Adamson, P.Andreopoulos, C.Auty, D. J.Ayres, D. S.Backhouse, C.Barr, G.Bernstein, R. H.Betancourt, M.Bhattarai, P.Bishai, M.Blake, A.Bock, G. J.Boehm, J.Boehnlein, D. J.Bogert, D.Bower, C.Budd, S.Cavanaugh, S.Cherdack, D.Childress, S.Choudhary, B. C.Cobb, J. H.Coelho, J. A. B.Coleman, S. J.Corwin, L.Cronin-Hennessy, D.Danko, I. Z.de Jong, J. K.Devenish, N. E.Diwan, M. V.Dorman, M.Escobar, C. O.Evans, J. J.Falk, E.Feldman, GaryFrohne, M. V.Gallagher, H. R.Godley, A.Goodman, M. C.Gouffon, P.Graf, N.Gran, R.Grashorn, E. W.Grzelak, K.Habig, A.Harris, D.Harris, P. G.Hartnell, J.Hatcher, R.Heller, K.Himmel, A.Holin, A.Huang, X.Hylen, J.Ilic, J.Irwin, G. M.Isvan, Z.Jaffe, D. E.James, C.Jensen, D.Kafka, T.Kasahara, S. M. S.Koizumi, G.Kopp, S.Kordosky, M.Krahn, Z.Kreymer, A.Lang, K.Lefeuvre, G.Ling, J.Litchfield, P. J.Litchfield, R. P.Loiacono, L.Lucas, P.Ma, J.Mann, W. A.Marshak, M. L.Marshall, J. S.Mayer, N.McGowan, A. M.Mehdiyev, R.Meier, J. R.Messier, M. D.Michael, D. G.Miller, W. H.Mishra, S. R.Mitchell, J.Moore, C. D.Morfín, J.Mualem, L.Mufson, S.Musser, J.Naples, D.Nelson, J. K.Newman, H. B.Nichol, R. J.Ochoa-Ricoux, J. P.Oliver, W. P.Orchanian, M.Ospanov, R.Paley, J.Para, A.Patterson, R. B.Pawloski, G.Pearce, G. F.Petyt, D. A.Pittam, R.Plunkett, R. K.Rameika, R. A.Raufer, T. M.Rebel, B.Rodrigues, P. A.Rosenfeld, C.Rubin, H. A.Ryabov, V. A.Sanchez, M. C.Schneps, J.Schreiner, P.Shanahan, P.Smart, W.Smith, C.Sousa, A.Strait, M.Swain, S.Tagg, N.Talaga, R. L.Thomas, J.Thomson, M. A.Tinti, G.Toner, RuthTzanakos, G.Urheim, J.Vahle, P.Viren, B.Weber, A.Webb, R. C.White, C.Whitehead, L.Wojcicki, S. G.Wright, D. M.Yang, T.Zhang, K.Zois, M.Zwaska, R.2016-09-132010Adamson, P., C. Andreopoulos, D. J. Auty, D. S. Ayres, C. Backhouse, G. Barr, R. H. Bernstein, et al. 2010. “New Constraints on Muon-Neutrino to Electron-Neutrino Transitions in MINOS.” Phys. Rev. D 82 (5) (September 21). doi:10.1103/physrevd.82.051102.1550-7998http://nrs.harvard.edu/urn-3:HUL.InstRepos:28447977This paper reports results from a search for νμ→νe transitions by the MINOS experiment based on a 7×1020 protons-on-target exposure. Our observation of 54 candidate νe events in the far detector with a background of 49.1±7.0(stat)±2.7(syst) events predicted by the measurements in the near detector requires 2sin2(2θ13)sin2θ23<0.12(0.20) at the 90% C.L. for the normal (inverted) mass hierarchy at δCP=0. The experiment sets the tightest limits to date on the value of θ13 for nearly all values of δCP for the normal neutrino mass hierarchy and maximal sin2(2θ23).en-USmass: hierarchyneutrino: mass differenceCP: violationMINOSexperimental resultsFermilabneutrino/mu: secondary beamneutrino: oscillationneutrino/e: particle identificationneutrino: mixing anglebackgroundJournal Article2016-09-1310.1103/PhysRevD.82.051102