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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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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 |
format | article |
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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, \(p_{\mu}>400~{\rm MeV}/c\) and \(\theta_{\mu}<30^{\circ}\), in the laboratory frame. Absence of pions and protons in the detectable phase space of "\(p_{\pi}>200~{\rm MeV}/c\) and \(\theta_{\pi}<70^{\circ}\)", and "\(p_{\rm p}>600~{\rm MeV}/c\) and \(\theta_{\rm p}<70^{\circ}\)" 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><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.2004.13989</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Cross-sections ; Experiments ; Hydrocarbons ; Modules ; Muons ; Neutrino beams ; Neutrinos ; Nucleons ; Particle physics ; Pions ; Protons</subject><ispartof>arXiv.org, 2020-04</ispartof><rights>2020. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.proquest.com/docview/2396454057?pq-origsite=primo$$EHTML$$P50$$Gproquest$$Hfree_for_read</linktohtml><link.rule.ids>780,784,25753,27925,37012,44590</link.rule.ids></links><search><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 Berguño</creatorcontrib><creatorcontrib>Campbell, T</creatorcontrib><creatorcontrib>Cartwright, S L</creatorcontrib><creatorcontrib>Catanesi, M G</creatorcontrib><creatorcontrib>Christodoulou, G</creatorcontrib><creatorcontrib>Cook, L</creatorcontrib><creatorcontrib>Denner, P F</creatorcontrib><creatorcontrib>F Di Lodovico</creatorcontrib><creatorcontrib>Dunne, P</creatorcontrib><creatorcontrib>Finch, A J</creatorcontrib><creatorcontrib>Fujii, Y</creatorcontrib><creatorcontrib>Fukuda, Y</creatorcontrib><creatorcontrib>Gorin, A</creatorcontrib><creatorcontrib>Hadley, D R</creatorcontrib><creatorcontrib>Hartz, M</creatorcontrib><creatorcontrib>Hayato, Y</creatorcontrib><creatorcontrib>Hogan, M</creatorcontrib><creatorcontrib>Ishida, T</creatorcontrib><creatorcontrib>Ishii, T</creatorcontrib><creatorcontrib>Iwamoto, K</creatorcontrib><creatorcontrib>Jamieson, B</creatorcontrib><creatorcontrib>Johnson, S</creatorcontrib><creatorcontrib>Jung, C K</creatorcontrib><creatorcontrib>Kabirnezhad, M</creatorcontrib><creatorcontrib>Kaboth, A C</creatorcontrib><creatorcontrib>Kakuno, H</creatorcontrib><creatorcontrib>Kameda, J</creatorcontrib><creatorcontrib>Katayama, Y</creatorcontrib><creatorcontrib>Katori, T</creatorcontrib><creatorcontrib>Kearns, E</creatorcontrib><creatorcontrib>Khabibullin, M</creatorcontrib><creatorcontrib>Knight, A</creatorcontrib><creatorcontrib>Kormos, L L</creatorcontrib><creatorcontrib>Koshio, Y</creatorcontrib><creatorcontrib>Kubo, H</creatorcontrib><creatorcontrib>Lagoda, J</creatorcontrib><creatorcontrib>Lamoureux, M</creatorcontrib><creatorcontrib>Last, D</creatorcontrib><creatorcontrib>Mahn, K</creatorcontrib><creatorcontrib>Matsubara, T</creatorcontrib><creatorcontrib>Matsushita, K</creatorcontrib><creatorcontrib>Mauger, C</creatorcontrib><creatorcontrib>McCarthy, M</creatorcontrib><creatorcontrib>Mefodiev, A</creatorcontrib><creatorcontrib>Minamino, A</creatorcontrib><creatorcontrib>Mine, S</creatorcontrib><creatorcontrib>Moriyama, S</creatorcontrib><creatorcontrib>Mueller, Th A</creatorcontrib><creatorcontrib>Murphy, S</creatorcontrib><creatorcontrib>Niewczas, K</creatorcontrib><creatorcontrib>Nowak, J</creatorcontrib><creatorcontrib>Okada, R</creatorcontrib><creatorcontrib>Oser, S M</creatorcontrib><creatorcontrib>Palomino, J L</creatorcontrib><creatorcontrib>Pari, M</creatorcontrib><creatorcontrib>Parker, W C</creatorcontrib><creatorcontrib>Posiadala-Zezula, M</creatorcontrib><creatorcontrib>Reinherz-Aronis, E</creatorcontrib><creatorcontrib>Riccio, C</creatorcontrib><creatorcontrib>Ruggeri, A C</creatorcontrib><creatorcontrib>Ruggles, C</creatorcontrib><creatorcontrib>Santucci, G</creatorcontrib><creatorcontrib>Scott, M</creatorcontrib><creatorcontrib>Seiya, Y</creatorcontrib><creatorcontrib>Sekiguchi, T</creatorcontrib><creatorcontrib>Shah, R</creatorcontrib><creatorcontrib>Shorrock, W</creatorcontrib><creatorcontrib>Soler, F J 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, \(p_{\mu}>400~{\rm MeV}/c\) and \(\theta_{\mu}<30^{\circ}\), in the laboratory frame. Absence of pions and protons in the detectable phase space of "\(p_{\pi}>200~{\rm MeV}/c\) and \(\theta_{\pi}<70^{\circ}\)", and "\(p_{\rm p}>600~{\rm MeV}/c\) and \(\theta_{\rm p}<70^{\circ}\)" 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, \(p_{\mu}>400~{\rm MeV}/c\) and \(\theta_{\mu}<30^{\circ}\), in the laboratory frame. Absence of pions and protons in the detectable phase space of "\(p_{\pi}>200~{\rm MeV}/c\) and \(\theta_{\pi}<70^{\circ}\)", and "\(p_{\rm p}>600~{\rm MeV}/c\) and \(\theta_{\rm p}<70^{\circ}\)" 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> |
fulltext | fulltext |
identifier | EISSN: 2331-8422 |
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issn | 2331-8422 |
language | eng |
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source | Publicly Available Content Database |
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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