First Observation of Cabibbo-Suppressed Ξ_c^0 Decays

preprint2013arXivOpen access
Belle CollaborationR. ChistovI. AdachiH. AiharaD. M. AsnerV. AulchenkoT. AushevA. M. BakichA. BalaV. BhardwajB. BhuyanA. BondarG. BonviciniA. BozekM. BračkoJ. BrodzickaT. E. BrowderV. ChekelianA. ChenP. ChenB. G. CheonK. ChilikinI. -S. ChoK. ChoV. ChobanovaY. ChoiD. CinabroM. DanilovZ. DoležalD. DuttaS. EidelmanD. EpifanovH. FarhatJ. E. FastM. FeindtT. FerberA. FreyV. GaurN. GabyshevS. GangulyR. GillardY. M. GohB. GolobJ. HabaT. HaraK. HayasakaH. HayashiiY. HoriiY. HoshiW. -S. HouH. J. HyunT. IijimaA. IshikawaR. ItohY. IwasakiT. JuliusD. H. KahJ. H. KangE. KatoT. KawasakiH. KichimiC. KieslingD. Y. KimH. J. KimJ. B. KimJ. H. KimK. T. KimY. J. KimK. KinoshitaJ. KlucarB. R. KoP. KodyšS. KorparP. KrižanT. KumitaA. KuzminY. -J. KwonJ. S. LangeS. -H. LeeJ. LiY. LiJ. LibbyC. LiuY. LiuD. LiventsevP. LukinD. MatvienkoH. MiyataR. MizukG. B. MohantyA. MollT. MoriN. MuramatsuR. MussaE. NakanoM. NakaoZ. NatkaniecM. NayakE. NedelkovskaC. NgS. NishidaO. NitohS. OgawaS. OkunoS. L. OlsenC. OswaldG. PakhlovaC. W. ParkH. ParkH. K. ParkR. PestotnikM. PetričL. E. PiilonenM. RitterM. RöhrkenA. RostomyanH. SahooT. SaitoK. SakaiY. SakaiS. SandilyaD. SantelL. SanteljT. SanukiV. SavinovO. SchneiderG. SchnellC. SchwandaD. SemmlerK. SenyoO. SeonM. E. SeviorM. ShapkinC. P. ShenT. -A. ShibataJ. -G. ShiuB. ShwartzA. SibidanovF. SimonY. -S. SohnA. SokolovE. SolovievaM. StaričM. StederM. SumihamaT. SumiyoshiU. TamponiK. TanidaG. TatishviliY. TeramotoM. UchidaT. UglovY. UnnoS. UnoP. UrquijoY. UsovS. E. VahsenC. Van HulseP. VanhoeferG. VarnerK. E. VarvellA. VinokurovaM. N. WagnerC. H. WangM. -Z. WangP. WangX. L. WangY. WatanabeK. M. WilliamsE. WonB. D. YabsleyJ. YamaokaY. YamashitaS. YashchenkoY. YookY. YusaZ. P. ZhangV. ZhilichV. ZhulanovA. Zupanc

Abstract

We report the first observation of the Cabibbo-suppressed decays Ξc0→Ξ−K+Ξ_c^0\rightarrow Ξ^- K^+, $Ξ_c^0\raΛK^+ K^-$ and Ξc0→ΛϕΞ_c^0\rightarrow Λϕ, using a data sample of 711 fb−1711\, \mathrm{fb}^{-1} collected at the Υ(4S)Υ(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+e−e^+ e^- collider. We measure the ratios of branching fractions to be $\frac{{\cal B}(Ξ_c^0\ra Ξ^- K^+)}{{\cal B}(Ξ^0_c\raΞ^-π^+)}=(2.75\pm 0.51\pm 0.25)\times 10^{-2}$, $\frac{{\cal B}(Ξ_c^0\raΛK^+ K^-)}{{\cal B}(Ξ_c^0\rightarrowΞ^- π^+)}=(2.86\pm 0.61\pm 0.24)\times 10^{-2}$ and $\frac{{\cal B}(Ξ_c^0\ra Λϕ)}{{\cal B}(Ξ^0_c\raΞ^-π^+)}=(3.43\pm 0.58\pm 0.32)\times 10^{-2}$, where the first uncertainty is statistical and the second is systematic.

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