Neutrino Oscillation Physics Potential of the T2K Experiment

preprint2015arXivOpen access
K. AbeJ. AdamH. AiharaT. AkiriC. AndreopoulosS. AokiA. ArigaS. AssylbekovD. AutieroM. BarbiG. J. BarkerG. BarrP. Bartet-FriburgM. BassM. BatkiewiczF. BayV. BerardiB. E. BergerS. BerkmanS. BhadraF. d. M. BlaszczykA. BlondelC. BojechkoS. BordoniS. B. BoydD. BrailsfordA. BravarC. BronnerN. BuchananR. G. CallandJ. Caravaca Rodr'iguezS. L. CartwrightR. CastilloM. G. CatanesiA. CerveraD. CherdackG. ChristodoulouA. CliftonJ. ColemanS. J. ColemanG. CollazuolK. ConnollyL. CremonesiA. DabrowskaI. DankoR. DasS. DavisP. de PerioG. De RosaT. DealtryS. R. DennisC. DenshamD. DewhurstF. Di LodovicoS. Di LuiseO. DrapierT. DuboyskiK. DuffyJ. DumarchezS. DytmanM. DziewieckiS. Emery-SchrenkA. EreditatoL. EscuderoT. FeuselsA. J. FinchG. A. FiorentiniM. FriendY. FujiiY. FukudaA. P. FurmanskiV. GalymovA. GarciaS. GiffinC. GigantiK. GiljeD. GoeldiT. GolanM. GoninN. GrantD. GudinD. R. HadleyL. HaegelA. HaeslerM. D. HaighP. HamiltonD. HansenT. HaraM. HartzT. HasegawaN. C. HastingsT. HayashinoY. HayatoC. HeartyR. L. HelmerM. HierholzerJ. HignightA. HillairetA. HimmelT. HirakiS. HirotaJ. HoleczekS. HorikawaK. HuangA. K. IchikawaK. IekiM. IevaM. IkedaJ. ImberJ. InslerT. J. IrvineT. IshidaT. IshiiE. IwaiK. IwamotoK. IyogiA. IzmaylovA. JacobB. JamiesonR. A. JohnsonS. JohnsonJ. H. JoP. JonssonC. K. JungM. KabirnezhadA. C. KabothT. KajitaH. KakunoJ. KamedaY. KanazawaD. KarlenI. KarpikovT. KatoriE. KearnsM. KhabibullinA. KhotjantsevD. KielczewskaT. KikawaA. KilinskiJ. KimS. KingJ. KisielP. KitchingT. KobayashiL. KochT. KogaA. KolacekeA. KonakaL. L. KormosA. KorzenevY. KoshioW. KroppH. KuboY. KudenkoR. KurjataT. KutterJ. LagodaK. LaihemI. LamontE. LarkinM. LavederM. LaweM. LazosT. LindnerC. ListerR. P. LitchfieldA. LonghinJ. P. LopezL. LudoviciL. MagalettiK. MahnM. MalekS. ManlyA. D. MarinoJ. MarteauJ. F. MartinP. MartinsS. MartynenkoT. MaruyamaV. MatveevK. MavrokoridisE. MazzucatoM. McCarthyN. McCauleyK. S. McFarlandC. McGrewA. MefodievC. MetelkoM. MezzettoP. MijakowskiC. A. MillerA. MinaminoO. MineevA. MissertM. MiuraS. MoriyamaTh. A. MuellerA. MurakamiM. MurdochS. MurphyJ. MyslikT. NakadairaM. NakahataK. G. NakamuraK. NakamuraS. NakayamaT. NakayaK. NakayoshiC. NantaisC. NielsenM. NirkkoK. NishikawaY. NishimuraJ. NowakH. M. O'KeeffeR. OhtaK. OkumuraT. OkusawaW. OryszczakS. M. OserT. OvsyannikovaR. A. OwenY. OyamaV. PalladinoJ. L. PalominoV. PaoloneD. PayneO. PerevozchikovJ. D. PerkinY. PetrovL. PickardE. S. Pinzon GuerraC. PistilloP. PlonskiE. PoplawskaB. PopovM. Posiadala-ZezulaJ. -M. PoutissouR. PoutissouP. PrzewlockiB. QuilainE. RadicioniP. N. RatoffM. RavonelM. A. M. RaynerA. RedijM. ReevesE. Reinherz-AronisC. RiccioP. A. RodriguesP. RojasE. RondioS. RothA. RubbiaD. RuterboriesR. SaccoK. SakashitaF. S'anchezF. SatoE. ScantamburloK. ScholbergS. SchoppmannJ. SchwehrM. ScottY. SeiyaT. SekiguchiH. SekiyaD. SgalabernaR. ShahF. ShakerM. ShiozawaS. ShortY. ShustrovP. SinclairB. SmithM. SmyJ. T. SobczykH. SobelM. SorelL. SouthwellP. StamoulisJ. SteinmannB. StillY. SudaA. SuzukiK. SuzukiS. Y. SuzukiY. SuzukiR. TacikM. TadaS. TakahashiA. TakedaY. TakeuchiH. K. TanakaH. A. TanakaM. M. TanakaD. TerhorstR. TerriL. F. ThompsonA. ThorleyS. TobayamaW. TokiT. TomuraY. TotsukaC. TouramanisT. TsukamotoM. TzanovY. UchidaA. VacheretM. VaginsG. VasseurT. WachalaA. V. WaldronK. WakamatsuC. W. WalterD. WarkW. WarzychaM. O. WasckoA. WeberR. WendellR. J. WilkesM. J. WilkingC. WilkinsonZ. WilliamsonJ. R. WilsonR. J. WilsonT. WongjiradY. YamadaK. YamamotoC. YanagisawaT. YanoS. YenN. YershovM. YokoyamaK. YoshidaT. YuanM. YuA. ZalewskaJ. ZalipskaL. ZambelliK. ZarembaM. ZiembickiE. D. ZimmermanM. ZitoJ. Zmuda

