2006
DOI: 10.1103/physrevlett.97.202002
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Search for Invisible Decays ofηandηinJ/ψϕηandet al.

Abstract: Using a data sample of 58 x 10(6) J/psi decays collected with the Beijing Spectrometer II detector at the Beijing Electron Positron Collider, searches for invisible decays of eta and eta' in J/psi to phi eta and phi eta' are performed. The phi signals, which are reconstructed in K+K- final states, are used to tag the eta and eta' decays. No signals are found for the invisible decays of either eta or eta', and upper limits at the 90% confidence level are determined to be 1.65 x 10(-3) for the ratio B(eta-->invi… Show more

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Cited by 59 publications
(64 citation statements)
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“…[15], which in our case are M ψ , g ψe + e − , A and R. M ψ is of course very close to the nominal mass of the ψ(3770), g ψe + e − determines the strength of the cross section, A is related to the width of the resonance, and R determines the fall down of the resonance shape above the resonance peak. The parameters are fitted to the data of the cross section for e + e − → DD [12][13][14].…”
Section: Resultsmentioning
confidence: 99%
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“…[15], which in our case are M ψ , g ψe + e − , A and R. M ψ is of course very close to the nominal mass of the ψ(3770), g ψe + e − determines the strength of the cross section, A is related to the width of the resonance, and R determines the fall down of the resonance shape above the resonance peak. The parameters are fitted to the data of the cross section for e + e − → DD [12][13][14].…”
Section: Resultsmentioning
confidence: 99%
“…[11] were based on a particular quark model. , [13], [14]) for the cross section of e + e − → D 0D0 reaction, using the form factor of Eq. (34) and the parameters in Table II.…”
Section: Resultsmentioning
confidence: 99%
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