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Measurements of \(\bar{\nu}_{\mu}\) and \(\bar{\nu}_{\mu} + \nu_{\mu}\) charged-current cross-sections without detected pions nor protons on water and hydrocarbon at mean antineutrino energy of 0.86 GeV

We report measurements of the flux-integrated \(\bar{\nu}_\mu\) and \(\bar{\nu}_\mu+\nu_\mu\) charged-current cross-sections on water and hydrocarbon targets using the T2K anti-neutrino beam, with a mean neutrino energy of 0.86 GeV. The signal is defined as the (anti-)neutrino charged-current intera...

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Published in:arXiv.org 2020-04
Main Authors: Abe, K, Alt, C, Barrow, D, Batkiewicz-Kwasniak, M, Beloshapkin, A, Berkman, S, Berns, L, Blondel, A, Bolognesi, S, Bonus, T, D Bravo Berguño, Campbell, T, Cartwright, S L, Catanesi, M G, Christodoulou, G, Cook, L, Denner, P F, F Di Lodovico, Dunne, P, Finch, A J, Fujii, Y, Fukuda, Y, Gorin, A, Hadley, D R, Hartz, M, Hayato, Y, Hogan, M, Ishida, T, Ishii, T, Iwamoto, K, Jamieson, B, Johnson, S, Jung, C K, Kabirnezhad, M, Kaboth, A C, Kakuno, H, Kameda, J, Katayama, Y, Katori, T, Kearns, E, Khabibullin, M, Knight, A, Kormos, L L, Koshio, Y, Kubo, H, Lagoda, J, Lamoureux, M, Last, D, Mahn, K, Matsubara, T, Matsushita, K, Mauger, C, McCarthy, M, Mefodiev, A, Minamino, A, Mine, S, Moriyama, S, Mueller, Th A, Murphy, S, Niewczas, K, Nowak, J, Okada, R, Oser, S M, Palomino, J L, Pari, M, Parker, W C, Posiadala-Zezula, M, Reinherz-Aronis, E, Riccio, C, Ruggeri, A C, Ruggles, C, Santucci, G, Scott, M, Seiya, Y, Sekiguchi, T, Shah, R, Shorrock, W, Soler, F J P, Suvorov, S, Suzuki, Y, Sztuc, A A, Takeuchi, Y, Tanaka, H A, Tanaka, S, Toki, W, Touramanis, C, Towstego, T, Uno, W, Vagins, M, Wang, Y, Wendell, R, Wilkinson, C, Wilson, J R, Wood, K, Yamamoto, K, Yasutome, K, Yokoyama, M, Zarnecki, G, Zimmerman, E D, Zsoldos, S
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container_title arXiv.org
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creator Abe, K
Alt, C
Barrow, D
Batkiewicz-Kwasniak, M
Beloshapkin, A
Berkman, S
Berns, L
Blondel, A
Bolognesi, S
Bonus, T
D Bravo Berguño
Campbell, T
Cartwright, S L
Catanesi, M G
Christodoulou, G
Cook, L
Denner, P F
F Di Lodovico
Dunne, P
Finch, A J
Fujii, Y
Fukuda, Y
Gorin, A
Hadley, D R
Hartz, M
Hayato, Y
Hogan, M
Ishida, T
Ishii, T
Iwamoto, K
Jamieson, B
Johnson, S
Jung, C K
Kabirnezhad, M
Kaboth, A C
Kakuno, H
Kameda, J
Katayama, Y
Katori, T
Kearns, E
Khabibullin, M
Knight, A
Kormos, L L
Koshio, Y
Kubo, H
Lagoda, J
Lamoureux, M
Last, D
Mahn, K
Matsubara, T
Matsushita, K
Mauger, C
McCarthy, M
Mefodiev, A
Minamino, A
Mine, S
Moriyama, S
Mueller, Th A
Murphy, S
Niewczas, K
Nowak, J
Okada, R
Oser, S M
Palomino, J L
Pari, M
Parker, W C
Posiadala-Zezula, M
Reinherz-Aronis, E
Riccio, C
Ruggeri, A C
Ruggles, C
Santucci, G
Scott, M
Seiya, Y
Sekiguchi, T
Shah, R
Shorrock, W
Soler, F J P
Suvorov, S
Suzuki, Y
Sztuc, A A
Takeuchi, Y
Tanaka, H A
Tanaka, S
Toki, W
Touramanis, C
Towstego, T
Uno, W
Vagins, M
Wang, Y
Wendell, R
Wilkinson, C
Wilson, J R
Wood, K
Yamamoto, K
Yasutome, K
Yokoyama, M
Zarnecki, G
Zimmerman, E D
Zsoldos, S
description We report measurements of the flux-integrated \(\bar{\nu}_\mu\) and \(\bar{\nu}_\mu+\nu_\mu\) charged-current cross-sections on water and hydrocarbon targets using the T2K anti-neutrino beam, with a mean neutrino 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 nor 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}
