Measurements of ν̅μ and ν̅μ + νμ charged-current cross-sections without detected pions or protons on water and hydrocarbon at a mean anti-neutrino energy of 0.86 GeV. (2nd March 2021)

• Record Type: Journal Article
• Authors: Abe, K; Akhlaq, N; Akutsu, R; Ali, A; Alt, C; Andreopoulos, C; Anthony, L; Antonova, M; Aoki, S; Ariga, A; Arihara, T; Asada, Y; Ashida, Y; Atkin, E T; Awataguchi, Y; Ban, S; Barbi, M; Barker, G J; Barr, G; Barrow, D; Barry, C; Batkiewicz-Kwasniak, M; Beloshapkin, A; Bench, F; Berardi, V; Berkman, S; Berns, L; Bhadra, S; Bienstock, S; Blanchet, A; Blondel, A; Bolognesi, S; Bonus, T; Bourguille, B; Boyd, S B; Brailsford, D; Bravar, A; Bravo Berguño, D; Bronner, C; Bron, S; Bubak, A; Buizza Avanzini, M; Calcutt, J; Campbell, T; Cao, S; Cartwright, S L; Catanesi, M G; Cervera, A; Chappell, A; Checchia, C; Cherdack, D; Chikuma, N; Christodoulou, G; Cicerchia, M; Coleman, J; Collazuol, G; Cook, L; Coplowe, D; Cudd, A; Dabrowska, A; De Rosa, G; Dealtry, T; Denner, P F; Dennis, S R; Densham, C; Dergacheva, A; Di Lodovico, F; Dokania, N; Dolan, S; Doyle, T A; Drapier, O; Dumarchez, J; Dunne, P; Eguchi, A; Eklund, L; Emery-Schrenk, S; Ereditato, A; Fernandez, P; Feusels, T; Finch, A J; Fiorentini, G A; Fiorillo, G; Francois, C; Friend, M; Fujii, Y; Fujita, R; Fukuda, D; Fukuda, R; Fukuda, Y; Fusshoeller, K; Gameil, K; Giganti, C; Golan, T; Gonin, M; Gorin, A; Guigue, M; Hadley, D R; Haigh, J T; Hamacher-Baumann, P; Harris, D A; Hartz, M; Hasegawa, T; Hassani, S; Hastings, N C; Hayashino, T; Hayato, Y; Hiramoto, A; Hogan, M; Holeczek, J; Hong Van, N T; Honjo, T; Iacob, F; Ichikawa, A K; Ikeda, M; Ishida, T; Ishii, T; Ishitsuka, M; Iwamoto, K; Izmaylov, A; Izumi, N; Jakkapu, M; Jamieson, B; Jenkins, S J; Jesús-Valls, C; Jiang, M; Johnson, S; Jonsson, P; Jung, C K; Jurj, P B; Kabirnezhad, M; Kaboth, A C; Kajita, T; Kakuno, H; Kameda, J; Karlen, D; Kasetti, S P; Kataoka, Y; Katayama, Y; Katori, T; Kato, Y; Kearns, E; Khabibullin, M; Khotjantsev, A; Kikawa, T; Kikutani, H; Kim, H; Kim, J; King, S; Kisiel, J; Knight, A; Knox, A; Kobata, T; Kobayashi, T; Koch, L; Koga, T; Konaka, A; Kormos, L L; Koshio, Y; Kostin, A; Kowalik, K; Kubo, H; Kudenko, Y; Kukita, N; Kuribayashi, S; Kurjata, R; Kutter, T; Kuze, M; Labarga, L; Lagoda, J; Lamoureux, M; Last, D; Laveder, M; Lawe, M; Licciardi, M; Lindner, T; Litchfield, R P; Liu, S L; Li, X; Longhin, A; Ludovici, L; Lu, X; Lux, T; Machado, L N; Magaletti, L; Mahn, K; Malek, M; Manly, S; Maret, L; Marino, A D; Marti-Magro, L; Martin, J F; Maruyama, T; Matsubara, T; Matsushita, K; Matveev, V; Mauger, C; Mavrokoridis, K; Mazzucato, E; McCarthy, M; McCauley, N; McElwee, J; McFarland, K S; McGrew, C; Mefodiev, A; Metelko, C; Mezzetto, M; Minamino, A; Mineev, O; Mine, S; Miura, M; Molina Bueno, L; Moriyama, S; Morrison, J; Mueller, Th A; Munteanu, L; Murphy, S; Nagai, Y; Nakadaira, T; Nakahata, M; Nakajima, Y; Nakamura, A; Nakamura, K G; Nakamura, K; Nakano, Y; Nakayama, S; Nakaya, T; Nakayoshi, K; Nantais, C; Naseby, C E R; Ngoc, T V; Nguyen, V Q; Niewczas, K; Nishikawa, K; Nishimura, Y; Noah, E; Nonnenmacher, T S; Nova, F; Novella, P; Nowak, J; Nugent, J C; O'Keeffe, H M; O'Sullivan, L; Odagawa, T; Ogawa, T; Okada, R; Okumura, K; Okusawa, T; Oser, S M; Owen, R A; Oyama, Y; Palladino, V; Palomino, J L; Paolone, V; Pari, M; Parker, W C; Parsa, S; Pasternak, J; Paudyal, P; Pavin, M; Payne, D; Penn, G C; Pickering, L; Pidcott, C; Pintaudi, G; Pinzon Guerra, E S; Pistillo, C; Popov, B; Porwit, K; Posiadala-Zezula, M; Pritchard, A; Quilain, B; Radermacher, T; Radicioni, E; Radics, B; Ratoff, P N; Reinherz-Aronis, E; Riccio, C; Rondio, E; Roth, S; Rubbia, A; Ruggeri, A C; Ruggles, C; Rychter, A; Sakashita, K; Sánchez, F; Santucci, G; Schloesser, C M; Scholberg, K; Schwehr, J; Scott, M; Seiya, Y; Sekiguchi, T; Sekiya, H; Sgalaberna, D; Shah, R; Shaikhiev, A; Shaker, F; Shaykina, A; Shiozawa, M; Shorrock, W; Shvartsman, A; Skwarczynski, K; Smirnov, A; Smy, M; Sobczyk, J T; Sobel, H; Soler, F J P; Sonoda, Y; Spina, R; Steinmann, J; Suvorov, S; Suzuki, A; Suzuki, S Y; Suzuki, Y; Sztuc, A A; Tada, M; Tajima, M; Takeda, A; Takeuchi, Y; Tanaka, H K; Tanaka, H A; Tanaka, S; Tanihara, Y; Tani, M; Teshima, N; Thompson, L F; Toki, W; Touramanis, C; Towstego, T; Tsui, K M; Tsukamoto, T; Tzanov, M; Uchida, Y; Uno, W; Vagins, M; Valder, S; Vallari, Z; Vargas, D; Vasseur, G; Vilela, C; Vinning, W G S; Vladisavljevic, T; Volkov, V V; Wachala, T; Walker, J; Walsh, J G; Wang, Y; Wark, D; Wascko, M O; Weber, A; Wendell, R; Wilking, M J; Wilkinson, C; Wilson, J R; Wilson, R J; Wood, K; Wret, C; Xia, J; Yamada, Y; Yamamoto, K; Yanagisawa, C; Yang, G; Yano, T; Yasutome, K; Yen, S; Yershov, N; Yokoyama, M; Yoshida, T; Yoshimoto, Y; Yu, M; Zalewska, A; Zalipska, J; Zaremba, K; Zarnecki, G; Ziembicki, M; Zimmerman, E D; Zito, M; Zsoldos, S; Zykova, A;
• Is Part Of: Progress of theoretical and experimental physics. Volume 2021:Number 4(2021)
• Publication Date: 2021-03-02
• Subjects: C04 -- C32; Physics -- Periodicals; Mathematical physics -- Periodicals; 530.05
• DOI: 10.1093/ptep/ptab014
• Languages: English
• ISSNs: 2050-3911

