Refine
Document Type
- Article (68)
- Preprint (28)
- Doctoral Thesis (1)
Language
- English (97)
Has Fulltext
- yes (97)
Is part of the Bibliography
- no (97)
Keywords
- BESIII (7)
- Branching fraction (7)
- e +-e − Experiments (4)
- Lepton colliders (3)
- Charm Physics (2)
- Charmed mesons (2)
- Electroweak interaction (2)
- Initial state radiation (2)
- Leptonic, semileptonic & radiative decays (2)
- Particle decays (2)
Using a sample of (10.09±0.04)×109 J/ψ events collected with the BESIII detector, a partial wave analysis of J/ψ→γη′η′ is performed.The masses and widths of the observed resonances and their branching fractions are reported. The main contribution is from J/ψ→γf0(2020) with f0(2020)→η′η′, which is found with a significance of greater than 25σ. The product branching fraction B(J/ψ → γf0(2020))⋅B(f0(2020) → η′η′ is measured to be (2.63±0.06(stat.) + 0.31−0.46(syst.))×10−4.
Using 5.9 pb−1 of e+e− annihilation data collected at center-of-mass energies from 3.640 to 3.701 GeV with the BESIII detector at the BEPCII Collider, we measure the observed cross sections of e+e−→K0SX (where X=anything). From a fit to these observed cross sections with the sum of continuum and ψ(3686) and J/ψ Breit-Wigner functions and considering initial state radiation and the BEPCII beam energy spread, we obtain for the first time the inclusive decay branching fraction B(ψ(3686)→K0SX)=(16.04±0.29±0.90)%, where the first uncertainty is statistical and the second is systematic.
Based on a sample of (10.09±0.04)×109 J/ψ events collected with the BESIII detector operating at the BEPCII storage ring, a partial wave analysis of the decay J/ψ→γηη′ is performed. An isoscalar state with exotic quantum numbers JPC=1−+, denoted as η1(1855), has been observed for the first time with statistical significance larger than 19σ. Its mass and width are measured to be (1855±9+6−1)~MeV/c2 and (188±18+3−8)~MeV, respectively. The product branching fraction B(J/ψ→γη1(1855)→γηη′) is measured to be (2.70±0.41+0.16−0.35)×10−6. The first uncertainties are statistical and the second are systematic. In addition, an upper limit on the branching ratio B(f0(1710)→ηη′)/B(f0(1710)→ππ) is determined to be 1.61×10−3 at 90\% confidence level, which lends support to the hypothesis that the f0(1710) has a large glueball component.
Based on (10087±44)×106 J/ψ events collected with the BESIII detector, the process J/ψ→γπ+π−η′ is studied using two dominant decay channels of the η′ meson, η′→γπ+π− and η′→ηπ+π−,η→γγ. The X(2600) is observed with a statistical significance larger than 20σ in the π+π−η′ invariant mass spectrum, and it has a strong correlation to a structure around 1.5 GeV/{\it c}2 in the π+π− invariant mass spectrum. A simultaneous fit on the π+π−η′ and π+π− invariant mass spectra with the two η′ decay modes indicates that the mass and width of the X(2600) state are 2617.8±2.1+18.2−1.9 MeV/{\it c}2 and 200±8+20−17 MeV, respectively. The corresponding branching fractions are measured to be B(J/ψ→γX(2600))⋅B(X(2600)→f0(1500)η′)⋅B(f0(1500)→π+π−) = (3.39±0.18+0.91−0.66)×10−5 and B(J/ψ→γX(2600))⋅B(X(2600)→f′2(1525)η′)⋅B(f′2(1525)→π+π−) = (2.43±0.13+0.31−1.11)×10−5, where the first uncertainties are statistical, and the second systematic.
