Adamson, P.Anghel, I.Backhouse, C.Barr, G.Bishai, M.Blake, A.Bock, G. J.Bogert, D.Cao, S. V.Castromonte, C. M.Childress, S.Coelho, J. A. B.Corwin, L.Cronin-Hennessy, D.de Jong, J. K.Devan, A. V.Devenish, N. E.Diwan, M. V.Escobar, C. O.Evans, J. J.Falk, E.Feldman, GaryFrohne, M. V.Gallagher, H. R.Gomes, R. A.Goodman, M. C.Gouffon, P.Graf, N.Gran, R.Grzelak, K.Habig, A.Hahn, S. R.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, J.Litchfield, P. J.Lucas, P.Mann, W. A.Marshak, M. L.Mathis, M.Mayer, N.McGowan, A. M.Medeiros, M. M.Mehdiyev, R.Meier, J. R.Messier, M. D.Michael, D. G.Miller, W. H.Mishra, S. R.Moed Sher, S.Moore, C. D.Mualem, L.Musser, J.Naples, D.Nelson, J. K.Newman, H. B.Nichol, R. J.Nowak, J. A.O’Connor, J.Oliver, W. P.Orchanian, M.Pahlka, R. B.Paley, J.Patterson, R. B.Pawloski, G.Phan-Budd, S.Plunkett, R. K.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.Thomson, M. A.Tinti, G.Tognini, S. C.Toner, RuthTorretta, D.Tzanakos, G.Urheim, J.Vahle, P.Viren, B.Weber, A.Webb, R. C.White, C.Whitehead, L.Whitehead, L. H.Wojcicki, S. G.Zwaska, R.2016-09-132013Adamson, P., I. Anghel, C. Backhouse, G. Barr, M. Bishai, A. Blake, G. J. Bock, et al. 2013. “Measurement of Neutrino and Antineutrino Oscillations Using Beam and Atmospheric Data in MINOS.” Physical Review Letters 110 (25) (June). doi:10.1103/physrevlett.110.251801.0031-9007http://nrs.harvard.edu/urn-3:HUL.InstRepos:28455195We report measurements of oscillation parameters from νμ and ν⎯⎯μ disappearance using beam and atmospheric data from MINOS. The data comprise exposures of 10.71×1020 protons on target in the νμ-dominated beam, 3.36×1020 protons on target in the ν⎯⎯μ-enhanced beam, and 37.88 kton yr of atmospheric neutrinos. Assuming identical ν and ν⎯⎯ oscillation parameters, we measure |Δm2|=(2.41+0.09−0.10)×10−3  eV2 and sin2(2θ)=0.950+0.035−0.036. Allowing independent ν and ν⎯⎯ oscillations, we measure antineutrino parameters of |Δm⎯⎯⎯2|=(2.50+0.23−0.25)×10−3  eV2 and sin2(2θ⎯⎯)=0.97+0.03−0.08, with minimal change to the neutrino parameters.en-USneutrino: oscillationantineutrino: oscillationneutrino/mu: secondary beamantineutrino/mu: secondary beamneutrino: atmosphereneutrino: mass differenceneutrino: mixing angleMINOSexperimental resultsJournal Article2016-09-1310.1103/PhysRevLett.110.251801