6533b862fe1ef96bd12c6081
RESEARCH PRODUCT
Search for theZ(4430)−atBABAR
B. AubertM. BonaY. KaryotakisJ. P. LeesV. PoireauE. PrencipeX. PrudentV. TisserandJ. Garra TicoE. GraugesL. LopezA. PalanoM. PappagalloG. EigenB. StuguL. SunG. S. AbramsM. BattagliaD. N. BrownR. N. CahnR. G. JacobsenL. T. KerthYu. G. KolomenskyG. LynchI. L. OsipenkovM. T. RonanK. TackmannT. TanabeC. M. HawkesN. SoniA. T. WatsonH. KochT. SchroederD. WalkerD. J. AsgeirssonB. G. FulsomC. HeartyT. S. MattisonJ. A. MckennaM. BarrettA. KhanV. E. BlinovA. D. BukinA. R. BuzykaevV. 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. BuchananH. AtmacanJ. W. GaryF. LiuO. LongG. M. VitugZ. YasinL. ZhangV. SharmaC. CampagnariT. M. HongD. KovalskyiM. A. MazurJ. D. RichmanT. W. BeckA. M. EisnerC. J. FlaccoC. A. HeuschJ. KrosebergW. S. LockmanA. J. MartinezT. SchalkB. A. SchummA. SeidenM. G. WilsonL. O. WinstromC. H. ChengD. A. DollB. EchenardF. 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PhysicsNuclear and High Energy PhysicsParticle physicsMass distribution010308 nuclear & particles physicsElectron–positron annihilation01 natural scienceslaw.inventionLuminosityNuclear physicsScattering amplitudeReflection (mathematics)law0103 physical sciencesZ(4430)010306 general physicsColliderLegendre polynomialsdescription
We report the results of a search for Z(4430)^- decay to J/Ψ π^- or Ψ(2S)π^- in B(^-.0)→ J/Ψ π^-K^(0.+) and B^(-.0) → Ψ(2S)π^-K^(0.+) decays. The data were collected with the BABAR detector at the SLAC PEP-II asymmetric-energy e^+e^- collider operating at center-of-mass energy 10.58 GeV, and the sample corresponds to an integrated luminosity of 413 fb^(-1). Each K π^- mass distribution exhibits clear K^*(892) and K_2^*(1430) signals, and the efficiency-corrected spectrum is well described by a superposition of the associated Breit-Wigner intensity distributions, together with an S-wave contribution obtained from the LASS I=1/2 K π^- scattering amplitude measurements. Each K π^- angular distribution varies significantly in structure with K π^- mass, and is represented in terms of low-order Legendre polynomial moments. We find that each J/Ψ π^- or Ψ (2S)π^- mass distribution is well described by the reflection of the measured K π^- mass and angular distribution structures. We see no significant evidence for a Z(4430)^- signal for any of the processes investigated, neither in the total J/Ψ π^- or Ψ(2S) π^- mass distribution, nor in the corresponding distributions for the regions of K π- mass for which observation of the Z(4430)^- signal was reported. We obtain branching-fraction upper limits [script B](B^- → Z^-[overline K]^0,Z^- → J/Ψ π^-)<1.5×10^(-5), [script B](B^0 → Z^-K^+,Z^- → J/Ψ π^-)<0.4×10^(-5), [script B](B → Z-[overline K]0,Z → Ψ(2S)π-)<4.7×10-5, and [script B](B^0 → Z^-K^+,Z^- → Ψ(2S)π^-)<3.1×10^(-5) at 95% confidence level, where the Z(4430)- mass and width have been fixed to the reported central values
year | journal | country | edition | language |
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2009-06-01 | Physical Review D |