6533b824fe1ef96bd127fea7
RESEARCH PRODUCT
Updated T2K measurements of muon neutrino and antineutrino disappearance using 1.5×1021 protons on target
S. MartynenkoJ. LagodaR. J. WilsonC. K. JungA. N. KhotjantsevM. IkedaP. F. DennerMasato ShiozawaL. LudoviciS. BhadraT. MaruyamaD. ShawW. H. TokiS. KingK. ZarembaA. T. SuzukiJ. F. MartinG.d. BarrR. TacikD. FukudaW. R. KroppD. AutieroT. NakadairaE. KearnsS. TobayamaT. ShirahigeMasashi YokoyamaH. KakunoL. ZambelliWilsonT. FeuselsK. NakamuraY. TakeuchiT. KajitaA. HiramotoT. HasegawaA. MefodievM. R. VaginsA. BlondelA. RychterTsuyoshi NakayaK. NishikawaL. MaretJ. L. PalominoP. NovellaJan T. SobczykM. M. KhabibullinAtsushi TakedaRyuji TamuraT. YanoYoshikazu YamadaP. N. RatoffA. ShaikhievT. KutterR. G. CallandF. SanchezT. TomuraM. FriendK. MavrokoridisF. GizzarelliXianguo LuTeppei KatoriGiovanni FiorentiniO. DrapierC. W. WalterS. BordoniS. BordoniAlessandro RuggeriA. MinaminoH.a. TanakaS. BerkmanS. BerkmanM. ZitoAndré RubbiaM. HartzE. RadicioniS. V. CaoJ. D. PerkinM. MccarthyT. ThakoreS. B. BoydM. BarbiAlyssa GarciaDennisTakahiro HirakiS. ManlyE. LarkinTodd D. StewartR. A. IntontiJ. T. HaighM. J. WilkingD. KarlenY. PetrovC. WilkinsonHiroyuki SekiyaA. CliftonC. TouramanisAkitaka ArigaKo OkumuraA. CerveraM. JiangAntonio EreditatoT. LouM. YuM. LaweN. YershovR. J. WilkesJ. HaradaH. W. SobelM. KabirnezhadShigeki AokiY. FukudaL. PickardD. DewhurstZ. J. LiptakA. D. MarinoK. SakashitaPaoloneKendall MahnL. SouthwellH. K. TanakaS. M. OserA. BravarA. J. FinchJ. MyslikJ. M. PoutissouC. BronnerM. G. CatanesiM. Posiadala-zezulaYuichi OyamaT. GolanS. SuvorovR. P. LitchfieldM. LicciardiE. RondioMagdalena MalekM. YamamotoB. QuilainN. MccauleyYuki FujiiC. M. NantaisP. JonssonGareth J. BarkerKoji YamamotoK. KowalikHadleyR. TerriK. HuangP. MartinsAsher KabothN. ChikumaLeïla HaegelMarco LavederA. KonakaMichal DziewieckiY. SeiyaJ. P. ColemanO. V. MineevP. PrzewlockiP. LasorakP. P. KollerDavid A. WarkT. HayashinoM. BatkiewiczA. DabrowskaJ. DumarchezJ. HoleczekJ. SchwehrT. RadermacherF. ShakerS. BolognesiC. ChecchiaR. ShahM. A. M. RaynerM. AntonovaDavide SgalabernaMb AvanziniT. OkusawaD. HansenThomas B. CampbellK. NakayoshiG. De RosaR. A. OwenYusuke KoshioGalymovN. D. PatelR. L. HelmerPalladinoS. DolanT. LindnerD. CoploweC. DenshamYusuke SudaC. VilelaA. CuddE. MazzucatoT. DealtryK. E. DuffyEsp GuerraA. MissertJ. ImberM. MezzettoXiao-yan LiM. MiuraC. WretT. YuanA. KorzenevJ. MorrisonM. ZiembickiA. PritchardP. PaudyalL. L. KormosJ. P. LopezB. JamiesonJ. ZalipskaJ. InslerS. L. CartwrightK. S. McfarlandBerardiM. TzanovC. J. MetelkoD. TerhorstD. BrailsfordR. PoutissouP. Bartet-friburgA. RedijJ. Y. KimM. RavonelS. BienstockJ. AmeyY. AshidaG. VasseurG. ChristodoulouY. NakanishiK. NakamuraK. IwamotoKenichi YoshidaC. NielsenS. MoriyamaMasayuki NakahataY. UchidaA. LonghinT. KogaZ. VallariW. Y. MaH. J. KimL. F. ThompsonC. RiccioE. D. ZimmermanM. PavinM. HoganJan KisielT. KobayashiSy SuzukiA. C. WeberSteven C. JohnsonS. NakayamaR. A. WendellS. YenG. CollazuolMark ScottB. A. PopovS. Emery-schrenkKate ScholbergMatveevA. K. IchikawaP. StowellS. MineS. RothJ. KamedaTh. A. MuellerP. MijakowskiA. KnightM. LamoureuxH. M. O'keeffeS. ShortM. O. WasckoT. TsukamotoJ. ZmudaC. PistilloY. NishimuraL. PickeringJ. SteinmannT. IshidaM. NirkkoE. Reinherz-aronisT. OvsyannikovaC. BarryC. YanagisawaYoshihiro SuzukiB. RossiT. VladisavljevicE. ScantamburloR.p. KurjataT. WachalaT. IshiiSeiko HirotaM. GoninF. HosomiM. B. SmyW. OryszczakD. CherdackK. AbeA. ZalewskaC. McgrewL. KochY. HayatoC. AndreopoulosC. AndreopoulosA. HillairetArtur F. IzmaylovS. BanA. KnoxF. Di LodovicoT. SekiguchiM. TadaD. J. PayneM. SorelYu. G. KudenkoN. C. HastingsKeigo NakamuraI. LamontL. MagalettiC. GigantiJ. A. NowakE. IwaiA. ChappellPatrick Dunnesubject
PhysicsNuclear physicsParticle physicsMuon010308 nuclear & particles physics0103 physical sciencesT2K experimentMuon neutrinoNeutrino010306 general physicsNeutrino oscillation7. Clean energy01 natural sciencesdescription
We report measurements by the T2K experiment of the parameters $\theta_{23}$ and $\Delta m^{2}_{32}$ governing the disappearance of muon neutrinos and antineutrinos in the three flavor neutrino oscillation model. Utilizing the ability of the experiment to run with either a mainly neutrino or a mainly antineutrino beam, the parameters are measured separately for neutrinos and antineutrinos. Using $7.482 \times 10^{20}$ POT in neutrino running mode and $7.471 \times 10^{20}$ POT in antineutrino mode, T2K obtained, $\sin^{2}(\theta_{23})=0.51^{+0.08}_{-0.07}$ and $\Delta m^{2}_{32} = 2.53^{+0.15}_{-0.13} \times 10^{-3}$eV$^{2}$/c$^{4}$ for neutrinos, and $\sin^{2}({\overline{\theta}}_{23})=0.42^{+0.25}_{-0.07}$ and ${\Delta\overline{m}^2}_{32} = 2.55^{+0.33}_{-0.27} \times 10^{-3}$eV$^{2}$/c$^{4}$ for antineutrinos (assuming normal mass ordering). No significant differences between the values of the parameters describing the disappearance of muon neutrinos and antineutrinos were observed.
year | journal | country | edition | language |
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2017-07-31 | Physical Review D |