Rodriguez, A.Whitehead, L.Alcaraz-Aunion, J. L.Andringa, S.Aoki, S.Argyriades, J.Asakura, K.Ashie, R.Berghaus, F.Berns, H.Bhang, H.Blondel, A.Borghi, S.Bouchez, J.Burguet-Castell, J.Casper, D.Catala, J.Cavata, C.Cervera, A.Chen, S. M.Cho, K. O.Choi, J. H.Dore, U.Espinal, X.Fechner, M.Fernandez, E.Fujii, Y.Fukuda, Y.Gomez-Cadenas, J. J.Gran, R.Hara, T.Hasegawa, M.Hasegawa, T.Hayato, Y.Helmer, R. L.Hiraide, K.Hosaka, J.Ichikawa, A. K.Iinuma, M.Ikeda, A.Ishida, T.Ishihara, K.Ishii, T.Ishitsuka, M.Itow, Y.Iwashita, T.Jang, H. I.Jeon, E. J.Jeong, I. S.Joo, K. K.Jover, G.Jung, C. K.Kajita, T.Kameda, J.Kaneyuki, K.Kato, I.Kearns, E.Kim, C. O.Khabibullin, M.Khotjantsev, A.Kielczewska, D.Kim, J. Y.Kim, S. B.Kitching, P.Kobayashi, K.Kobayashi, T.Konaka, A.Koshio, Y.Kropp, W.Kudenko, Y.Kuno, Y.Kurimoto, Y.Kutter, T.Learned, J.Likhoded, S.Lim, I. T.Loverre, P. F.Ludovici, L.Maesaka, H.Mallet, J.Mariani, CamilloMatsuno, S.Matveev, V. A.McConnel, K.McGrew, C.Mikheyev, S.Minamino, A.Mine, S.Mineev, O.Mitsuda, C.Miura, M.Moriguchi, Y.Moriyama, S.Nakadaira, T.Nakahata, M.Nakamura, K.Nakano, I.Nakaya, T.Nakayama, S.Namba, T.Nambu, R.Nawang, S.Nishikawa, K.Nitta, K.Nova, F.Novella, P.Obayashi, Y.Okada, A.Okumura, K.Oser, S. M.Oyama, Y.Pac, M. Y.Pierre, F.Saji, C.Sakuda, M.Sanchez, F.Scholberg, K.Schroeter, R.Sekiguchi, M.Shiozawa, M.Shiraishi, K. K.Sitjes, G.Smy, M.Sobel, H.Sorel, M.Stone, J.Sulak, L.Suzuki, A.Suzuki, Y.Tada, M.Takahashi, T.Takenaga, Y.Takeuchi, Y.Taki, K.Takubo, Y.Tamura, N.Tanaka, M.Terri, R.T'Jampens, S.Tornero-Lopez, A.Totsuka, Y.Vagins, M. R.Walter, C. W.Wang, W.Wilkes, R. J.Yamada, S.Yamada, Y.Yamamoto, S.Yanagisawa, C.Yershov, N.Yokoyama, H.Yokoyama, M.Yoo, J.Yoshida, M.Zalipska, J.2018-01-102018-01-102008-08-011550-7998http://hdl.handle.net/10919/81652Single charged pion production in charged-current muon neutrino interactions with carbon is studied using data collected in the K2K long-baseline neutrino experiment. The mean energy of the incident muon neutrinos is 1.3 GeV. The data used in this analysis are mainly from a fully active scintillator detector, SciBar. The cross section for single &#960;⁺ production in the resonance region (W < 2 GeV/c²) relative to the charged-current quasi-elastic cross section is found to be 0.734 ^+0.140 _−0.153. The energy-dependent cross section ratio is also measured. The results are consistent with a previous experiment and the prediction of our model.? - ? (16) page(s)In CopyrightAstronomy & AstrophysicsPhysics, Particles & FieldsPhysicsCROSS-SECTION MEASUREMENTSK2K SCIBAR DETECTORANTINEUTRINO INTERACTIONSHIGH-ENERGIESCONSTRUCTIONDEUTERIUMHYDROGENPHYSICSPERFORMANCEGARGAMELLEArticle - Refereedhttps://doi.org/10.1103/PhysRevD.78.032003783Mariani, C [0000-0003-3284-4681]1550-2368