Abstract

Abstract: We report measurements of the flux-integrated ν̅ μ and ν̅ μ + ν μ charged-current cross-sections on water and hydrocarbon targets using the T2K anti-neutrino beam with a mean beam energy of 0.86 GeV. The signal is defined as the (anti-)neutrino charged-current interaction with one induced $\mu^\pm$ and no detected charged pion or proton. These measurements are performed using a new WAGASCI module recently added to the T2K setup in combination with the INGRID Proton Module. The phase space of muons is restricted to the high-detection efficiency region, $p_{\mu}>400~{\rm MeV}/c$ and $\theta_{\mu}<30^{\circ}$, in the laboratory frame. An absence of pions and protons in the detectable phase spaces of $p_{\pi}>200~{\rm MeV}/c$, $\theta_{\pi}<70^{\circ}$ and $p_{\rm p}>600~{\rm MeV}/c$, $\theta_{\rm p}<70^{\circ}$ is required. In this paper, both the $\overline{\nu}_\mu$ cross-sections and $\overline{\nu}_\mu+\nu_\mu$ cross-sections on water and hydrocarbon targets and their ratios are provided by using the D'Agostini unfolding method. The results of the integrated $\overline{\nu}_\mu$ cross-section measurements over this phase space are $\sigma_{\rm H_{2}O}=(1.082\pm0.068(\rm stat.)^{+0.145}_{-0.128}(\rm syst.)) \times 10^{-39}\, {\rm cm^{2} / nucleon}$, $\sigma_{\rm CH}=(1.096\pm0.054(\rm stat.)^{+0.132}_{-0.117}(\rm syst.)) \times 10^{-39}\, {\rm cm^{2} / nucleon}$, and $\sigma_{\rm H_{2}O}/\sigma_{\rm CH} = 0.987\pm0.078(\rm stat.)^{+0.093}_{-0.090}(\rm syst.)$ . The $\overline{\nu}_\mu+\nu_\mu$ cross-section is $\sigma_{\rm H_{2}O} = (1.155\pm0.064(\rm stat.)^{+0.148}_{-0.129}(\rm syst.)) \times 10^{-39}\, {\rm cm^{2} / nucleon}$, $\sigma_{\rm CH}=(1.159\pm0.049(\rm stat.)^{+0.129}_{-0.115}(\rm syst.)) \times 10^{-39}\, {\rm cm^{2} / nucleon}$, and $\sigma_{\rm H_{2}O}/\sigma_{\rm CH}=0.996\pm0.069(\rm stat.)^{+0.083}_{-0.078}(\rm syst.)$ .