6533b7d9fe1ef96bd126d51d
RESEARCH PRODUCT
Measurements of ν̅ μ and ν̅ μ + ν μ charged-current cross-sections without detected pions or protons on water and hydrocarbon at a mean anti-neutrino energy of 0.86 GeV
M. BarbiT. VladisavljevicA. LonghinA. ShaykinaM. LaweMichelangelo PariA. BlanchetThorsten LuxY. SonodaL. Molina BuenoT. KikawaS. ParsaV. Q. NguyenH. W. SobelH. W. SobelM. GoninJ. XiaA. T. SuzukiA. DergachevaC. E. R. NasebyJ. F. MartinN. KukitaM. LicciardiT. FeuselsT. FeuselsY. TaniharaC. AltT. NakadairaShuji TanakaR. ShahR. ShahJ. LagodaR. J. WilsonM. PavinS. J. JenkinsJ. R. WilsonD. FukudaL. O'sullivanJochen SteinmannXianguo LuM. R. VaginsM. R. VaginsH. KikutaniJ. G. WalshA. BubakP. JonssonR. A. OwenP. NovellaK. IwamotoK. NiewczasAndré RubbiaJaroslaw PasternakY. YoshimotoM. Batkiewicz-kwasniakM. MiuraMarco LavederA. ZykovaJ. P. ColemanT. HayashinoYuto AshidaA. J. FinchR. FukudaC. WretA. KnoxT. AriharaT. SekiguchiR. AkutsuJ. MorrisonN. MccauleyM. GuigueA. PritchardP. B. JurjA. A. SztucJ. L. PalominoG. ZarneckiPatrick DunneP. PaudyalA. BlondelA. BlondelT. KogaB. A. PopovT. HonjoA. RychterP. Hamacher-baumannOleg MineevC. PistilloM. JakkapuM. Buizza AvanziniB. JamiesonG. ChristodoulouK. NakamuraK. NakamuraT. A. DoyleE. Reinherz-aronisKeigo NakamuraTakaaki KajitaE. RondioB. QuilainC. J. DenshamK. YasutomeK. FusshoellerHiroyuki SekiyaHiroyuki SekiyaS. L. CartwrightF. ShakerW. UnoC. M. NantaisF. NovaK. PorwitP. F. DennerR. FujitaY. FukudaKendall MahnA. K. IchikawaV. PaoloneAkitaka ArigaKo OkumuraKo OkumuraG. PintaudiS. MoriyamaKate ScholbergKate ScholbergD. CherdackM. ZiembickiS. RothJ. KamedaJ. ZalipskaC. VilelaS. KuribayashiE. S. Pinzon GuerraTh. A. MuellerB. RadicsM. IkedaA. ZalewskaFederico SanchezB. BourguilleYousuke KataokaZ. VallariY. TakeuchiY. TakeuchiK. WoodR.p. KurjataL. F. ThompsonS. ValderT. OgawaT. GolanM. HartzM. HartzE. D. ZimmermanC. McgrewMasayuki NakahataMasayuki NakahataC. PidcottL. KochY. AsadaA. GorinG. A. FiorentiniA. KnightA. ShvartsmanN. TeshimaC. ChecchiaA. BravarVladimir VolkovY. UchidaShigeki AokiYuichi OyamaA. NakamuraS. SuvorovS. SuvorovR. P. LitchfieldTakatomi YanoY. HayatoY. HayatoC. AndreopoulosC. AndreopoulosR. A. WendellR. A. WendellS. BolognesiH. M. O'keeffeJ. HoleczekS. HassaniG. FiorilloT. RadermacherThomas B. CampbellYuki FujiiK. NakayoshiD. Bravo BerguñoE. RadicioniT. KobataW. H. TokiHiromasa TanakaHiromasa TanakaV. A. MatveevM. B. SmyT. TowstegoL. MaretP. N. RatoffT. KutterKoji YamamotoM. MccarthyM. ZitoHidekazu KakunoPablo FernandezM. O. WasckoS. MineG. YangE. MazzucatoK. KowalikLaura Gutermuth AnthonyM. YuD. L. WarkD. L. WarkF. Di LodovicoYutaka NakajimaJan KisielT. BonusM. FriendTeppei KatoriYanbin WangM. TadaD. J. PayneK. AbeT. OkusawaJungsang KimJungsang KimS. Y. SuzukiN. IzumiD. VargasJ. DumarchezN. ChikumaVincenzo BerardiD. BarrowEtam NoahC. BronnerSteven C. JohnsonS. NakayamaS. NakayamaF. J. P. SolerL. L. KormosW. ShorrockMasaki IshitsukaYoshihiro SuzukiM. KuzeT. TsukamotoK. SkwarczynskiL. LabargaA. EguchiK. SakashitaS. M. OserS. M. OserL. BernsS. YenM. HoganT. KobayashiN. C. HastingsM. AntonovaR. OkadaT. OdagawaYoshikazu YamadaYoshikazu YamadaA. N. KhotjantsevAlan Cosimo RuggeriJ. SchwehrD. KarlenD. KarlenT. YoshidaY. SeiyaA. MinaminoHidetoshi KuboA. D. MarinoHyun-chul KimA. IzmaylovL. PickeringY. NishimuraS. ManlyS. BanS. BienstockK. M. TsuiK. S. McfarlandF. BenchA. C. WeberA. C. WeberY. KatayamaG. VasseurC. Jesús-vallsC. RugglesG. SantucciO. DrapierD. A. HarrisS. Emery-schrenkH. K. TanakaT. WachalaT. IshidaS. P. KasettiN. AkhlaqM. M. KhabibullinS. L. LiuM. Posiadala-zezulaM. G. CatanesiM. MalekL. MagalettiC. GigantiN. DokaniaS. BerkmanS. BerkmanRoberto