{"title":"中微子对18O的诱导反应及水中18O混合物Cherenkov探测器对超新星中微子事件的影响","authors":"Toshio Suzuki , Ken'ichiro Nakazato , Makoto Sakuda","doi":"10.1016/j.nuclphysa.2023.122719","DOIUrl":null,"url":null,"abstract":"<div><p>Neutrino-nucleus reaction cross sections on <sup>18</sup>O are evaluated by shell-model calculations and compared with those on <sup>16</sup>O. Important contributions from Gamow-Teller transitions are noticed for <sup>18</sup>O (<span><math><msub><mrow><mi>ν</mi></mrow><mrow><mi>e</mi></mrow></msub></math></span>, e<sup>−</sup>) <sup>18</sup>F in contrary to the case for <sup>16</sup>O, where spin-dipole transitions are dominant contributions. Calculated cross sections for <sup>18</sup>O (<span><math><msub><mrow><mi>ν</mi></mrow><mrow><mi>e</mi></mrow></msub></math></span>, e<sup>−</sup>) <sup>18</sup>F are shown to be larger than for <sup>16</sup>O at low neutrino energies below 20 MeV in natural water with the 0.205% admixture of <sup>18</sup>O due to the lower threshold energy (1.66 MeV) for <sup>18</sup>O than that for <sup>16</sup><span>O (15.42 MeV). The resulting electron spectra, that is, the cross sections as functions of emitted electron energy </span><span><math><msub><mrow><mi>T</mi></mrow><mrow><mi>e</mi></mrow></msub></math></span>, are also shown to be quite different, reflecting the different threshold energies. The electron spectra from (<span><math><msub><mrow><mi>ν</mi></mrow><mrow><mi>e</mi></mrow></msub></math></span>, e<sup>−</sup>) reactions on <sup>18</sup>O and <sup>16</sup><span>O in water Cherenkov detectors for supernova<span> neutrino detection are investigated for both the cases with and without the neutrino oscillation and compared with those of the neutrino-electron scattering. It has been shown that the contribution from </span></span><sup>18</sup>O (0.205% mixture) enhances the rates from <sup>16</sup>O by 60% for the case without the oscillation and by 20-30% for the case with the oscillation below <span><math><msub><mrow><mi>T</mi></mrow><mrow><mi>e</mi></mrow></msub></math></span> =20 MeV. For the case with the neutrino oscillation, the event rates for <sup>18</sup>O and <sup>16</sup>O become comparable to those of the neutrino-electron scattering. However, their rates at low energy (<span><math><msub><mrow><mi>T</mi></mrow><mrow><mi>e</mi></mrow></msub><mo><</mo></math></span> 20 MeV) are much lower than those of the neutrino-electron scattering, which is important for the pointing accuracy to the supernova direction.</p></div>","PeriodicalId":19246,"journal":{"name":"Nuclear Physics A","volume":null,"pages":null},"PeriodicalIF":1.7000,"publicationDate":"2023-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Neutrino-induced reactions on 18O and implications of 18O mixture in water Cherenkov detectors on supernova neutrino events\",\"authors\":\"Toshio Suzuki , Ken'ichiro Nakazato , Makoto Sakuda\",\"doi\":\"10.1016/j.nuclphysa.2023.122719\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>Neutrino-nucleus reaction cross sections on <sup>18</sup>O are evaluated by shell-model calculations and compared with those on <sup>16</sup>O. Important contributions from Gamow-Teller transitions are noticed for <sup>18</sup>O (<span><math><msub><mrow><mi>ν</mi></mrow><mrow><mi>e</mi></mrow></msub></math></span>, e<sup>−</sup>) <sup>18</sup>F in contrary to the case for <sup>16</sup>O, where spin-dipole transitions are dominant contributions. Calculated cross sections for <sup>18</sup>O (<span><math><msub><mrow><mi>ν</mi></mrow><mrow><mi>e</mi></mrow></msub></math></span>, e<sup>−</sup>) <sup>18</sup>F are shown to be larger than for <sup>16</sup>O at low neutrino energies below 20 MeV in natural water with the 0.205% admixture of <sup>18</sup>O due to the lower threshold energy (1.66 MeV) for <sup>18</sup>O than that for <sup>16</sup><span>O (15.42 MeV). The resulting electron spectra, that is, the cross sections as functions of emitted electron energy </span><span><math><msub><mrow><mi>T</mi></mrow><mrow><mi>e</mi></mrow></msub></math></span>, are also shown to be quite different, reflecting the different threshold energies. The electron spectra from (<span><math><msub><mrow><mi>ν</mi></mrow><mrow><mi>e</mi></mrow></msub></math></span>, e<sup>−</sup>) reactions on <sup>18</sup>O and <sup>16</sup><span>O in water Cherenkov detectors for supernova<span> neutrino detection are investigated for both the cases with and without the neutrino oscillation and compared with those of the neutrino-electron scattering. It has been shown that the contribution from </span></span><sup>18</sup>O (0.205% mixture) enhances the rates from <sup>16</sup>O by 60% for the case without the oscillation and by 20-30% for the case with the oscillation below <span><math><msub><mrow><mi>T</mi></mrow><mrow><mi>e</mi></mrow></msub></math></span> =20 MeV. For the case with the neutrino oscillation, the event rates for <sup>18</sup>O and <sup>16</sup>O become comparable to those of the neutrino-electron scattering. However, their rates at low energy (<span><math><msub><mrow><mi>T</mi></mrow><mrow><mi>e</mi></mrow></msub><mo><</mo></math></span> 20 MeV) are much lower than those of the neutrino-electron scattering, which is important for the pointing accuracy to the supernova direction.</p></div>\",\"PeriodicalId\":19246,\"journal\":{\"name\":\"Nuclear Physics A\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":1.7000,\"publicationDate\":\"2023-10-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Physics A\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0375947423001227\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, NUCLEAR\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Physics A","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0375947423001227","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, NUCLEAR","Score":null,"Total":0}
Neutrino-induced reactions on 18O and implications of 18O mixture in water Cherenkov detectors on supernova neutrino events
Neutrino-nucleus reaction cross sections on 18O are evaluated by shell-model calculations and compared with those on 16O. Important contributions from Gamow-Teller transitions are noticed for 18O (, e−) 18F in contrary to the case for 16O, where spin-dipole transitions are dominant contributions. Calculated cross sections for 18O (, e−) 18F are shown to be larger than for 16O at low neutrino energies below 20 MeV in natural water with the 0.205% admixture of 18O due to the lower threshold energy (1.66 MeV) for 18O than that for 16O (15.42 MeV). The resulting electron spectra, that is, the cross sections as functions of emitted electron energy , are also shown to be quite different, reflecting the different threshold energies. The electron spectra from (, e−) reactions on 18O and 16O in water Cherenkov detectors for supernova neutrino detection are investigated for both the cases with and without the neutrino oscillation and compared with those of the neutrino-electron scattering. It has been shown that the contribution from 18O (0.205% mixture) enhances the rates from 16O by 60% for the case without the oscillation and by 20-30% for the case with the oscillation below =20 MeV. For the case with the neutrino oscillation, the event rates for 18O and 16O become comparable to those of the neutrino-electron scattering. However, their rates at low energy ( 20 MeV) are much lower than those of the neutrino-electron scattering, which is important for the pointing accuracy to the supernova direction.
期刊介绍:
Nuclear Physics A focuses on the domain of nuclear and hadronic physics and includes the following subsections: Nuclear Structure and Dynamics; Intermediate and High Energy Heavy Ion Physics; Hadronic Physics; Electromagnetic and Weak Interactions; Nuclear Astrophysics. The emphasis is on original research papers. A number of carefully selected and reviewed conference proceedings are published as an integral part of the journal.