G. S. Huang
A5105457868- Particle physics theoretical and experimental studies
- Quantum Chromodynamics and Particle Interactions
- High-Energy Particle Collisions Research
- Dark Matter and Cosmic Phenomena
- Neutrino Physics Research
- Black Holes and Theoretical Physics
- Computational Physics and Python Applications
- Nuclear physics research studies
- Particle Detector Development and Performance
- Medical Imaging Techniques and Applications
- Superconducting Materials and Applications
- Advanced DC-DC Converters
- Particle Accelerators and Free-Electron Lasers
- Advanced Memory and Neural Computing
- Atomic and Subatomic Physics Research
- Neuroscience and Neural Engineering
- Cellular Automata and Applications
- Radiation Therapy and Dosimetry
- Geophysics and Gravity Measurements
- Geomagnetism and Paleomagnetism Studies
- Stochastic processes and statistical mechanics
- Radioactive Decay and Measurement Techniques
- Berberine and alkaloids research
- Cardiovascular, Neuropeptides, and Oxidative Stress Research
- Pulmonary Hypertension Research and Treatments
University of Science and Technology of China
2016-2025
Purple Mountain Observatory
2024
Chinese Academy of Sciences
2005-2024
Institute of High Energy Physics
2003-2023
University of Edinburgh
2023
Henan University
2023
Inner Mongolia University
2023
Imperial College London
2023
University of Oklahoma
2011-2012
MSD (Serbia)
2011
Paper presents a three-level soft switching LLC series resonant dc/dc converter. Zero-voltage (ZVS) is achieved for each main switch without any auxiliary circuit. Voltage stress of half input voltage. Zero-current-switching (ZCS) rectifier diodes. Wide input/output range can be under low frequency because two-stage resonance. Only one magnetic component required in this Efficiency higher high line input, so converter preferable candidate power products with the requirement hold up time. For...
The folding kinetics of a truncated form the N-terminal domain phage lambda repressor [lambda 6-85] has been investigated by using technique dynamic NMR. 6-85 shown previously to fold in purely two-state fashion. This allows determination and unfolding rates from simulation exchange-broadened aromatic resonances Tyr-22. were determined over range 1.35 3.14 M urea. urea dependence both rate constants is exponential, suggesting that rate-determining step invariant at concentrations studied....
Using $20.7\text{ }\text{ }{\mathrm{pb}}^{\ensuremath{-}1}$ of ${e}^{+}{e}^{\ensuremath{-}}$ annihilation data taken at $\sqrt{s}=3.671\text{ }\mathrm{GeV}$ with the $\mathrm{CLEO}\mathrm{\text{\ensuremath{-}}}c$ detector, precision measurements electromagnetic form factors charged pion, kaon, and proton have been made for timelike momentum transfer $|{Q}^{2}|=13.48\text{ }{\mathrm{GeV}}^{2}$ by reaction ${e}^{+}{e}^{\ensuremath{-}}\ensuremath{\rightarrow}{h}^{+}{h}^{\ensuremath{-}}$. The...
Using $281\text{ }\text{ }{\mathrm{pb}}^{\ensuremath{-}1}$ of ${e}^{+}{e}^{\ensuremath{-}}$ collisions recorded at the $\ensuremath{\psi}(3770)$ resonance with CLEO-c detector CESR (Cornell Electron Storage Ring), we determine absolute hadronic branching fractions charged and neutral $D$ mesons using a double tag technique. Among measurements for three ${D}^{0}$ six ${D}^{+}$ modes, obtain reference...
The decay channel J/psi --> gamma(pi)(+)pi(-)eta is analyzed using a sample of 5.8 x 10(7) events collected with the BESII detector. A resonance, Chi(1835), observed in pi(+)pi(-)eta invariant-mass spectrum statistical significance 7.7 sigma. fit Breit-Wigner function yields mass M = 1833.7 +/- 6.1(stat) 2.7(syst) MeV/c(2), width Tau 67.7 20.3(stat) 7.7(syst) and product branching fraction B(J/psi gammaChi) . B(Chi pi(+)pi(-)eta) [2.2 0.4(stat) 0.4(syst)] 10(-4). Chi(1835) are not compatible...
Based on 58 million BESII J/psi events, the bar{K}^*(892)^0K^+pi^- channel in K^+K^-pi^+pi^- is studied. A clear low mass enhancement invariant spectrum of K^+pi^- observed. The does not come from background other decay channels, nor phase space. Two independent partial wave analyses have been performed. Both favor that kappa, an isospinor scalar resonant state. average and width kappa two are 878 +- 23^{+64}_{-55} MeV/c^2 499 52^{+55}_{-87} MeV/c^2, respectively, corresponding to a pole at...
