Higher-order multipole amplitudes in charmonium radiative transitions

نویسندگان

  • M. Artuso
  • S. Blusk
  • S. Khalil
  • R. Mountain
  • K. Randrianarivony
  • T. Skwarnicki
  • S. Stone
  • J. C. Wang
  • L. M. Zhang
  • G. Bonvicini
  • D. Cinabro
  • A. Lincoln
  • M. J. Smith
  • P. Zhou
  • J. Zhu
  • P. Naik
  • J. Rademacker
  • D. M. Asner
  • K. W. Edwards
  • J. Reed
  • A. N. Robichaud
  • G. Tatishvili
  • E. J. White
  • R. A. Briere
  • H. Vogel
  • P. U. E. Onyisi
  • J. L. Rosner
  • J. P. Alexander
  • D. G. Cassel
  • R. Ehrlich
  • L. Fields
  • R. S. Galik
  • L. Gibbons
  • S. W. Gray
  • D. L. Hartill
  • B. K. Heltsley
  • J. M. Hunt
  • D. L. Kreinick
  • V. E. Kuznetsov
  • J. Ledoux
  • H. Mahlke-Krüger
  • J. R. Patterson
  • D. Peterson
  • D. Riley
  • A. Ryd
  • A. J. Sadoff
  • X. Shi
  • S. Stroiney
  • W. M. Sun
  • J. Yelton
  • P. Rubin
  • N. Lowrey
  • S. Mehrabyan
  • M. Selen
  • J. Wiss
  • M. Kornicer
  • R. E. Mitchell
  • M. R. Shepherd
  • C. M. Tarbert
  • D. Besson
  • T. K. Pedlar
  • J. Xavier
  • D. Cronin-Hennessy
  • K. Y. Gao
  • J. Hietala
  • R. Poling
  • P. Zweber
  • S. Dobbs
  • Z. Metreveli
  • K. K. Seth
  • B. J. Y. Tan
  • A. Tomaradze
  • S. Brisbane
  • J. Libby
  • L. Martin
  • A. Powell
  • P. Spradlin
  • C. Thomas
  • G. Wilkinson
  • H. Mendez
  • J. Y. Ge
  • D. H. Miller
  • I. P. J. Shipsey
  • B. Xin
  • G. S. Adams
  • D. Hu
  • B. Moziak
  • J. Napolitano
  • K. M. Ecklund
  • J. Insler
  • H. Muramatsu
  • C. S. Park
  • E. H. Thorndike
چکیده

Using 24 million ψ′ ≡ ψ(2S) decays in CLEO-c, we have searched for higher multipole admixtures in electric-dipole-dominated radiative transitions in charmonia. We find good agreement between our data and theoretical predictions for magnetic quadrupole (M2) amplitudes in the transitions ψ′ → γχc1,c2 and χc1,c2 → γJ/ψ, in striking contrast to some previous measurements. Let b2 and a2 denote the normalized M2 amplitudes in the respective aforementioned decays, where the superscript J refers to the angular momentum of the χcJ . By performing unbinned maximum likelihood fits to full five-parameter angular distributions, we found the following values of M2 admixtures for Jχ=1: aJ=1 2 = (−6.26± 0.63± 0.24)× 10−2 and bJ=1 2 = (2.76± 0.73± 0.23)× 10−2, which agree well with theoretical expectations for a vanishing anomalous magnetic moment of the charm quark. For Jχ=2, if we fix the electric octupole (E3) amplitudes to zero as theory predicts for transitions between charmonium S states and P states, we find aJ=2 2 = (−9.3±1.6±0.3)×10−2 and bJ=2 2 = (1.0± 1.3± 0.3)× 10−2. If we allow for E3 amplitudes we find, with a four-parameter fit, aJ=2 2 = (−7.9±1.9±0.3)×10−2, bJ=2 2 = (0.2±1.4±0.4)×10−2, aJ=2 3 = (1.7±1.4±0.3)×10−2, and bJ=2 3 = (−0.8 ± 1.2 ± 0.2) × 10−2. We determine the ratios aJ=1 2 /aJ=2 2 = 0.67 −0.13 and aJ=1 2 /b J=1 2 = −2.27 −0.99, where the theoretical predictions are independent of the charmed quark magnetic moment and are aJ=1 2 /a J=2 2 = 0.676± 0.071 and aJ=1 2 /bJ=1 2 = −2.27± 0.16.

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تاریخ انتشار 2009