First Measurement of the Λc+→pη′Λ_c^+ \to p η' decay

preprint2022arXivOpen access
Belle CollaborationS. X. LiJ. X. CuiC. P. ShenI. AdachiH. AiharaS. Al SaidD. M. AsnerH. AtmacanT. AushevR. AyadV. BabuP. BeheraK. BelousM. BessnerV. BhardwajB. BhuyanT. BilkaD. BodrovG. BonviciniJ. BorahA. BozekM. BrackoP. BranchiniT. E. BrowderA. BudanoM. CampajolaD. CervenkovM. -C. ChangP. ChangV. ChekelianA. ChenB. G. CheonK. ChilikinH. E. ChoK. ChoS. -J. ChoS. -K. ChoiY. ChoiS. ChoudhuryD. CinabroS. CunliffeS. DasN. DashG. De NardoG. De PietroR. DhamijaF. Di CapuaZ. DolezalT. V. DongD. EpifanovT. FerberD. FerlewiczB. G. FulsomR. GargV. GaurN. GabyshevA. GiriP. GoldenzweigB. GolobE. GrazianiT. GuT. HaraK. HayasakaH. HayashiiW. -S. HouK. InamiA. IshikawaM. IwasakiY. IwasakiW. W. JacobsE. -J. JangS. JiaY. JinK. K. JooJ. KahnA. B. KaliyarK. H. KangY. KatoT. KawasakiH. KichimiC. KieslingC. H. KimD. Y. KimY. -K. KimK. KinoshitaP. KodysT. KonnoA. KorobovS. KorparE. KovalenkoP. KrizanR. KroegerP. KrokovnyM. KumarR. KumarK. KumaraY. -J. KwonT. LamM. LaurenzaS. C. LeeJ. LiL. K. LiY. LiL. Li GioiJ. LibbyD. LiventsevA. MartiniM. MasudaT. MatsudaD. MatvienkoS. K. MauryaF. MeierM. MerolaK. MiyabayashiR. MizukR. MussaM. NakaoD. NarwalZ. NatkaniecA. NatochiiL. NayakN. K. NisarS. NishidaK. NishimuraK. OgawaS. OgawaH. OnoP. OskinP. PakhlovG. PakhlovaT. PangS. PardiS. -H. ParkS. PatraT. K. PedlarR. PestotnikL. E. PiilonenT. PodobnikV. PopovM. T. PrimM. RohrkenA. RostomyanN. RoutG. RussoD. SahooS. SandilyaA. SangalT. SanukiV. SavinovG. SchnellJ. SchuelerC. SchwandaA. J. SchwartzY. SeinoK. SenyoM. E. SeviorM. ShapkinC. SharmaV. ShebalinJ. -G. ShiuB. ShwartzF. SimonE. SolovievaS. StanicM. StaricZ. S. StottlerM. SumihamaK. SumisawaT. SumiyoshiW. SutcliffeM. TakizawaU. TamponiK. TanidaF. TenchiniK. TrabelsiM. UchidaY. UnnoK. UnoS. UnoP. UrquijoS. E. VahsenR. van TonderG. VarnerA. VinokurovaE. WaheedD. WangE. WangM. -Z. WangS. WatanukiE. WonX. XuB. D. YabsleyW. YanH. YeJ. H. YinY. YusaY. ZhaiV. ZhilichV. Zhukova

Abstract

We present the first measurement of the branching fraction of the singly Cabibbo-suppressed (SCS) decay Λc+→pη′Λ_c^+ \to p η' with η′→ηπ+π−η' \to ηπ^+π^-, using a data sample corresponding to an integrated luminosity of 981 fb−1\rm fb^{-1}, collected by the Belle detector at the KEKB e+e^{+}e−e^{-} asymmetric-energy collider. A significant Λc+Λ_c^+ signal is observed for the first time with a signal significance of 5.4σσ. The relative branching fraction with respect to the normalization mode Λc+→pK−π+Λ_c^+ \to pK^-π^+ is measured to be \begin{equation*} \frac{{\cal B}(Λ_c^+ \to p η')}{{\cal B}(Λ_c^+ \to p K^-π^+)} = (7.54 \pm 1.32 \pm 0.75) \times 10^{-3}, \end{equation*} where the uncertainties are statistical and systematic, respectively. Using the world-average value of B(Λc+→pK−π+)=(6.28±0.32)×10−2{\cal B}(Λ_c^+ \to p K^-π^+) = (6.28\pm0.32)\times10^{-2}, we obtain \begin{equation*} {\cal B}(Λ_c^+ \to p η') = (4.73 \pm 0.82 \pm 0.47 \pm 0.24)\times 10^{-4}, \end{equation*} where the uncertainties are statistical, systematic, and from B(Λc+→pK−π+){\cal B}(Λ_c^+ \to pK^-π^+), respectively.

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