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A Search for Muon-neutrino to Electron-neutrino and Muon-antineutrino to Electron-antineutrino Oscillations at NuTeV

S. Avvakumov, T. Adams, A. Alton, L. deBarbaro, P. deBarbaro, R. H. Bernstein, A. Bodek, T. Bolton, J. Brau, D. Buchholz, H. Budd, L. Bugel, J. Conrad, R. B. Drucker, B. T. Fleming, R. Frey, J. A. Formaggio, J. Goldman, M. Goncharov, D. A. Harris, R. A. Johnson, J. H. Kim, S. Koutsoliotas, M. J. Lamm, W. Marsh, D. Mason, J. McDonald, K. S. McFarland, C. McNulty, D. Naples, P. Nienaber, V. Radescu, A. Romosan, W. K. Sakumoto, H. Schellman, M. H. Shaevitz, P. Spentzouris, E. G. Stern, N. Suwonjandee, M. Tzanov, M. Vakili, A. Vaitaitis, U. K. Yang, J. Yu, G. P. Zeller, E. D. Zimmerman

hep-exarXiv:hep-ex/0203018

Abstract

Limits on νμ νe and νμ νe oscillations are extracted using the NuTeV detector with sign-selected νμ and μ beams. In μ mode, for the case of 2 2α= 1, Δm2 > 2.6 eV2 is excluded, and for Δm2 1000 eV2, 2 2α> 1.1 × 10-3. The NuTeV data exclude the high Δm2 end of νμ νe oscillations parameters favored by the LSND experiment without the need to assume that the oscillation parameters for ν and are the same. We present the most stringent experimental limits for νμ(νμ) νe (νe) oscillations in the large Δm2 region.

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