Abstract

We report the results of a search for Z(4430)−Z(4430)^- decay to J/ψπ−J/ψπ^- or ψ(2S)π−ψ(2S)π^- in $B^{-,0}\to \jpsiπ^- K^{0,+}$ and $B^{-,0}\to \psitwos π^- K^{0,+}$ decays. The data were collected with the BABAR detector at the SLAC PEP-II asymmetric-energy e+e−e^+e^- collider operating at center of mass energy 10.58 \gev, and the sample corresponds to an integrated luminosity of 413 fb−1^{-1}. Each KπKπ mass distribution exhibits clear K∗(892)K^{\ast}(892) and K2∗(1430)K^{\ast}_2(1430) signals, and the efficiency-corrected spectrum is well-described by a superposition of the associated Breit-Wigner intensity distributions, together with an SS-wave contribution obtained from the LASS I=1/2I=1/2 KπKπ scattering amplitude measurements. Each KπKπ angular distribution varies significantly in structure with KπKπ mass, and is represented in terms of low-order Legendre polynomial moments. We find that each J/ψπJ/ψπ or ψ(2S)πψ(2S)π mass distribution is well-described by the reflection of the measured KπKπ mass and angular distribution structures. We see no significant evidence for a Z(4430)−Z(4430)^- signal for any of the processes investigated, neither in the total J/ψπJ/ψπ or ψ(2S)πψ(2S)π mass distribution, nor in the corresponding distributions for the regions of KπKπ mass for which observation of the Z(4430)−Z(4430)^- signal was reported. We obtain branching fraction upper limits B(B−→Z−K0ˉ,Z−→J/ψπ−)<1.5×10−5{\cal{B}}(B^-\to Z^-\bar{K^0}, Z^-\to J/ψπ^-)<1.5\times 10^{-5}, B(B0→Z−K+,Z−→J/ψπ−)<0.4×10−5{\cal{B}}(B^0\to Z^-K^+, Z^-\to J/ψπ^-)<0.4\times 10^{-5}, B(B−→Z−K0ˉ,Z−→ψ(2S)π−)<4.7×10−5{\cal{B}}(B^-\to Z^-\bar{K^0}, Z^-\to ψ(2S)π^-)<4.7\times 10^{-5}, and B(B0→Z−K+,Z−→ψ(2S)π−)<3.1×10−5{\cal{B}}(B^0\to Z^-K^+, Z^-\to ψ(2S)π^-)<3.1\times 10^{-5} at 95% confidence level, where the Z(4430)−Z(4430)^- mass and width have been fixed to the reported central values.

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