Studies of B0 ---> rho+- pi-+ and evidence of B0 ----> rho0 pi0
Kazuo AbeY. ChaoS. KobayashiD. ŽontarD. LiventsevR. KulasiriS. VahsenD. EpifanovS. StaničY. AsanoH. KichimiG. R. MoloneyV. ZhilichY.-J. KwonH. ShibuyaY. MiyabayashiM. AkatsuS. UeharaJ. TanakaS. L. OlsenK. SuzukiD.W. KimSushil KumarT. UglovH. KakunoM. PetersMakoto AsaiM. TanakaY. ChoiT. MoriMegumi ShimoyamaSaburou SaitohS.H. LeeN. KatayamaK. HoshinaH. ParkRichard M. DowdT. SumiyoshiS. OkunoJ. BrodzickaT. IgakiJ. W. NamF. TakasakiB. G. CheonZ.P. ZhangH. MiyakeKōji YoshidaH. IshinoT. TsuboyamaJ. ZhangK.F. ChenAkiko OgawaB. GolobT. IijimaA. IshikawaJ. S. LangeA. J. SchwartzM. IwasakiR. GuoP. K. BeheraA. BożekM. YokoyamaHeyoung YangM. Róz̀anśkaE.M. HeenanA. MatyjaP. PakhlovS. SuzukiK. AbeF. OhnoH. YutaK. HasukoA. GordonR. SeusterJ. LiJ. YashimaC.H. WangK. HaraK. UenoH. HayashiiL. Y. DongA. LimosaniS. UnoY. WatanabeF.J. RongaP. YehY. SakaiJ. HabaT. YamanakaS. KorparS. BanerjeeA. BayP. KrižanK. InamiD. MohapatraS. OgawaG. MajumderM. E. SeviorO. SchneiderD. MarlowT. AushevN. KawamuraN. KentShuji MatsumotoV. SidorovM. SatapathyH. NakazawaK. SumisawaE. WonT. HiguchiL. E. PiilonenF. HandaB. YabsleyS.-W. LinN. TamuraJ. SchümannH. SagawaJ. S. KangW. OstrowiczIlija BizjakN. ParslowN. SoniT. TsukamotoM. BračkoHyunwoo KimZ. NatkaniecK. F. ChenHirofumi FujiiJ. KanekoT. HokuueHsuan‐Cheng HuangK. KinoshitaN. RootM.Z. WangM. TomotoH. YamamotoY. IgarashiI. AdachiG. N. TaylorHiroshi MatsumotoV. EigesK. SenyoK. NeichiH. MiyataC. HagnerR. KaganG. LederY. UnnoH. SakaueK. KorotushenkoJ.G. WangP. ChangR. AbeY. HoshiR. ChistovD. ZürcherM. WatanabeO. TajimaT. OkabeY. YamadaK. TanabeB. TakeshitaY. SettaiT. SarangiV. SiegleK. TakahashiA. KusakaM. IwamotoJ. B. SinghY. MikamiS. EidelmanG. GokhrooC.W. ParkM. DashM. YamauchiY. TamaiS.U. KataokaY. EnariM. NakaoT. MatsuishiI. HiguchiH. AiharaH.J. KimY. BanI. BednyM. StaričT. AsoA. SugiC. SchwandaT. NozakiK. TamaiH. PałkaY. TeramotoY. HsiungT. KawasakiA. SugiyamaM. PernickaM. KataokaRong LüT. MatsubaraJ.-P. PerroudT. E. BrowderN. GabyshevY. UshirodaW.-S. HouA. DrutskoyP. KrokovnyShumpei MoriZhanwen ZhuKoya AbeY. ChoiC.W. EvertonByoung Sup AhnA. SatpathyW. MitaroffL. S. PeakS. NoguchiS. SchrenkS. TokudaC. C. KuoY. NagasakaM. Große PerdekampYasunari HaradaH. GulerT. NagamineA. BondarHideyuki KawaiT. MatsumotoA. TchouvikovK. E. VarvellC.C. ZhangG. S. VarnerE. KuriharaM. IwasakiA. KibayashiKenta UchidaL.C. MoffittO. NitohJ. DragicA. M. BakichS.-K. ChoiH. YanaiT. TomuraT.-A. ShibataK. TrabelsiP. KapustaK. MiyabayashiHeejong KimS. BahinipatiThomas ZieglerY. YusaK. AbeR. ItohL. WidhalmJ.H. KimHyejin JangF. FangY. IwasakiT.H. KimS.Y. SuzukiM. DanilovS. NaritaM.-C. ChangC.C. WangS. K. SwainH. KawaiE. BanaśJ.H. KangY. KawakamiA. KuzminY. YuanE.A. DodsonP. KoppenburgT. SekiL. HinzT. HojoH. SakamotoS.N. ToveyM. HazumiE. NakanoT. LesiakS. NishidaY. ZhengK.S. ParkT. NakadairaB. ShwartzAtsushi YamaguchiY. YamashitaT. HaraH.O. KimA. GarmashS.K. KimN. C. HastingsF. MandlJ. MuellerT. OhshimaG. F. MoorheadJ. MacNaughtonH. OzakiAkira MurakamiS. SemenovY. OnukiT. GershonN. Uozaki
0
Citation
0
Reference
20
Related Paper
Cite
Raspberry Pi
Cite
Citations (0)
Cite
Citations (0)
X(3872)
Cite
Citations (1)
Cite
Citations (0)
Cite
Citations (0)
Cite
Citations (0)
We study the processes e+e−→π+π−π0π0π0γ and π+π−π0π0ηγ in which an energetic photon is radiated from the initial state. The data are collected with the BABAR detector at SLAC. About 14 000 and 4700 events, respectively, are selected from a data sample corresponding to an integrated luminosity of 469 fb−1. The invariant mass of the hadronic final state defines the effective e+e− center-of-mass energy. From the mass spectra, the first precise measurement of the e+e−→π+π−π0π0π0 cross section and the first measurement ever of the e+e−→π+π−π0π0η cross section are performed. The center-of-mass energies range from threshold to 4.35 GeV. The systematic uncertainty is typically between 10% and 13%. The contributions from ωπ0π0, ηπ+π−, and other intermediate states are presented. We observe the J/ψ and ψ(2S) in most of these final states and measure the corresponding branching fractions, many of them for the first time.30 MoreReceived 30 October 2018DOI:https://doi.org/10.1103/PhysRevD.98.112015Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI. Funded by SCOAP3.Published by the American Physical SocietyPhysics Subject Headings (PhySH)Research AreasParticle interactionsParticle productionParticles & Fields
Cite
Citations (28)
Branching (polymer chemistry)
Cite
Citations (0)
Branching (polymer chemistry)
Cite
Citations (0)
We report evidence for the $b\to u$ transition $B^0 \to D_s^{+}π^-$ and the results of a search for $B^0 \to D_s^{*+} π^-$ from a sample of $61.6\times 10^6$ $Y(4S)$ decays into $B$ meson pairs collected with the BaBar detector at the PEP II asymmetric $e^{+}e^{-}$ collider. The observed $B^0 \to D_s^{+} π^-$ yield has a probability of $4.4 \times 10^{-4}$ to be a fluctuation of the background (3.5 $σ$) and we measure the branching fraction $B^0 \to D_s^{+} π^-=3.1 \pm 1.0 ({\rm stat.})\pm 1.0 ({\rm syst.})$. We also set a limit $B^0 \to D_s^{*+} π^-
Branching fraction
B meson
Cite
Citations (0)