Using a sample of 14 × 10 6 ψ(2S) events accumulated with the BES II detector, evidence for f
Ablikim M.;Bai J. Z.;Bian J. G.;Cai X.;Chang J. F.;Chen H. S.;Chen H. X.;Chen J. C.;Chen Jin;Chen M. L.;Chen Y. B.;Chu Y. P.
Physical Review D Particles Fields Gravitation and Cosmology
2004
The decays of J / ψ and ψ (2 S) to n K
Ablikim M.;Bai J. Z.;Cai X.;Chen H. S.;Chen H. X.;Chen J. C.;Chen Jin;Chen Y. B.;Chu Y. P.;Deng Z. Y.;Du S. X.;Fang J.
Physics Letters Section B Nuclear Elementary Particle and High Energy Physics
2008
Using 5.8 × 10 7 J / ψ events collected in the BESII detector, the radiative decay J / ψ → γ φ{symbol} φ{symbol} → γ K + K - K
Ablikim M.;Bai J. Z.;Bai Y.;Cai X.;Chen H. S.;Chen H. X.;Chen J. C.;Chen Jin;Chen Y. B.;Chu Y. P.;Deng Z. Y.;Du S. X.
Physics Letters Section B Nuclear Elementary Particle and High Energy Physics
2008
The polarization of the χ
Ablikim M.;Bai J. Z.;Bian J. G.;Cai X.;Chang J. F.;Chen H. S.;Chen H. X.;Chen J. C.;Chen Jin;Chen M. L.;Chen Y. B.;Chu Y. P.
Physical Review D Particles Fields Gravitation and Cosmology
2004
K*(892) 0 K̄*(892) 0 signals from χ
Ablikim M.;Bai J. Z.;Bian J. G.;Cai X.;Chang J. F.;Chen H. S.;Chen H. X.;Chen J. C.;Chen Jin;Chen M. L.;Chen Y. B.;Chu Y. P.
Physical Review D Particles Fields Gravitation and Cosmology
2004
Using 58 million J/ψ and 14 million ψ(2S) decays obtained by the BES II experiment, the branching fraction of J/ψ→π + π - π 0 is determined. The result is (2.10±0.12) X10 -2 , which is significantly higher than previous measurements.
Bai J. Z.;Bian J. G.;Cai X.;Chang J. F.;Chen H. S.;Chen H. X.;Chen J.;Chen J. C.;Chen M. L.;Chen Y. B.;Chu Y. P.;Cui X. Z.
Physical Review D Particles Fields Gravitation and Cosmology
2004
Decays of the ψ(2S) into vector plus pseudoscalar meson final states have been studied with 14 × 10 6 ψ(2S) events collected with the BESII detector. Branching fractions of ψ(2S) → Φη, Φη′, and ωη′, and upper limits of ψ(2S) → Φπ 0 and ωη are obtained: B(ψ(2S) → Φη) = (3.3 ± 1.1 ± 0.5) × 10 -5 , B(ψ(2S) → Φη′) = (3.1 ± 1.4 ± 0.7) × 10 -5 , and B(ψ-(2S) → ωη′) = (3.2
Ablikim M.;Bai J. Z.;Bian J. G.;Cai X.;Chang J. F.;Chen H. S.;Chen H. X.;Chen J. C.;Chen Jin;Chen M. L.;Chen Y. B.;Chu Y. P.
Physical Review D Particles Fields Gravitation and Cosmology
2004
Cross sections and form factors for e + e - → ωπ 0 , ρη, and ρη′ at center of mass energies of 3.650, 3.686, and 3.773 GeV are measured using data samples collected with the BESII detector at the BEPC. Also, the branching fractions of ψ(2S) → ωπ 0 , ρη, and ρη′ are determined to be (1.87 +0.68
Ablikim M.;Bai J. Z.;Bian J. G.;Cai X.;Chang J. F.;Chen H. S.;Chen H. X.;Chen J. C.;Chen Jin;Chen M. L.;Chen Y. B.;Chu Y. P.
Physical Review D Particles Fields Gravitation and Cosmology
2004
Rare decay modes J / ψ → D
Ablikim M.;Bai J. Z.;Cai X.;Chen H. S.;Chen H. X.;Chen J. C.;Chen Jin;Chen Y. B.;Chu Y. P.;Deng Z. Y.;Du S. X.;Fang J.
Physics Letters Section B Nuclear Elementary Particle and High Energy Physics
2008
By analyzing approximately 33 pb -1 of sample data collected at and around 3.773 GeV with the BES-II detector at the BEPC collider, we directly measured the branching fractions for the neutral and charged D inclusive semimuonic decays to be BF (D 0 → μ + X) = (6.8 ± 1.5 ± 0.8) % and BF (D + → μ + X) = (17.6 ± 2.7 ± 1.8) %, and determined the ratio of the two branching fractions to be frac(BF (D + → μ + X), BF (D 0 → μ + X)) = 2.59 ± 0.70 ± 0.25. © 2008 Elsevier B.V. All rights reserved.
Ablikim M.;Bai J. Z.;Bai Y.;Cai X.;Chen H. S.;Chen H. X.;Chen J. C.;Chen Jin;Chen Y. B.;Chu Y. P.;Deng Z. Y.;Du S. X.
Physics Letters Section B Nuclear Elementary Particle and High Energy Physics
2008