Using a data sample with total integrated luminosity of 10.0 pb$^{-1}$ collected at center-of-mass energies 2.6, 3.07 and 3.65 GeV BESII, cross sections for $e^+e^-$ annihilation into hadronic final states ($R$ values) are measured statistical errors that smaller than 1%, systematic about 3.5%. The running strong interaction coupling constants $α_s^{(3)}(s)$ $α_s^{(5)}(M_Z^2)$ determined from the $R$ values.
Recent observations of the light component cosmic-ray spectrum have revealed unexpected features that motivate further and more precise measurements up to highest energies. The Dark Matter Particle Explorer is a satellite-based experiment has been operational since December 2015, continuously collecting data on high-energy cosmic particles with very good statistics, energy resolution, particle identification capabilities. In this work, latest proton+helium in range from 46 GeV 464 TeV are...
We measure the cross section for e+e- -->psi(3770) -->hadrons at Ec.m.=3773 MeV to be (6.38+/-0.08(+0.41)(-0.30) nb using CLEO detector CESR collider. The difference between this and -->DD same energy is found (-0.01+/-0.08(+0.41)(-0.30) nb. With observed total section, we extract Gamma(ee)(psi(3770))=(0.204+/-0.003(+0.041)(-0.027) keV. Uncertainties shown are statistical systematic, respectively.
An enhancement near the mp+MΛ mass threshold is observed in combined pΛ¯ and p¯Λ invariant-mass spectrum from J/ψ→pK−Λ¯+c.c. decays. It can be fit with an S-wave Breit-Wigner resonance a m=2075±12(stat)±5(syst) MeV width of Γ=90±35(stat)±9(syst) MeV; it also P-wave resonance. Evidence for similar ψ′→pK−Λ¯+c.c. The analysis based on samples 5.8×107J/ψ 1.4×107ψ′ decays accumulated BES II detector at Beijing Electron-Positron Collider.Received 19 May...
Using 14M $\psi(2S)$ events accumulated by BESII at the BEPC, a Covariant Helicity Amplitude Analysis is performed for $\psi(2S)\to\pi^+\pi^-J/\psi, J/\psi\to \mu^+\mu^-$. The $\pi^+\pi^-$ mass spectrum, distinctly different from phase space, suggests $\sigma$ production in this process. Two theoretical schemes are used global fit to data. results consistent with existence of $\sigma$. pole position determined be $(552^{+84}_{-106})-i(232^{+81}_{-72})$ MeV/$c^2$.
We have studied the inclusive photon spectrum in psi(2S) decays using CLEO III detector. present most precise measurements of electric dipole (E1) transition rates for psi(2S)--> gamma chicJ(1P) (J=0,1,2). also confirm hindered magnetic (M1) transition, psi(2S)-->gamma etac(1S). However, direct M1 etac(2S) observed by Crystal Ball as a narrow peak at energy 91 MeV is not found our data.
A broad peak is observed at low K+K− invariant mass in J/ψ→K+K−π0 decays found a sample of 5.8×107 J/ψ events collected with the BESII detector. The statistical significance resonance much larger than 5σ. partial wave analysis shows that JPC this structure 1--. Its pole position determined to be [1576−55+49(stat)−91+98(syst)] MeV/c2−i2[818−23+22(stat)−133+64(syst)] MeV/c2. These parameters are not compatible any known meson resonances.Received 21 June...
Using a data sample of 58×106 J/ψ decays collected with the Beijing Spectrometer II detector at Electron Positron Collider, searches for invisible η and η′ in to ϕη ϕη′ are performed. The ϕ signals, which reconstructed K+K− final states, used tag decays. No signals found either or η′, upper limits 90% confidence level determined be 1.65×10−3 ratio B(η→invisible)B(η→γγ) 6.69×10−2 B(η′→invisible)B(η′→γγ). These first into states.Received 4 July...
The decay channel $J/\ensuremath{\psi}\ensuremath{\rightarrow}\ensuremath{\gamma}\ensuremath{\omega}\ensuremath{\omega}$, $\ensuremath{\omega}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\pi}}^{0}$ is analyzed using a sample of $5.8\ifmmode\times\else\texttimes\fi{}{10}^{7}$ $J/\ensuremath{\psi}$ events collected with the BESII detector. $\ensuremath{\omega}\ensuremath{\omega}$ invariant mass distribution peaks at $1.76\text{ }\text{...