- Main
Measurements of ν̄μ and ν̄μ + νμ charged-current cross-sections without detected pions nor protons on water and hydrocarbon at mean antineutrino energy of 0.86 GeV
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- Thompson, LF;
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- Uno, W;
- Vagins, M;
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- Vargas, D;
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- Vinning, WGS;
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- Volkov, VV;
- Wachala, T;
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- Wascko, MO;
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- Wilking, MJ;
- Wilkinson, C;
- Wilson, JR;
- Wilson, RJ;
- Wood, K;
- Wret, C;
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- Yamada, Y;
- Yamamoto, K;
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- 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, ED;
- Zito, M;
- Zsoldos, S;
- Zykova, A
Abstract
We report measurements of the flux-integrated and + 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 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, 400 and 30 , in the laboratory frame. An absence of pions and protons in the detectable phase spaces of 200, 70 and 600, 70 is required. In this paper, both the; cross-sections and +; cross-sections on water and hydrocarbon targets and their ratios are provided by using the D'Agostini unfolding method. The results of the integrated ; 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 +; 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.);.
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