doi_str_mv 10.48550/arxiv.2004.13989
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The signal is defined as the (anti-)neutrino charged-current interaction with one induced \(\mu^\pm\) and no detected charged pion nor 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, \(p_{\mu}&gt;400~{\rm MeV}/c\) and \(\theta_{\mu}&lt;30^{\circ}\), in the laboratory frame. Absence of pions and protons in the detectable phase space of "\(p_{\pi}&gt;200~{\rm MeV}/c\) and \(\theta_{\pi}&lt;70^{\circ}\)", and "\(p_{\rm p}&gt;600~{\rm MeV}/c\) and \(\theta_{\rm p}&lt;70^{\circ}\)" is required. In this paper, both of the \(\bar{\nu}_\mu\) cross-sections and \(\bar{\nu}_\mu+\nu_\mu\) cross-sections on water and hydrocarbon targets, and their ratios are provided by using D'Agostini unfolding method. The results of the integrated \(\bar{\nu}_\mu\) 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 \(\sigma_{\rm H_{2}O}/\sigma_{\rm CH} = 0.987\pm0.078(\rm stat.)^{+0.093}_{-0.090}(\rm syst.)\). 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P</creatorcontrib><creatorcontrib>Suvorov, S</creatorcontrib><creatorcontrib>Suzuki, Y</creatorcontrib><creatorcontrib>Sztuc, A A</creatorcontrib><creatorcontrib>Takeuchi, Y</creatorcontrib><creatorcontrib>Tanaka, H A</creatorcontrib><creatorcontrib>Tanaka, S</creatorcontrib><creatorcontrib>Toki, W</creatorcontrib><creatorcontrib>Touramanis, C</creatorcontrib><creatorcontrib>Towstego, T</creatorcontrib><creatorcontrib>Uno, W</creatorcontrib><creatorcontrib>Vagins, M</creatorcontrib><creatorcontrib>Wang, Y</creatorcontrib><creatorcontrib>Wendell, R</creatorcontrib><creatorcontrib>Wilkinson, C</creatorcontrib><creatorcontrib>Wilson, J R</creatorcontrib><creatorcontrib>Wood, K</creatorcontrib><creatorcontrib>Yamamoto, K</creatorcontrib><creatorcontrib>Yasutome, K</creatorcontrib><creatorcontrib>Yokoyama, M</creatorcontrib><creatorcontrib>Zarnecki, G</creatorcontrib><creatorcontrib>Zimmerman, E D</creatorcontrib><creatorcontrib>Zsoldos, S</creatorcontrib><title>Measurements of \(\bar{\nu}_{\mu}\) and \(\bar{\nu}_{\mu} + \nu_{\mu}\) charged-current cross-sections without detected pions nor protons on water and hydrocarbon at mean antineutrino energy of 0.86 GeV</title><title>arXiv.org</title><description>We report measurements of the flux-integrated \(\bar{\nu}_\mu\) and \(\bar{\nu}_\mu+\nu_\mu\) charged-current cross-sections on water and hydrocarbon targets using the T2K anti-neutrino beam, with a mean neutrino 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 nor 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, \(p_{\mu}&gt;400~{\rm MeV}/c\) and \(\theta_{\mu}&lt;30^{\circ}\), in the laboratory frame. Absence of pions and protons in the detectable phase space of "\(p_{\pi}&gt;200~{\rm MeV}/c\) and \(\theta_{\pi}&lt;70^{\circ}\)", and "\(p_{\rm p}&gt;600~{\rm MeV}/c\) and \(\theta_{\rm p}&lt;70^{\circ}\)" is required. In this paper, both of the \(\bar{\nu}_\mu\) cross-sections and \(\bar{\nu}_\mu+\nu_\mu\) cross-sections on water and hydrocarbon targets, and their ratios are provided by using D'Agostini unfolding method. The results of the integrated \(\bar{\nu}_\mu\) 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 \(\bar{\nu}_\mu+\nu_\mu\) 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 \(\sigma_{\rm H_{2}O}/\sigma_{\rm CH}\,=\,0.996\pm0.069(\rm stat.)^{+0.083}_{-0.078}(\rm syst.)\).