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|a Zhao, M.
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|a Massachusetts Institute of Technology. Department of Physics
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|a Massachusetts Institute of Technology. Laboratory for Nuclear Science
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|a Fisher, Peter H.
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|a Zhao, M.
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|a Yamamoto, R. K.
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|a Taylor, Frank E.
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|a Spitznagel, M.
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|a Sciolla, Gabriella
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|a Henderson, Shawn Wesley
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|a Dujmic, Denis
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|a Cowan, Ray Franklin
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|a Fisher, Peter H.
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|a Yamamoto, R. K.
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|a Taylor, Frank E.
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|a Spitznagel, M.
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|a Sciolla, Gabriella
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|a Henderson, Shawn Wesley
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|a Dujmic, Denis
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|a Cowan, Ray Franklin
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|a Fisher, Peter H.
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|a Search for the Z(4430)[superscript -] at BABAR
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|a Search for the Z(4430)- at BABAR
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|b American Physical Society,
|c 2010-06-02T19:42:45Z.
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|z Get fulltext
|u http://hdl.handle.net/1721.1/55371
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|a We report the results of a search for Z(4430)- decay to J/psi pi- or psi(2S)pi - in B-,0→J/psi pi-K0,+ and B-,0-->psi(2S)pi-K0,+ 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[superscript -1]. Each Kpi- mass distribution exhibits clear K*(892) and K[subscript 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 Kpi- scattering amplitude measurements. Each Kpi- angular distribution varies significantly in structure with Kpi- mass, and is represented in terms of low-order Legendre polynomial moments. We find that each J/psi pi- or psi(2S)pi- mass distribution is well described by the reflection of the measured Kπ- 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/psi pi- or psi(2S)pi- mass distribution, nor in the corresponding distributions for the regions of Kpi- mass for which observation of the Z(4430)- signal was reported. We obtain branching-fraction upper limits B(B- -->Z-K[over-bar] 0,Z-→J/psi pi-)<1.5×10[superscript -5], B(B0-->Z-K+,Z- -->J/psi pi-)<0.4×10[superscript -5], B(B- -->Z-K[over-bar] 0,Z- -->psi(2S)pi-)<4.7×10[superscript -5], and B(B0-->Z-K+,Z--->psi(2S)pi-)<3.1×10[superscript -5] at 95% confidence level, where the Z(4430)- mass and width have been fixed to the reported central values.
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|a Science and Technology Facilities Council, United Kingdom
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|a MEC (Spain)
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|a Ministry of Education and Science of the Russian Federation
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|a Norges forskningsråd
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|a FOM of the Netherlands
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|a Istituto Nazionale di Fisica Nucleare of Italy
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|a Deutsche Forschungsgemeinschaft
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|a Bundesministerium für Bildung und Forschung, Germany
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|a Institut National de Physique Nucleaire et Physique des Particules/CNRS
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|a Commissariat à l'Energie Atomique (France)
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|a Natural Sciences and Engineering Research Council of Canada
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|a National Science Foundation
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|a United States Department of Energy
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|a en_US
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|a Article
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|t Physical Review D
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