Physics Potential of a Long Baseline Neutrino Oscillation Experiment Using J-PARC Neutrino Beam and Hyper-Kamiokande

preprint2015arXivOpen access
Hyper-Kamiokande Proto-Collaboraion:K. AbeH. AiharaC. AndreopoulosI. AnghelA. ArigaT. ArigaR. AsfandiyarovM. AskinsJ. J. BackP. BallettM. BarbiG. J. BarkerG. BarrF. BayP. BeltrameV. BerardiM. BergevinS. BerkmanT. BerryS. BhadraF. d. M. BlaszczykA. BlondelS. BolognesiS. B. BoydA. BravarC. BronnerF. S. CafagnaG. CarminatiS. L. CartwrightM. G. CatanesiK. ChoiJ. H. ChoiG. CollazuolG. CowanL. CremonesiG. DaviesG. De RosaC. DenshamJ. DetwilerD. DewhurstF. Di LodovicoS. Di LuiseO. DrapierS. EmeryA. EreditatoP. FernándezT. FeuselsA. FinchM. FittonM. FriendY. FujiiY. FukudaD. FukudaV. GalymovK. GanezerM. GoninP. GumplingerD. R. HadleyL. HaegelA. HaeslerY. HagaB. HartfielM. HartzY. HayatoM. HierholzerJ. HillA. HimmelS. HirotaS. HoriuchiK. HuangA. K. IchikawaT. IijimaM. IkedaJ. ImberK. InoueJ. InslerR. A. IntontiT. IrvineT. IshidaH. IshinoM. IshitsukaY. ItowA. IzmaylovB. JamiesonH. I. JangM. JiangK. K. JooC. K. JungA. KabothT. KajitaJ. KamedaY. KaradhzovT. KatoriE. KearnsM. KhabibullinA. KhotjantsevJ. Y. KimS. B. KimY. KishimotoT. KobayashiM. KogaA. KonakaL. L. KormosA. KorzenevY. KoshioW. R. KroppY. KudenkoT. KutterM. KuzeL. LabargaJ. LagodaM. LavederM. LaweJ. G. LearnedI. T. LimT. LindnerA. LonghinL. LudoviciW. MaL. MagalettiK. MahnM. MalekC. MarianiL. MartiJ. F. MartinC. MartinP. P. J. MartinsE. MazzucatoN. McCauleyK. S. McFarlandC. McGrewM. MezzettoH. MinakataA. MinaminoS. MineO. MineevM. MiuraJ. MonroeT. MoriS. MoriyamaT. MuellerF. MuheimM. NakahataK. NakamuraT. NakayaS. NakayamaM. NeedhamT. NichollsM. NirkkoY. NishimuraE. NoahJ. NowakH. NunokawaH. M. O'KeeffeY. OkajimaK. OkumuraS. M. OserE. O'SullivanT. OvsiannikovaR. A. OwenY. OyamaJ. PérezM. Y. PacV. PalladinoJ. L. PalominoV. PaoloneD. PayneO. PerevozchikovJ. D. PerkinC. PistilloS. PlayferM. Posiadala-ZezulaJ. -M. PoutissouB. QuilainM. QuintoE. RadicioniP. N. RatoffM. RavonelM. A. RaynerA. RedijF. RetiereC. RiccioE. RichardE. RondioH. J. RoseM. Ross-LonerganC. RottS. D. RountreeA. RubbiaR. SaccoM. SakudaM. C. SanchezE. ScantamburloK. ScholbergM. ScottY. SeiyaT. SekiguchiH. SekiyaA. ShaikhievI. ShimizuM. ShiozawaS. ShortG. SinnisM. B. SmyJ. SobczykH. W. SobelT. StewartJ. L. StoneY. SudaY. SuzukiA. T. SuzukiR. SvobodaR. TacikA. TakedaA. TaketaY. TakeuchiH. A. TanakaH. K. M. TanakaH. TanakaR. TerriL. F. ThompsonM. ThorpeS. TobayamaN. TolichT. TomuraC. TouramanisT. TsukamotoM. TzanovY. UchidaM. R. VaginsG. VasseurR. B. VogelaarC. W. WalterD. WarkM. O. WasckoA. WeberR. WendellR. J. WilkesM. J. WilkingJ. R. WilsonT. XinK. YamamotoC. YanagisawaT. YanoS. YenN. YershovM. YokoyamaM. Zito

Abstract

Hyper-Kamiokande will be a next generation underground water Cherenkov detector with a total (fiducial) mass of 0.99 (0.56) million metric tons, approximately 20 (25) times larger than that of Super-Kamiokande. One of the main goals of Hyper-Kamiokande is the study of CPCP asymmetry in the lepton sector using accelerator neutrino and anti-neutrino beams. In this paper, the physics potential of a long baseline neutrino experiment using the Hyper-Kamiokande detector and a neutrino beam from the J-PARC proton synchrotron is presented. The analysis uses the framework and systematic uncertainties derived from the ongoing T2K experiment. With a total exposure of 7.5 MW ×\times 107^7 sec integrated proton beam power (corresponding to 1.56×10221.56\times10^{22} protons on target with a 30 GeV proton beam) to a 2.52.5-degree off-axis neutrino beam, it is expected that the leptonic CPCP phase δCPδ_{CP} can be determined to better than 19 degrees for all possible values of δCPδ_{CP}, and CPCP violation can be established with a statistical significance of more than 3 σ3\,σ (5 σ5\,σ) for 76%76\% (58%58\%) of the δCPδ_{CP} parameter space. Using both νeν_e appearance and νμν_μ disappearance data, the expected 1σσ uncertainty of sin⁡2θ23\sin^2θ_{23} is 0.015(0.006) for sin⁡2θ23=0.5(0.45)\sin^2θ_{23}=0.5(0.45).

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