; Thomas, J. C.; Thomson, M. A.; Tinti, G.; Tognini, S. C.; Toner, R.; Torretta, D.; Tzanakos, G.; Urheim, J.; Vahle, P.; Viren, B.; Weber, A.; Webb, R.; White, C.; Whitehead, L.; Wojcicki, S. G.; Zwaska, R.

doi:10.1103/physrevlett.110.251801

Cited by 245 publications

(239 citation statements)

References 18 publications

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“…However, such models try to generate tri-bimaximal neutrino mixing, which has been ruled out by the measurement of the reactor angle θ 13 [11][12][13][14] and also global fits of neutrino oscillation data [35]. One of us has constructed a warped extra dimension model with S 4 flavor symmetry where democratic mixing is produced at leading order and non-zero θ 13 can arise from subleading corrections [36]. In this work, we shall re-consider the issue of predicting flavor properties in particle physics by combining the conventional predictive power inherent in the use of non-Abelian flavor symmetries with the presence of warped extra dimensions.…”

Section: Jhep01(2016)007mentioning

confidence: 99%

“…The resulting non-Abelian flavor symmetries are typically broken spontaneously down to two different residual subgroups in the neutrino and the charged lepton sectors, leading to zero reactor mixing parameter, θ 13 = 0 . However, the measurement of a non-zero value for the reactor angle [11][12][13][14] implies the need to revamp the original flavor symmetry-based approaches in order to generate θ 13 = 0 [15] or else look for alternative possibilities, such as bi-large neutrino mixing [16][17][18].…”

Section: Introductionmentioning

confidence: 99%

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Warped flavor symmetry predictions for neutrino physics

Chen

Ding

Rojas

et al. 2016

J. High Energ. Phys.

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A realistic five-dimensional warped scenario with all standard model fields propagating in the bulk is proposed. Mass hierarchies would in principle be accounted for by judicious choices of the bulk mass parameters, while fermion mixing angles are restricted by a ∆(27) flavor symmetry broken on the branes by flavon fields.The latter gives stringent predictions for the neutrino mixing parameters, and the Dirac CP violation phase, all described in terms of only two independent parameters at leading order. The scheme also gives an adequate CKM fit and should be testable within upcoming oscillation experiments.

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Section: Jhep01(2016)007mentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

Warped flavor symmetry predictions for neutrino physics

Chen

Ding

Rojas

et al. 2016

J. High Energ. Phys.

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“…The T2K experiment has confirmed the neutrino oscillation in the ν µ → ν e appearance events [1], which provide us the new information of the CP violation of the lepton sector by combining the data of reactor experiments [2][3][4][5]. Therefore, the detailed study of the neutrino mixing including the CP violating phase gives us clues to reach the flavor theory [6]- [28].…”

Section: Introductionmentioning

confidence: 99%

Linking leptonic CP violation to quark unitarity triangle

Tanimoto

Yamamoto

2015

J. High Energ. Phys.

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Abstract:We study the linking between the CP violating phase of the lepton sectors and the unitarity triangle of the B 0 meson system. Antusch, King, Malinsky and Spinrath have shown that the quark mass matrices with the negligible 1-3 mixing give an interesting relation between the phase of the quark mixing matrices and CP violating measure φ 2 (α). This approach is extended by considering the SO(10) GUT including the Pati-Salam symmetry, which links the Yukawa matrices of the quark sector to the one of the lepton sector. We discuss the relation of the CP violating phases between both quark and lepton sectors as well as the mixing angles. Then, the leptonic CP violating phase is predicted in terms of the angle of the unitarity triangle of the B 0 meson system. The leptonic CP violating phase δ PMNS is predicted in the region −74 • ∼ −89 • , which is the consistent with the recent T2K results. Our predicted phase is sensitive to φ 2 (α) and φ 3 (γ). These predictions will be clearly tested in the future neutrino experiments as well as the Belle-II experiment.

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“…Antineutrino oscillation parameters are mostly constrained by reactor neutrino experiments [33][34][35][36], the SuperKamiokande atmospheric neutrino data [37], and accelerator data from the Main Injector Neutrino Oscillation Search (MINOS) [38] and the Tokai to Kamioka Experiment (T2K) [39]. These imply the existence of two hierarchical masssquared differences ∆m 2 21 and ∆m 2 31 and three nonzero mixing angles θ 13 , θ 12 , θ 23 .…”

Section: Antineutrino Oscillation Parametersmentioning

confidence: 99%

Neutrino versus antineutrino oscillation parameters at DUNE and Hyper-Kamiokande experiments

Gouvêa

Kelly

2017

Phys. Rev. D

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Testing, in a non-trivial, model-independent way, the hypothesis that the three-massive-neutrinos paradigm properly describes nature is among the main goals of the current and the next generation of neutrino oscillation experiments. In the coming decade, the DUNE and Hyper-Kamiokande experiments will be able to study the oscillation of both neutrinos and antineutrinos with unprecedented precision. We explore the ability of these experiments, and combinations of them, to determine whether the parameters that govern these oscillations are the same for neutrinos and antineutrinos, as prescribed by the CPT-theorem. We find that both DUNE and Hyper-Kamiokande will be sensitive to unexplored levels of leptonic CPT-violation. Assuming the parameters for neutrino and antineutrino oscillations are unrelated, we discuss the ability of these experiments to determine the neutrino and antineutrino mass-hierarchies, atmospheric-mixing octants, and CP-odd phases, three key milestones of the experimental neutrino physics program. Additionally, if the CPT-theorem is violated in nature in a way that is consistent with all present neutrino and antineutrino oscillation data, we find that DUNE and Hyper-Kamiokande have the potential to ultimately establish leptonic CPT-invariance violation.

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Measurement of Neutrino and Antineutrino Oscillations Using Beam and Atmospheric Data in MINOS

Cited by 245 publications

References 18 publications

Warped flavor symmetry predictions for neutrino physics

Warped flavor symmetry predictions for neutrino physics

Linking leptonic CP violation to quark unitarity triangle

Neutrino versus antineutrino oscillation parameters at DUNE and Hyper-Kamiokande experiments

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