Combined analysis of Belle and Belle II data to determine the CKM angle ϕ3 ϕ_{3} using B+→D(KS0h−h+)h+B^+ \to D(K_{S}^0 h^- h^+) h^+ decays

preprint2021arXivOpen access
BelleBelle II Collaborations:F. AbudinénL. AggarwalH. AhmedH. AiharaN. AkopovS. Al SaidA. AloisioN. Anh KyH. AtmacanV. AushevR. AyadV. BabuS. BacherS. BaehrS. BahinipatiP. BambadeSw. BanerjeeS. BansalJ. BaudotJ. BeckerP. K. BeheraK. BelousJ. V. BennettF. U. BernlochnerM. BertemesE. BertholetM. BessnerS. BettariniF. BianchiT. BilkaD. BiswasA. BobrovD. BodrovG. BonviciniJ. BorahA. BozekM. BračkoP. BranchiniR. A. BriereT. E. BrowderA. BudanoS. BussinoM. CampajolaL. CaoG. CasarosaC. CecchiP. CheemaV. ChekelianA. ChenB. G. CheonK. ChilikinK. ChirapatpimolH. -E. ChoS. -J. ChoS. -K. ChoiY. ChoiS. ChoudhuryD. CinabroL. CoronaS. CunliffeT. CzankS. DasF. DattolaE. De La Cruz-BureloG. de MarinoS. K. MauryaG. De NardoM. De NuccioG. De PietroR. de SangroM. DestefanisS. DeyA. De Yta-HernandezR. DhamijaA. Di CantoZ. DoležalI. Domínguez JiménezT. V. DongM. DorigoD. DossettS. DubeyG. DujanyM. EliachevitchD. EpifanovP. FeichtingerD. FerlewiczT. FillingerS. FioreA. FodorF. FortiB. G. FulsomA. GabrielliE. GanievM. Garcia-HernandezV. GaurA. GazR. GiordanoA. GiriA. GlazovR. GodangP. GoldenzweigB. GolobW. GradlE. GrazianiD. GreenwaldT. GuY. GuanK. GudkovaJ. GuilliamsC. HadjivasiliouS. HalderT. HaraO. HartbrichK. HayasakaH. HayashiiS. HazraI. Heredia de la CruzA. HershenhornT. HiguchiE. C. HillW. -S. HouC. -L. HsuT. IijimaK. InamiA. IshikawaM. IwasakiW. W. JacobsE. -J. JangY. JinH. JunkerkalefeldA. B. KaliyarK. H. KangR. KarlG. KaryanY. KatoC. KetterC. KieslingC. -H. KimD. Y. KimK. -H. KimY. -K. KimK. KinoshitaP. KodyšT. KogaS. KohaniS. KorparE. KovalenkoT. M. G. KraetzschmarP. KrižanP. KrokovnyT. KuhrJ. KumarM. KumarR. KumarK. KumaraA. KuzminY. -J. KwonS. LacapraraY. -T. LaiC. La LicataL. LanceriJ. S. LangeR. LeboucherS. C. LeeP. LeitlJ. LiS. X. LiL. Li GioiJ. LibbyK. LieretZ. LiptakQ. Y. LiuD. LiventsevS. LongoT. LueckC. LyuM. MaggioraR. MaitiS. MaityR. ManfrediE. ManoniS. MarcelloA. MartiniL. MassaccesiM. MasudaK. MatsuokaD. MatvienkoJ. A. McKennaF. MeierM. MerolaF. MetznerM. MilesiC. MillerK. MiyabayashiR. MizukG. B. MohantyN. Molina-GonzalezH. -G. MoserF. MuellerC. MurphyR. MussaK. R. NakamuraT. NakanoM. NakaoM. NarukiD. NarwalA. NatochiiL. NayakM. NayakG. NazaryanN. K. NisarS. NishidaK. NishimuraY. OnishchukH. OnoP. OskinG. PakhlovaA. PaladinoA. PantaE. PaoloniK. ParhamS. -H. ParkA. PasseriA. PathakS. PatraR. PestotnikL. E. PiilonenT. PodobnikS. PokharelL. PolatC. PrazS. PrellE. PrencipeM. T. PrimH. PurwarA. RabusovP. RadosS. RaizS. ReiterM. RemnevI. Ripp-BaudotG. RizzoL. B. RizzutoS. H. RobertsonM. RöhrkenJ. M. RoneyA. RostomyanN. RoutD. SahooD. A. SandersS. SandilyaL. SanteljY. SatoV. SavinovB. ScavinoG. SchnellJ. SchuelerA. J. SchwartzY. SeinoA. SelceK. SenyoM. E. SeviorM. ShapkinC. SharmaT. ShillingtonB. ShwartzA. SibidanovF. SimonJ. B. SinghA. SofferE. SolovievaS. SpataroB. SpruckS. StefkovaZ. S. StottlerR. StroiliK. SumisawaW. SutcliffeS. Y. SuzukiM. TabataM. TakizawaK. TanidaF. TenchiniR. TiwaryD. TonelliE. TorassaK. TrabelsiM. UchidaI. UedaT. UglovK. UnoS. UnoY. UshirodaS. E. VahsenR. van TonderK. E. VarvellA. VinokurovaL. VitaleH. M. WakelingE. WangM. -Z. WangX. L. WangA. WarburtonS. WatanukiO. WerbyckaC. WesselE. WonB. D. YabsleyW. YanH. YeK. YoshiharaY. YusaL. ZaniY. ZhaiY. ZhangV. ZhilichQ. D. ZhouX. Y. ZhouV. I. Zhukova

Abstract

We present a measurement of the Cabibbo-Kobayashi-Maskawa unitarity triangle angle ϕ3 ϕ_{3} (also known as~γγ) using a model-independent Dalitz plot analysis of \linebreak B+→D(KS0h+h−)h+B^+\to D\left(K_{S}^{0}h^{+}h^{-}\right)h^+, where DD is either a D0D^0 or Dˉ0\bar{D}{}^0 meson and hh is either a ππ or KK. This is the first measurement that simultaneously uses Belle and Belle~II data, combining samples corresponding to integrated luminosities of \SI{711}{fb^{-1}} and \SI{128}{fb^{-1}}, respectively. All data were accumulated from energy-asymmetric e+e−e^+e^- collisions at a centre-of-mass energy corresponding to the mass of the Υ(4S)Υ(4S) resonance. We measure ϕ3=(78.4±11.4±0.5±1.0)∘ϕ_3 = \left(78.4 \pm 11.4 \pm 0.5 \pm 1.0 \right)^{\circ}, where the first uncertainty is statistical, the second is the experimental systematic uncertainty and the third is from the uncertainties on external measurements of the DD-decay strong-phase parameters.

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