Measurement of the νμν_μ CCQE cross section on carbon with the ND280 detector at T2K

preprint2015arXivOpen access
T2K CollaborationK. AbeJ. AdamH. AiharaT. AkiriC. AndreopoulosS. AokiA. ArigaS. AssylbekovD. AutieroM. BarbiG. J. BarkerG. BarrM. BassM. BatkiewiczF. BayV. BerardiB. E. BergerS. BerkmanS. BhadraF. d. M. BlaszczykA. BlondelC. BojechkoS. BolognesiS. BordoniS. B. BoydD. BrailsfordA. BravarC. BronnerN. BuchananR. G. CallandJ. Caravaca RodríguezS. 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 LuiseS. DolanO. 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. JamiesonM. JiangS. 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. KochA. KolacekeA. KonakaL. L. KormosA. KorzenevY. KoshioW. KroppH. KuboY. KudenkoR. KurjataT. KutterJ. LagodaI. 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. SánchezF. SatoE. ScantamburloK. ScholbergS. SchoppmannJ. SchwehrM. ScottY. SeiyaT. SekiguchiH. SekiyaD. SgalabernaR. ShahF. ShakerD. ShawM. 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. WachalaK. 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 Charged-Current Quasi-Elastic (CCQE) interaction, νl+n→l−+pν_{l} + n \rightarrow l^{-} + p, is the dominant CC process at Eν∼1E_ν\sim 1 GeV and contributes to the signal in accelerator-based long-baseline neutrino oscillation experiments operating at intermediate neutrino energies. This paper reports a measurement by the T2K experiment of the νμν_μ CCQE cross section on a carbon target with the off-axis detector based on the observed distribution of muon momentum (pμp_μ) and angle with respect to the incident neutrino beam (θμθ_μ). The flux-integrated CCQE cross section was measured to be (0.83±0.12)×10−38 cm2(0.83 \pm 0.12) \times 10^{-38}\textrm{ cm}^{2} in good agreement with NEUT MC value of 0.88×10−38 cm2{0.88 \times 10^{-38}} \textrm{ cm}^{2}. The energy dependence of the CCQE cross section is also reported. The axial mass, MAQEM_A^{QE}, of the dipole axial form factor was extracted assuming the Smith-Moniz CCQE model with a relativistic Fermi gas nuclear model. Using the absolute (shape-only) pμcosθμp_μcosθ_μ distribution, the effective MAQEM_A^{QE} parameter was measured to be 1.26−0.18+0.21 GeV/c2{1.26^{+0.21}_{-0.18} \textrm{ GeV}/c^{2}} (1.43−0.22+0.28 GeV/c2{1.43^{+0.28}_{-0.22} \textrm{ GeV}/c^{2}}).

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