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  • Abe, K; Alt, C; Barrow, D; Batkiewicz-Kwasniak, M; Beloshapkin, A; Bolognesi, S; Bonus, T; Bourguille, B; Boyd, S B; D Bravo Berguño; Bron, S; Bubak, A; M Buizza Avanzini; Cervera, A; Christodoulou, G; Dabrowska, A; Dealtry, T; Dunne, P; Feusels, T; Finch, A J; Fiorentini, G A; Fukuda, D; Fukuda, Y; Fusshoeller, K; Guigue, M; Holeczek, J; N T Hong Van; Iacob, F; Ishitsuka, M; Izmaylov, A; Jakkapu, M; Jiang, M; Johnson, S; Kakuno, H; Kameda, J; Karlen, D; Kasetti, S P; Kataoka, Y; Kim, H; Knox, A; Kobata, T; Koch, L; Kuribayashi, S; Kutter, T; Licciardi, M; Lindner, T; Liu, S L; X Lu; Malek, M; Manly, S; Marino, A D; Marti-Magro, L; Martin, J F; Maruyama, T; Matveev, V; Mazzucato, E; Metelko, C; Mezzetto, M; Miura, M; L Molina Bueno; Nakamura, A; Nakamura, K; Naseby, C E R; Ngoc, T V; Nishikawa, K; Noah, E; O'Sullivan, L; Odagawa, T; Pasternak, J; Pickering, L; Pidcott, C; Radermacher, T; Radicioni, E; Riccio, C; Schwehr, J; Sgalaberna, D; Shiozawa, M; Sobczyk, J T; Sobel, H; Steinmann, J; Suvorov, S; Suzuki, Y; Sztuc, A A; Tada, M; Tanaka, H A; Toki, W; Touramanis, C; Towstego, T; Vallari, Z; Walker, J; Wendell, R; Wilking, M J; Wret, C; Xia, J; Yamamoto, K; Yasutome, K; Yokoyama, M; Zarnecki, G; Zimmerman, E D; Zsoldos, S

    arXiv.org, 10/2020
    Paper, Journal Article

    The electron (anti-)neutrino component of the T2K neutrino beam constitutes the largest background in the measurement of electron (anti-)neutrino appearance at the far detector. The electron neutrino scattering is measured directly with the T2K off-axis near detector, ND280. The selection of the electron (anti-)neutrino events in the plastic scintillator target from both neutrino and anti-neutrino mode beams is discussed in this paper. The flux integrated single differential charged-current inclusive electron (anti-)neutrino cross-sections, \(d\sigma/dp\) and \(d\sigma/d\cos(\theta)\), and the total cross-sections in a limited phase-space in momentum and scattering angle (\(p > 300\) MeV/c and \(\theta \leq 45^{\circ}\)) are measured using a binned maximum likelihood fit and compared to the neutrino Monte Carlo generator predictions, resulting in good agreement.