6533b833fe1ef96bd129b6dc
RESEARCH PRODUCT
Thee+e−→2(π+π−)π0,2(π+π−)η,K+K−π+π−π0andK+K−π+π−ηcross sections measured with initial-state radiation
B. AubertM. BonaD. BoutignyY. KaryotakisJ. P. LeesV. PoireauX. PrudentV. TisserandA. ZghicheJ. Garra TicoE. GraugesL. LopezA. PalanoM. PappagalloG. EigenB. StuguL. SunG. S. AbramsM. BattagliaD. N. BrownJ. Button-shaferR. N. CahnY. GroysmanR. G. JacobsenJ. A. KadykL. T. KerthYu. G. KolomenskyG. KukartsevD. Lopes PegnaG. LynchL. M. MirT. J. OrimotoI. L. OsipenkovM. T. RonanK. TackmannT. TanabeW. A. WenzelP. Del Amo SanchezC. M. HawkesA. T. WatsonH. KochT. SchroederD. WalkerD. J. AsgeirssonT. Cuhadar-donszelmannB. G. FulsomC. HeartyT. S. MattisonJ. A. MckennaM. BarrettA. KhanM. SaleemL. TeodorescuV. E. BlinovA. D. BukinV. P. DruzhininV. B. GolubevA. P. OnuchinS. I. SerednyakovYu. I. SkovpenE. P. SolodovK. Yu. TodyshevM. BondioliS. CurryI. EschrichD. KirkbyA. J. LankfordP. LundM. MandelkernE. C. MartinD. P. StokerS. AbachiC. BuchananS. D. FoulkesJ. W. GaryF. LiuO. LongB. C. ShenG. M. VitugL. ZhangH. P. PaarS. RahatlouV. SharmaJ. W. BerryhillC. CampagnariA. CunhaB. DahmesT. M. HongD. 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FinocchiaroS. PacettiP. PatteriI. M. PeruzziM. PiccoloM. RamaA. ZalloA. BuzzoR. ContriM. Lo VetereM. M. MacriM. R. MongeS. PassaggioC. PatrignaniE. RobuttiA. SantroniS. TosiK. S. ChaisanguanthumM. MoriiJ. WuR. S. DubitzkyJ. MarksS. SchenkU. UwerD. J. BardP. D. DaunceyR. L. FlackJ. A. NashW. Panduro VazquezM. TibbettsP. K. BeheraX. ChaiM. J. CharlesU. MallikJ. CochranH. B. CrawleyL. DongV. EygesW. T. MeyerS. PrellE. I. RosenbergA. E. RubinY. Y. GaoA. V. GritsanZ. J. GuoC. K. LaeA. G. DenigM. FritschG. SchottN. ArnaudJ. BéquilleuxA. D’orazioM. DavierG. GrosdidierA. HöckerV. LepeltierF. Le DiberderA. M. LutzS. PruvotS. RodierP. RoudeauM. H. SchuneJ. SerranoV. SordiniA. StocchiW. F. WangG. WormserD. J. LangeD. M. WrightI. BinghamJ. P. BurkeC. A. ChavezJ. R. FryE. GabathulerR. GametD. E. HutchcroftD. J. PayneK. C. SchofieldC. TouramanisA. J. BevanK. A. GeorgeF. Di LodovicoR. SaccoG. CowanH. U. FlaecherD. A. HopkinsS. ParamesvaranF. SalvatoreA. C. WrenD. N. BrownC. L. DavisJ. AllisonD. 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F. HarrisonJ. IlicT. E. LathamG. B. MohantyH. R. BandX. ChenS. DasuK. T. FloodJ. J. HollarP. E. KutterY. PanM. PieriniR. PrepostS. L. WuH. Nealsubject
PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionElectron–positron annihilationHadronElectron01 natural sciencesOmegaNuclear physics0103 physical sciencesIntermediate stateHigh Energy Physics::ExperimentInvariant mass010306 general physicsVEPP-2000description
We study the processes $e^+ e^-\to 2(\pi^+\pi^-)\pi^0\gamma$, $2(\pi^+\pi^-)\eta\gamma$, $K^+ K^-\pi^+\pi^-\pi^0\gamma$ and $K^+ K^-\pi^+\pi^-\eta\gamma$ with the hard photon radiated from the initial state. About 20000, 4300, 5500 and 375 fully reconstructed events, respectively, are selected from 232 fb$^{-1}$ of BaBar data. The invariant mass of the hadronic final state defines the effective $e^+ e^-$ center-of-mass energy, so that the obtained cross sections from the threshold to about 5 GeV can be compared with corresponding direct \epem measurements, currently available only for the $\eta\pi^+\pi^-$ and $\omega\pi^+\pi^-$ submodes of the $e^+ e^-\to 2(\pi^+\pi^-)\pi^0$ channel. Studying the structure of these events, we find contributions from a number of intermediate states, and we extract their cross sections where possible. In particular, we isolate the contribution from $e^+ e^-\to\omega(782)\pi^+\pi^-$ and study the $\omega(1420)$ and $\omega(1650)$ resonances. In the charmonium region, we observe the $J/\psi$ in all these final states and several intermediate states, as well as the $\psi(2S)$ in some modes, and we measure the corresponding branching fractions.
year | journal | country | edition | language |
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2007-11-20 | Physical Review D |