Search for the Z ( 4430 ) − at BABAR

We report the results of a search for Z ( 4430 ) − decay to J / ψ π − or ψ ( 2 S ) π − in B − , 0 → J / ψ π − K 0 , + and B − , 0 → ψ ( 2 S ) 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 1...

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Veröffentlicht in:Physical Review D 2009-06, Vol.79 (11), Article 112001
Hauptverfasser: Aubert, B., Bona, M., Karyotakis, Y., Lees, J. P., Poireau, V., Prencipe, E., Prudent, X., Tisserand, V., Tico, J. Garra, Grauges, E., Lopez, L., Palano, A., Pappagallo, M., Eigen, G., Stugu, B., Sun, L., Abrams, G. S., Battaglia, M., Brown, D. N., Cahn, R. N., Jacobsen, R. G., Kerth, L. T., Kolomensky, Yu. G., Lynch, G., Osipenkov, I. L., Ronan, M. T., Tackmann, K., Tanabe, T., Hawkes, C. M., Soni, N., Watson, A. T., Koch, H., Schroeder, T., Walker, D., Asgeirsson, D. J., Fulsom, B. G., Hearty, C., Mattison, T. S., McKenna, J. A., Barrett, M., Khan, A., Blinov, V. E., Bukin, A. D., Buzykaev, A. R., Druzhinin, V. P., Golubev, V. B., Onuchin, A. P., Serednyakov, S. I., Skovpen, Yu. I., Solodov, E. P., Todyshev, K. Yu, Bondioli, M., Curry, S., Eschrich, I., Kirkby, D., Lankford, A. J., Lund, P., Mandelkern, M., Martin, E. C., Stoker, D. P., Abachi, S., Buchanan, C., Atmacan, H., Gary, J. W., Liu, F., Long, O., Vitug, G. M., Yasin, Z., Zhang, L., Sharma, V., Campagnari, C., Hong, T. M., Kovalskyi, D., Mazur, M. A., Richman, J. D., Beck, T. W., Eisner, A. M., Flacco, C. J., Heusch, C. A., Kroseberg, J., Lockman, W. S., Martinez, A. J., Schalk, T., Schumm, B. A., Seiden, A., Wilson, M. G., Winstrom, L. O., Cheng, C. H., Doll, D. A., Echenard, B., Fang, F., Hitlin, D. G., Narsky, I., Piatenko, T., Porter, F. C., Andreassen, R., Mancinelli, G., Meadows, B. T., Mishra, K., Sokoloff, M. D.
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Sprache:eng
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Zusammenfassung:We report the results of a search for Z ( 4430 ) − decay to J / ψ π − or ψ ( 2 S ) π − in B − , 0 → J / ψ π − K 0 , + and B − , 0 → ψ ( 2 S ) 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 ( 2 S ) 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 ( 2 S ) 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 B ( B − → Z − ¯¯¯¯ K 0 , Z − → J / ψ π − ) < 1.5 × 10 − 5 , B ( B 0 → Z − K + , Z − → J / ψ π − ) < 0.4 × 10 − 5 , B ( B − → Z − ¯¯¯¯ K 0 , Z − → ψ ( 2 S ) π − ) < 4.7 × 10 − 5 , and B ( B 0 → Z − K + , Z − → ψ ( 2 S ) π − ) < 3.1 × 10 − 5 at 95% confidence level, where the Z ( 4430 ) − mass and width have been fixed to the reported central values.
ISSN:1550-7998
2470-0010
1550-2368
2470-0029
DOI:10.1103/PhysRevD.79.112001