</description><subject>Cross-sections</subject><subject>Experiments</subject><subject>Hydrocarbons</subject><subject>Modules</subject><subject>Muons</subject><subject>Neutrino beams</subject><subject>Neutrinos</subject><subject>Nucleons</subject><subject>Particle 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arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope></search><sort><creationdate>20200429</creationdate><title>Measurements of \(\bar{\nu}_{\mu}\) and \(\bar{\nu}_{\mu} + \nu_{\mu}\) charged-current cross-sections without detected pions nor protons on water and hydrocarbon at mean antineutrino energy of 0.86 GeV</title><author>Abe, K ; Alt, C ; Barrow, D ; Batkiewicz-Kwasniak, M ; Beloshapkin, A ; Berkman, S ; Berns, L ; Blondel, A ; Bolognesi, S ; Bonus, T ; D Bravo Berguño ; Campbell, T ; Cartwright, S L ; Catanesi, M G ; Christodoulou, G ; Cook, L ; Denner, P F ; F Di Lodovico ; Dunne, P ; Finch, A J ; Fujii, Y ; Fukuda, Y ; Gorin, A ; Hadley, D R ; Hartz, M ; Hayato, Y ; Hogan, M ; Ishida, T ; Ishii, T ; Iwamoto, K ; Jamieson, B ; Johnson, S ; Jung, C K ; Kabirnezhad, M ; Kaboth, A C ; Kakuno, H ; Kameda, J ; Katayama, Y ; Katori, T ; Kearns, E ; Khabibullin, M ; Knight, A ; Kormos, L L ; Koshio, Y ; Kubo, H ; Lagoda, J ; Lamoureux, M ; Last, D ; Mahn, K ; Matsubara, T ; Matsushita, K ; Mauger, C ; McCarthy, M ; Mefodiev, A ; Minamino, A ; Mine, S ; Moriyama, S ; Mueller, Th A ; Murphy, S ; Niewczas, K ; Nowak, J ; Okada, R ; Oser, S M ; Palomino, J L ; Pari, M ; Parker, W C ; Posiadala-Zezula, M ; Reinherz-Aronis, E ; Riccio, C ; Ruggeri, A C ; Ruggles, C ; Santucci, G ; Scott, M ; Seiya, Y ; Sekiguchi, T ; Shah, R ; Shorrock, W ; Soler, F J P ; Suvorov, S ; Suzuki, Y ; Sztuc, A A ; Takeuchi, Y ; Tanaka, H A ; Tanaka, S ; Toki, W ; Touramanis, C ; Towstego, T ; Uno, W ; Vagins, M ; Wang, Y ; Wendell, R ; Wilkinson, C ; Wilson, J R ; Wood, K ; Yamamoto, K ; Yasutome, K ; Yokoyama, M ; Zarnecki, G ; Zimmerman, E D ; Zsoldos, S</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_journals_23964540573</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Cross-sections</topic><topic>Experiments</topic><topic>Hydrocarbons</topic><topic>Modules</topic><topic>Muons</topic><topic>Neutrino beams</topic><topic>Neutrinos</topic><topic>Nucleons</topic><topic>Particle physics</topic><topic>Pions</topic><topic>Protons</topic><toplevel>online_resources</toplevel><creatorcontrib>Abe, K</creatorcontrib><creatorcontrib>Alt, C</creatorcontrib><creatorcontrib>Barrow, D</creatorcontrib><creatorcontrib>Batkiewicz-Kwasniak, M</creatorcontrib><creatorcontrib>Beloshapkin, A</creatorcontrib><creatorcontrib>Berkman, S</creatorcontrib><creatorcontrib>Berns, L</creatorcontrib><creatorcontrib>Blondel, A</creatorcontrib><creatorcontrib>Bolognesi, S</creatorcontrib><creatorcontrib>Bonus, T</creatorcontrib><creatorcontrib>D Bravo 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collection</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Abe, K</au><au>Alt, C</au><au>Barrow, D</au><au>Batkiewicz-Kwasniak, M</au><au>Beloshapkin, A</au><au>Berkman, S</au><au>Berns, L</au><au>Blondel, A</au><au>Bolognesi, S</au><au>Bonus, T</au><au>D Bravo Berguño</au><au>Campbell, T</au><au>Cartwright, S L</au><au>Catanesi, M G</au><au>Christodoulou, G</au><au>Cook, L</au><au>Denner, P F</au><au>F Di Lodovico</au><au>Dunne, P</au><au>Finch, A J</au><au>Fujii, Y</au><au>Fukuda, Y</au><au>Gorin, A</au><au>Hadley, D