Study of B‾0→D+h−(h=K/π)\overline{B}{}^0\rightarrow D^{+}h^{-} (h=K/π) decays at Belle

preprint2022arXivOpen access
Belle CollaborationE. WaheedP. UrquijoI. AdachiH. AiharaS. Al SaidD. M. AsnerH. AtmacanV. AulchenkoT. AushevS. BahinipatiP. BeheraK. BelousJ. BennettM. BessnerV. BhardwajB. BhuyanT. BilkaJ. BiswalA. BobrovD. BodrovJ. BorahA. BozekM. BrackoP. BranchiniT. E. BrowderA. BudanoM. CampajolaD. CervenkovM. -C. ChangP. ChangA. ChenB. G. CheonK. ChilikinH. E. ChoK. ChoS. -J. ChoS. -K. ChoiY. ChoiS. ChoudhuryD. CinabroS. CunliffeS. DasG. De NardoG. De PietroR. DhamijaF. Di CapuaZ. DolezalT. V. DongD. EpifanovT. FerberD. FerlewiczB. G. FulsomR. GargV. GaurN. GabyshevA. GiriP. GoldenzweigB. GolobE. GrazianiT. GuY. GuanK. GudkovaC. HadjivasiliouS. HalderO. HartbrichK. HayasakaH. HayashiiW. -S. HouC. -L. HsuT. IijimaK. InamiA. IshikawaR. ItohM. IwasakiY. IwasakiW. W. JacobsS. JiaY. JinK. K. JooA. B. KaliyarK. H. KangH. KichimiC. H. KimD. Y. KimK. -H. KimK. T. KimY. -K. KimK. KinoshitaP. KodysT. KonnoA. KorobovS. KorparE. KovalenkoP. KrizanR. KroegerP. KrokovnyM. KumarR. KumarK. KumaraY. -J. KwonY. -T. LaiJ. S. LangeM. LaurenzaS. C. LeeJ. LiL. K. LiY. B. LiL. Li GioiJ. LibbyK. LieretD. LiventsevC. MacQueenM. MasudaT. MatsudaM. MerolaF. MetznerK. MiyabayashiR. MizukG. B. MohantyR. MussaM. NakaoA. NatochiiL. NayakM. NayakM. NiiyamaN. K. NisarS. NishidaS. OgawaH. OnoP. OskinP. PakhlovG. PakhlovaT. PangH. ParkS. -H. ParkA. PasseriS. PatraS. PaulT. K. PedlarR. PestotnikL. E. PiilonenT. PodobnikV. PopovE. PrencipeM. T. PrimM. RohrkenA. RostomyanN. RoutG. RussoD. SahooS. SandilyaL. SanteljT. SanukiV. SavinovG. SchnellC. SchwandaA. J. SchwartzY. SeinoK. SenyoM. E. SeviorM. ShapkinC. SharmaC. P. ShenJ. -G. ShiuF. SimonJ. B. SinghA. SokolovE. SolovievaM. StaricZ. S. StottlerJ. F. StrubeM. SumihamaT. SumiyoshiW. SutcliffeM. TakizawaU. TamponiK. TanidaF. TenchiniK. TrabelsiM. UchidaT. UglovY. UnnoK. UnoS. UnoY. UsovS. E. VahsenR. van TonderG. VarnerK. E. VarvellA. VinokurovaC. H. WangE. WangM. -Z. WangP. WangX. L. WangJ. WiechczynskiE. WonB. D. YabsleyW. YanS. B. YangH. YeJ. YeltonJ. H. YinY. YusaZ. P. ZhangV. ZhilichV. Zhukova

Abstract

We present a measurement of the branching fractions of the Cabibbo favored B‾0→D+π−\overline{B}{}^0\rightarrow D^{+}π^{-} and the Cabibbo suppressed B‾0→D+K−\overline{B}{}^0\rightarrow D^{+}K^{-} decays. We find B(B‾0→D+π−)=(2.48±0.01±0.09±0.04)×10−3\mathcal{B}(\overline{B}{}^0\rightarrow D^{+}π^{-}) = (2.48 \pm 0.01 \pm 0.09 \pm 0.04) \times 10^{-3} and B(B‾0→D+K−)=(2.03±0.05±0.07±0.03)×10−4\mathcal{B}(\overline{B}{}^0\rightarrow D^{+}K^{-})= (2.03 \pm 0.05 \pm 0.07 \pm 0.03) \times 10^{-4} decays, where the first uncertainty is statistical, the second is systematic, and the third uncertainty is due to the D+→K−π+π+D^{+} \rightarrow K^{-}π^{+}π^{+} branching fraction. The ratio of branching fractions of B‾0→D+K−\overline{B}{}^0\rightarrow D^{+}K^{-} and B‾0→D+π−\overline{B}{}^0\rightarrow D^{+}π^{-} is measured to be RD=[8.19±0.20(stat)±0.23(syst)]×10−2R^{D} = [8.19 \pm 0.20(\rm stat) \pm 0.23(\rm syst)] \times 10^{-2} . These measurements are performed using the full Belle data set, which corresponds to 772×106BB‾772 \times 10^{6} B\overline{B} pairs.

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