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<dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:invenio="http://invenio-software.org/elements/1.0" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd"><dc:identifier>doi:10.1140/epjc/s10052-025-14938-9</dc:identifier><dc:language>eng</dc:language><dc:creator>Abe, K.</dc:creator><dc:creator>Afif, M. T.</dc:creator><dc:creator>Anthony, L.</dc:creator><dc:creator>Araya, A.</dc:creator><dc:creator>Arguello Quiroga, A.</dc:creator><dc:creator>Arimoto, S.</dc:creator><dc:creator>Batkiewicz-Kwasniak, M.</dc:creator><dc:creator>Beauchêne, A.</dc:creator><dc:creator>Casado, M. P.</dc:creator><dc:creator>Catanesi, M. G.</dc:creator><dc:creator>Cavanagh, C.</dc:creator><dc:creator>Cebrián, S.</dc:creator><dc:title>Sensitivity of the Hyper-Kamiokande experiment to neutrino oscillation parameters using accelerator neutrinos</dc:title><dc:identifier>ART-2026-148627</dc:identifier><dc:description>This paper presents the expected sensitivity to the neutrino oscillation parameters of the Hyper-Kamiokande long-baseline program. The Hyper-Kamiokande experiment, currently under construction in Japan, will measure the oscillations of accelerator-produced neutrinos with thousands of selected events per sample: this corresponds to an increase of statistics of a factor 25–100 with respect to recent results from the currently-running long-baseline neutrino oscillation experiment in Japan, T2K. In the most favorable scenario we will achieve the discovery of Charge-Parity (CP) violation in neutrino oscillation at 5σ C.L. in less than 3 years. With 10 years of data-taking, and assuming a neutrino : antineutrino beam running ratio of 1:3, a CP violation discovery at 5σ C.L. is possible for more than 60% of the actual values of the CP-violating phase, δCP. Moreover, we will measure δCP with a precision ranging from 20∘, in the case of maximal CP violation, to 6∘, in the case of CP conservation. We aim to achieve a 0.5% resolution on the Δm322 parameter, and a resolution between 3% and 0.5% on the sin2θ23 parameter, depending on its true value. These results are obtained by extending the analysis methods of T2K with dedicated tuning to take into account the Hyper-Kamiokande design: the larger far detector, the more powerful beam, the upgraded near detector ND280, and the planned additional Intermediate Water Cherenkov Detector.</dc:description><dc:date>2026</dc:date><dc:source>http://zaguan.unizar.es/record/169988</dc:source><dc:doi>10.1140/epjc/s10052-025-14938-9</dc:doi><dc:identifier>http://zaguan.unizar.es/record/169988</dc:identifier><dc:identifier>oai:zaguan.unizar.es:169988</dc:identifier><dc:relation>info:eu-repo/grantAgreement/ES/MCIU/PID2022-139198NB-I00</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MICINN/PID2021-124050NB-C31</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MICINN/PID2022-136297NB-I00</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/NextGenerationEU/PRTR</dc:relation><dc:identifier.citation>The European Physical Journal C 86, 2 (2026), [18 pp.]</dc:identifier.citation><dc:rights>by</dc:rights><dc:rights>https://creativecommons.org/licenses/by/4.0/deed.es</dc:rights><dc:rights>info:eu-repo/semantics/openAccess</dc:rights></dc:dc>

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