1983
DOI: 10.1103/physrevd.27.2755
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Radiative decays of heavy quarkonia in an extended vector-dominance model

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Cited by 22 publications
(13 citation statements)
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“…It should be also noted that phenomenological models can have compatible predictions. In an extended vector-dominance model one indeed finds the branching ratio from 5.3 × 10 −7 to 2.5 × 10 −6 [9], but this model has no direct relation to QCD as the fundamental theory of strong interaction.…”
mentioning
confidence: 98%
“…It should be also noted that phenomenological models can have compatible predictions. In an extended vector-dominance model one indeed finds the branching ratio from 5.3 × 10 −7 to 2.5 × 10 −6 [9], but this model has no direct relation to QCD as the fundamental theory of strong interaction.…”
mentioning
confidence: 98%
“…This process is important for testing various phenomenological mechanisms, including Vector Meson Dominance [32,33,34], η c − η mixing [35,36], two gluon couplings to qq states [33], and final state radiation by light quarks [32]. The value of R J/ψ = B(J/ψ→γη) B(J/ψ→γη ) is predicted in first order perturbation theory [32], and R ψ =…”
Section: ψ → γPmentioning
confidence: 99%
“…Baier and Grozin [9] showed that for light vector mesons (such as J/ψ) there might be an additional "anomaly" diagram that contributes significantly to the radiative decays. Noting that VDM has no direct relation to QCD as the fundamental theory of strong interactions, and referring to [7], Ma tries to address the problem by using factorization at tree level with NRQCD matrix elements to describe the heavy vector meson portion multiplied by a set of twist-2 and twist-3 gluonic distribution amplitudes [10].…”
Section: Introductionmentioning
confidence: 99%
“…Several authors have tried to explain the lack of signals in radiative Υ(1S) decays into pseudoscalar mesons, using a variety of models which produce branching fraction predictions of 10 −6 to 10 −4 . Employing the Vector Meson Dominance Model (VDM), Intemann [7] predicts the branching fractions for the heavy vector meson radiative decay into light pseudoscalar mesons. Using the mixing mechanism of η, η ′ with the as-yet-unobserved pseudoscalar resonance η b , Chao [8] first calculated the mixing angle λ ηη b in order to estimate the radiative branching fractions.…”
Section: Introductionmentioning
confidence: 99%