SpinaA. C. KabothA. C. KabothA. CerveraG. CollazuolMark ScottM. KabirnezhadK. MavrokoridisJ. A. NowakA. ChappellLars EklundT. S. NonnenmacherC. BarryS. MurphyC. RiccioC. MaugerT. DealtryE. T. AtkinM. CicerchiaAlexei Yu. SmirnovYuta KatoK. NishikawaM. LamoureuxL. N. MachadoJ. T. HaighS. ZsoldosV. PalladinoS. B. BoydL. Marti-magroL. Marti-magroK. ZarembaJan T. SobczykStephanie BronAtsushi TakedaJ. McelweeD. SgalabernaAhmed AliC. FrancoisY. AwataguchiXiao-yan LiW. G. S. VinningC. WilkinsonT. V. NgocC. YanagisawaC. YanagisawaGareth J. BarkerYuuki NakanoD. CoploweT. IshiiA. HiramotoT. HasegawaTakahiko MatsubaraS. V. CaoC. TouramanisM. J. WilkingM. JiangAntonio EreditatoN. YershovT. MaruyamaK. GameilK. GameilJ. C. NugentG.d. BarrS. KingF. IacobM. MezzettoD. R. HadleyY. NagaiW. C. ParkerM. TaniE. KearnsE. KearnsG. C. PennMasashi YokoyamaM. TzanovC. J. MetelkoYu.a. KudenkoYu.a. KudenkoA. DabrowskaK. MatsushitaD. BrailsfordN. T. Hong VanJ. WalkerA. MefodievS. DolanT. LindnerA. CuddS. R. DennisTsuyoshi NakayaTsuyoshi NakayaC. M. SchloesserC. K. JungC. K. JungMasato ShiozawaMasato ShiozawaL. LudoviciA. KostinS. BhadraL. CookL. CookA. BeloshapkinG. De RosaJ. CalcuttA. ShaikhievA. KonakaL. MunteanuM. TajimaYusuke KoshioYusuke Koshiosubject
chemistry.chemical_classificationPhysicsParticle physicsMuonProton010308 nuclear & particles physicsGeneral Physics and Astronomy01 natural sciencesHydrocarbonPionchemistry0103 physical sciences010306 general physicsNucleonEnergy (signal processing)Charged currentBar (unit)description
Abstract We report measurements of the flux-integrated ν̅μ and ν̅μ + νμ charged-current cross-sections on water and hydrocarbon targets using the T2K anti-neutrino beam with a mean beam energy of 0.86 GeV. The signal is defined as the (anti-)neutrino charged-current interaction with one induced $\mu^\pm$ and no detected charged pion or proton. These measurements are performed using a new WAGASCI module recently added to the T2K setup in combination with the INGRID Proton Module. The phase space of muons is restricted to the high-detection efficiency region, $p_{\mu}>400~{\rm MeV}/c$ and $\theta_{\mu}<30^{\circ}$, in the laboratory frame. An absence of pions and protons in the detectable phase spaces of $p_{\pi}>200~{\rm MeV}/c$, $\theta_{\pi}<70^{\circ}$ and $p_{\rm p}>600~{\rm MeV}/c$, $\theta_{\rm p}<70^{\circ}$ is required. In this paper, both the $\overline{\nu}_\mu$ cross-sections and $\overline{\nu}_\mu+\nu_\mu$ cross-sections on water and hydrocarbon targets and their ratios are provided by using the D’Agostini unfolding method. The results of the integrated $\overline{\nu}_\mu$ cross-section measurements over this phase space are $\sigma_{\rm H_{2}O}=(1.082\pm0.068(\rm stat.)^{+0.145}_{-0.128}(\rm syst.)) \times 10^{-39}\,{\rm cm^{2} / nucleon}$, $\sigma_{\rm CH}=(1.096\pm0.054(\rm stat.)^{+0.132}_{-0.117}(\rm syst.)) \times 10^{-39}\,{\rm cm^{2} / nucleon}$, and $\sigma_{\rm H_{2}O}/\sigma_{\rm CH} = 0.987\pm0.078(\rm stat.)^{+0.093}_{-0.090}(\rm syst.)$. The $\overline{\nu}_\mu+\nu_\mu$ cross-section is $\sigma_{\rm H_{2}O} = (1.155\pm0.064(\rm stat.)^{+0.148}_{-0.129}(\rm syst.)) \times 10^{-39}\,{\rm cm^{2} / nucleon}$, $\sigma_{\rm CH}=(1.159\pm0.049(\rm stat.)^{+0.129}_{-0.115}(\rm syst.)) \times 10^{-39}\,{\rm cm^{2} / nucleon}$, and $\sigma_{\rm H_{2}O}/\sigma_{\rm CH}=0.996\pm0.069(\rm stat.)^{+0.083}_{-0.078}(\rm syst.)$.
year | journal | country | edition | language |
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2021-03-02 | Progress of Theoretical and Experimental Physics |