R</au><au>Hartz, M</au><au>Hayato, Y</au><au>Hogan, M</au><au>Ishida, T</au><au>Ishii, T</au><au>Iwamoto, K</au><au>Jamieson, B</au><au>Johnson, S</au><au>Jung, C K</au><au>Kabirnezhad, M</au><au>Kaboth, A C</au><au>Kakuno, H</au><au>Kameda, J</au><au>Katayama, Y</au><au>Katori, T</au><au>Kearns, E</au><au>Khabibullin, M</au><au>Knight, A</au><au>Kormos, L L</au><au>Koshio, Y</au><au>Kubo, H</au><au>Lagoda, J</au><au>Lamoureux, M</au><au>Last, D</au><au>Mahn, K</au><au>Matsubara, T</au><au>Matsushita, K</au><au>Mauger, C</au><au>McCarthy, M</au><au>Mefodiev, A</au><au>Minamino, A</au><au>Mine, S</au><au>Moriyama, S</au><au>Mueller, Th A</au><au>Murphy, S</au><au>Niewczas, K</au><au>Nowak, J</au><au>Okada, R</au><au>Oser, S M</au><au>Palomino, J L</au><au>Pari, M</au><au>Parker, W C</au><au>Posiadala-Zezula, M</au><au>Reinherz-Aronis, E</au><au>Riccio, C</au><au>Ruggeri, A C</au><au>Ruggles, C</au><au>Santucci, G</au><au>Scott, M</au><au>Seiya, Y</au><au>Sekiguchi, T</au><au>Shah, R</au><au>Shorrock, W</au><au>Soler, F J P</au><au>Suvorov, S</au><au>Suzuki, Y</au><au>Sztuc, A A</au><au>Takeuchi, Y</au><au>Tanaka, H A</au><au>Tanaka, S</au><au>Toki, W</au><au>Touramanis, C</au><au>Towstego, T</au><au>Uno, W</au><au>Vagins, M</au><au>Wang, Y</au><au>Wendell, R</au><au>Wilkinson, C</au><au>Wilson, J R</au><au>Wood, K</au><au>Yamamoto, K</au><au>Yasutome, K</au><au>Yokoyama, M</au><au>Zarnecki, G</au><au>Zimmerman, E D</au><au>Zsoldos, S</au><format>book</format><genre>document</genre><ristype>GEN</ristype><atitle>Measurements of \(\bar{\nu}_{\mu}\) and \(\bar{\nu}_{\mu} + \nu_{\mu}\) charged-current cross-sections without detected pions nor protons on water and hydrocarbon at mean antineutrino energy of 0.86 GeV</atitle><jtitle>arXiv.org</jtitle><date>2020-04-29</date><risdate>2020</risdate><eissn>2331-8422</eissn><abstract>We report measurements of the flux-integrated \(\bar{\nu}_\mu\) and \(\bar{\nu}_\mu+\nu_\mu\) charged-current cross-sections on water and hydrocarbon targets using the T2K anti-neutrino beam, with a mean neutrino 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 nor 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, \(p_{\mu}&gt;400~{\rm MeV}/c\) and \(\theta_{\mu}&lt;30^{\circ}\), in the laboratory frame. Absence of pions and protons in the detectable phase space of "\(p_{\pi}&gt;200~{\rm MeV}/c\) and \(\theta_{\pi}&lt;70^{\circ}\)", and "\(p_{\rm p}&gt;600~{\rm MeV}/c\) and \(\theta_{\rm p}&lt;70^{\circ}\)" is required. In this paper, both of the \(\bar{\nu}_\mu\) cross-sections and \(\bar{\nu}_\mu+\nu_\mu\) cross-sections on water and hydrocarbon targets, and their ratios are provided by using D'Agostini unfolding method. The results of the integrated \(\bar{\nu}_\mu\) 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 \(\bar{\nu}_\mu+\nu_\mu\) 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 \(\sigma_{\rm H_{2}O}/\sigma_{\rm CH}\,=\,0.996\pm0.069(\rm stat.)^{+0.083}_{-0.078}(\rm syst.)\).</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.2004.13989</doi><oa>free_for_read</oa></addata></record>
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subjects Cross-sections
Experiments
Hydrocarbons
Modules
Muons
Neutrino beams
Neutrinos
Nucleons
Particle physics
Pions
Protons
title Measurements of \(\bar{\nu}_{\mu}\) and \(\bar{\nu}_{\mu} + \nu_{\mu}\) 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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