Search for the decay Bs0→ηηB_s^0\rightarrowηη

preprint2021arXivOpen access
Belle CollaborationB. BhuyanK. J. NathJ. BorahI. AdachiH. AiharaS. Al SaidD. M. AsnerH. AtmacanV. AulchenkoT. AushevR. AyadV. BabuI. BadhreesA. M. BakichP. BeheraJ. BennettV. BhardwajT. BilkaJ. BiswalA. BobrovA. BozekM. BračkoT. E. BrowderM. CampajolaD. ČervenkovV. ChekelianA. ChenB. G. CheonK. ChilikinK. ChoS. -K. ChoiY. ChoiS. ChoudhuryD. CinabroS. CunliffeN. DashF. Di CapuaS. Di CarloZ. DoležalT. V. DongS. DubeyS. EidelmanJ. E. FastT. FerberB. G. FulsomV. GaurN. GabyshevA. GarmashA. GiriP. GoldenzweigB. GolobJ. HabaT. HaraO. HartbrichK. HayasakaH. HayashiiW. -S. HouT. IijimaK. InamiG. IngugliaA. IshikawaR. ItohM. IwasakiY. IwasakiW. W. JacobsS. JiaY. JinD. JoffeK. K. JooA. B. KaliyarK. H. KangG. KaryanT. KawasakiH. KichimiC. KieslingD. Y. KimH. J. KimK. T. KimS. H. KimK. KinoshitaP. KodyšS. KorparD. KotchetkovP. KrižanR. KroegerP. KrokovnyR. KumarA. KuzminY. -J. KwonJ. S. LangeJ. K. LeeJ. Y. LeeS. C. LeeC. H. LiL. K. LiY. B. LiL. Li GioiJ. LibbyK. LieretD. LiventsevP. -C. LuT. LuoJ. MacNaughtonC. MacQueenM. MasudaD. MatvienkoM. MerolaK. MiyabayashiH. MiyataR. MizukG. B. MohantyT. MoriR. MussaT. NakanoM. NakaoM. NayakM. NiiyamaN. K. NisarS. NishidaK. OgawaS. OgawaH. OnoY. OnukiP. PakhlovG. PakhlovaB. PalT. PangS. PardiH. ParkS. PatraS. PaulT. K. PedlarR. PestotnikL. E. PiilonenV. PopovE. PrencipeM. RitterA. RostomyanG. RussoY. SakaiM. SalehiS. SandilyaL. SanteljT. SanukiV. SavinovO. SchneiderG. SchnellJ. SchuelerC. SchwandaY. SeinoK. SenyoM. E. SeviorV. ShebalinC. P. ShenJ. -G. ShiuE. SolovievaM. StaričT. SumiyoshiW. SutcliffeM. TakizawaU. TamponiK. TanidaF. TenchiniK. TrabelsiM. UchidaT. UglovY. UnnoS. UnoP. UrquijoY. UsovS. E. VahsenR. van TonderG. VarnerA. VossenC. H. WangM. -Z. WangP. WangJ. WiechczynskiE. WonS. B. YangH. YeJ. H. YinY. YusaZ. P. ZhangV. ZhilichV. Zhukova

Abstract

We report results from a search for the decay Bs0→ηηB_s^0\rightarrowηη using 121.4 fb−1^{-1} of data collected at the Υ(5S)Υ(5S) resonance with the Belle detector at the KEKB asymmetric-energy e+e−e^+e^- collider. We do not observe any signal and set an upper limit on the branching fraction of 14.3×10−514.3\times 10^{-5} at 90%90\% confidence level. This result represents a significant improvement over the previous most stringent limit.

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