Abstract

The observation of the recent electron neutrino appearance in a muon neutrino beam and the high-precision measurement of the mixing angle θ13θ_{13} have led to a re-evaluation of the physics potential of the T2K long-baseline neutrino oscillation experiment. Sensitivities are explored for CP violation in neutrinos, non-maximal sin⁡22θ23\sin^22θ_{23}, the octant of θ23θ_{23}, and the mass hierarchy, in addition to the measurements of δCPδ_{CP}, sin⁡2θ23\sin^2θ_{23}, and Δm322Δm^2_{32}, for various combinations of νν-mode and νˉ\barν-mode data-taking. With an exposure of 7.8×10217.8\times10^{21}~protons-on-target, T2K can achieve 1-σσ resolution of 0.050(0.054) on sin⁡2θ23\sin^2θ_{23} and 0.040(0.045)×10−3 eV20.040(0.045)\times10^{-3}~\rm{eV}^2 on Δm322Δm^2_{32} for 100\%(50\%) neutrino beam mode running assuming sin⁡2θ23=0.5\sin^2θ_{23}=0.5 and Δm322=2.4×10−3Δm^2_{32} = 2.4\times10^{-3} eV2^2. T2K will have sensitivity to the CP-violating phase δCPδ_{\rm{CP}} at 90\% C.L. or better over a significant range. For example, if sin⁡22θ23\sin^22θ_{23} is maximal (i.e θ23θ_{23}=45∘45^\circ) the range is −115∘<δCP<−60∘-115^\circ<δ_{\rm{CP}}<-60^\circ for normal hierarchy and +50∘<δCP<+130∘+50^\circ<δ_{\rm{CP}}<+130^\circ for inverted hierarchy. When T2K data is combined with data from the NOννA experiment, the region of oscillation parameter space where there is sensitivity to observe a non-zero δCPδ_{CP} is substantially increased compared to if each experiment is analyzed alone.

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