Using 448.1 × 106 ψ(3686) decays collected with the BESIII detector at the BEPCII e+e− storage rings, the branching fractions and angular distributions of the decays χcJ → Ξ−Ξ¯¯¯¯+ and Ξ0Ξ¯¯¯¯0 (J = 0, 1, 2) are measured based on a partial-reconstruction technique. The decays χc1 → Ξ0Ξ¯¯¯¯0 and χc2 → Ξ0Ξ¯¯¯¯0 are observed for the first time with statistical significances of 7σ and 15σ, respectively. The results of this analysis are in good agreement with previous measurements and have significantly improved precision.
Clinical application of transcranial Doppler for detection of cerebral emboli during cardiac surgery
(2010)
Objective: Neurologic injury is one of the most damaging complications for cardiac surgery. How to decrease neurologic impairment by improving perioperative monitoring remains a challenge for both cardiac surgeons and anesthetists. For this reason, transcranial doppler (TCD) has been widely used in cerebral monitoring during cardiac surgery. In this study, two experiments of clinical application of TCD for detection of cerebral emboli during cardiac surgery were to be done. One was “Solid and gaseous cerebral emboli during valvular surgery are significantly reduced with axillary artery cannulation”. The other was “Do intraoperative cerebral embolic signals differ between valvular surgery (VS) and CABG”. Methods: In experiment one, 20 valve and combined procedures with aortic cannulation (AoC group) were compared to 18 procedures with axillary cannulation (AxC group) in a prospective non-randomized study. In experiment two, 18 VS patients and 18 CABG patients were matched by extracorporeal circulation (ECC) time retrospectively. Intraoperative monitoring of both middle cerebral arteries was performed with TCD discriminating between solid and gaseous embolic signals (ES). Results: In experiment one, the AxC group had less solid ES than the AoC group (38±22 vs 55±25, P<0.05), but no significant difference was found in gaseous (501±271 vs 538±333, P>0.05) and total (539 ± 279 vs 593 ± 350, P>0.05) ES. The AxC group had less solid ES during arterial cannulation (2.1±1.5 vs 6.6±3.6, P<0.05) and during aortic cross-clamp time (4.4 ±3.1 vs 10.2 ± 5.1, P<0.05) than the AoC group. During ECC, gaseous ES was not significantly different between groups (398±210 vs 448±291, P>0.05). However, AxC showed less gaseous ES (85±68 vs 187±148, P<0.05) and less gaseous ES per minute (1.8±1.5 vs 4.5±3.2, P<0.05) during weaning off extracorporeal circulation than the AoC group. No significant difference in gaseous ES (313±163 vs 261±189, P>0.05) and gaseous ES per minute (3.1±2.2 vs 2.8±2.2, P>0.05) was found between groups from bypass start to aortic declamping. No neurologic complications occurred. In experiment two, no significant difference was found in solid (38±20 vs 40±26, P>0.05) or gaseous (457±263 vs 412±157, P>0.05) ES between the VS and CABG group during the whole recording time. During ECC, solid ES (20±10 vs 24±19, P>0.05) and gaseous ES (368±230 vs 317±157, P>0.05) were comparable between groups. Specifically, during weaning off ECC, the VS group had more gaseous ES/min (5.6±3.6 vs 3.1±1.2, P<0.05) than the CABG group. But this difference in gaseous ES/min was not significant during the period from bypass start to aortic declamping (2.5±1.8 vs 3.0±1.8, P>0.05). Conclusion: Cerebral embolization does occur during cardiac surgery. Through these two experiments, we demonstrated the feasibility and importance of clinical application of transcranial doppler for detection of cerebral emboli during cardiac surgery. Due to the diversity in clinical application of TCD, it is impossible to compare the number of ES between different research centers. More unified standards should be drawn in order to make wider clinical application possible. Up till now, no robust evidence shows the correlation between intraoperative ES and postoperative neurological impairment. The research on intraoperative ES and postoperative neurological impairment should rely on a complete concept.
Relative fractions and phases of the intermediate decays are determined. With the detection efficiency estimated by the results of the amplitude analysis, the branching fraction of Dþ s → K−Kþπþπ0 decay is measured to be ð5.42 0.10stat 0.17systÞ%.