112531924
Monte Carlo tuning for the BESIII time-of-flight system
Using experimental data, Monte Carlo tuning is implemented for performance parameters associated with the scintillation counters and readout electronics of the BESIII time-of-flight (TOF) system, as part of the full simulation model. The implementation of the tuning is described for simulations designed to reproduce the performance of a number of TOP system parameters, including pulse height, hit efficiency, time resolution, dead channels and background. In addition, comparisons with experimental data are presented.
125677069
TUBE CHAMBERS FOR THE MUON FILTER OF THE L3 DETECTOR
56005177
Inclusive J production in Z0 decays
Abstract Inclusive J production in Z0 decays is observed via the leptonic decay mode J → l+l− (l = e,μ). We measure the branching ratio Br(Z0 → J + X) = (4.1 ± 0.7 (stat.) ± 0.3 (sys.)) × 10−3. We have calculated the fraction of the J mesons from b-hadron decay and find a branching ratio of Br(b → J + X)= (1.3±0.2(stat.)±0.2(sys.)) × 10−2. We determine the average fractional energy of bottom hadrons 〈XE > = 0.70±0.03 (stat.)+0.02−0.01 (sys.) using the momentum spectrum of the J mesons. From a study of the angle between the J and the most energetic jet, we set an upper limit on the branching ratio Br ( Z 0 → q q g ∗ ; g ∗ → J + X ) −4 at 90% confidence level.
122214277
A water Cherenkov calorimeter for long baseline neutrino oscillation experiments
Abstract We propose a water-based large homogeneous calorimeter as the next generation neutrino detector for ν factories and/or conventional ν beams. The Cherenkov light produced in water is sufficient to have good energy resolution, and the pattern recognition is realized by a modular water tank structure. Monte Carlo simulations show that the detector performance is excellent for identifying neutrino CC events while rejecting backgrounds.
118039047
Physics of tau and charm
The physics of tau and charm started in early 70's after J/$\psi$ and $\tau$ were discovered. Since then several dedicated accelerators and experiments were built with increasing luminosities and studies on light hadron spectroscopy, charmonium, electroweak and QCD were never interupted. New interests and surprises are not rare in this area. With the newly built BEPCII/BESIII, an even brighter future is foreseen.
18893994
The mass production and quality control of RPCs for the Daya Bay experiment
Abstract Resistive plate chambers will be used in the Daya Bay reactor neutrino experiment to help veto backgrounds created by cosmic-ray muons. The mass production of RPCs began in 2008 and by the end of 2009, 1600 RPCs (3500 m 2 ) had been produced and tested. This paper describes the production and quality control procedures, and quality assurance using cosmic-ray testing.
110151526
Linearity analysis for position sensitive detectors using finite element method
Abstract A Finite Element Method (FEM) to simulate and analyze position-sensitive detector (PSD) is presented in this paper. A computational model and analytical method for PSD is proposed. For example, two types of PSD with additional resistive bordered, i.e., pin-cushion PSD and square-bordered PSD, are simulated. The relationships among the structural parameters, electrical parameters and the position linearity performance of these two PSD are investigated. In addition, the load impedance effect is analyzed. The results are consistent with other researchers’ experimental results.
119093990
Observational Constraints on Dark Energy and Cosmic Curvature
Current observational bounds on dark energy depend on our assumptions about the curvature of the universe. We present a simple and efficient method for incorporating constraints from cosmic microwave background (CMB) anisotropy data and use it to derive constraints on cosmic curvature and dark energy density as a free function of cosmic time using current CMB, Type Ia supernova (SN Ia), and baryon acoustic oscillation data. We show that there are two CMB shift parameters, R{identical_to}{radical}({omega}{sub m}H{sub 0}{sup 2})r(z{sub CMB}) (the scaled distance to recombination) and l{sub a}{identical_to}{pi}r(z{sub CMB})/r{sub s}(z{sub CMB}) (the angular scale of the sound horizon at recombination), with measured values that are nearly uncorrelated with each other. Allowing nonzero cosmic curvature, the three-year WMAP (Wilkinson Microwave Anisotropy Probe) data give R=1.71{+-}0.03, l{sub a}=302.5{+-}1.2, and {omega}{sub b}h{sup 2}=0.02173{+-}0.00082, independent of the dark energy model. The corresponding bounds for a flat universe are R=1.70{+-}0.03, l{sub a}=302.2{+-}1.2, and {omega}{sub b}h{sup 2}=0.022{+-}0.00082. We give the covariance matrix of (R,l{sub a},{omega}{sub b}h{sup 2}) from the three-year WMAP data. We find that (R,l{sub a},{omega}{sub b}h{sup 2}) provide an efficient and intuitive summary of CMB data as far as dark energy constraints are concerned. Assuming the Hubble Space Telescope (HST) prior of H{sub 0}=72{+-}8more » (km/s) Mpc{sup -1}, using 182 SNe Ia (from the HST/GOODS program, the first year Supernova Legacy Survey, and nearby SN Ia surveys), (R,l{sub a},{omega}{sub b}h{sup 2}) from WMAP three-year data, and SDSS (Sloan Digital Sky Survey) measurement of the baryon acoustic oscillation scale, we find that dark energy density is consistent with a constant in cosmic time, with marginal deviations from a cosmological constant that may reflect current systematic uncertainties or true evolution in dark energy. A flat universe is allowed by current data: {omega}{sub k}=-0.006{sub -0.012-0.025}{sup +0.013+0.025} for assuming that the dark energy equation of state w{sub X}(z) is constant, and {omega}{sub k}=-0.002{sub -0.018-0.032}{sup +0.018+0.041} for w{sub X}(z)=w{sub 0}+w{sub a}(1-a) (68% and 95% confidence levels). The bounds on cosmic curvature are less stringent if dark energy density is allowed to be a free function of cosmic time, and are also dependent on the assumption about the early time property of dark energy. We demonstrate this by studying two examples. Significant improvement in dark energy and cosmic curvature constraints is expected as a result of future dark energy and CMB experiments.« less
121470985
Spectral action on a fuzzy sphere
In this paper, the spectral action for the free Dirac operator on a fuzzy 2-sphere is considered, based on the known results. We show that from the spectral point of view, the behavior of the fuzzy sphere can be divided into three regimes: the classical regime, the quasi-classical regime and the fuzzy regime. We also consider its application to quantum cosmology.
124635518
Tensor effects on the proton sd states in neutron-rich Ca isotopes and bubble structure of exotic nuclei
In the framework of the Hartree-Fock-Bogoliubov (HFB) approach with Skyrme interactions SLy5+T, SLy5+T-omega and several sets of the TIJ parametrizations, the evolution of the proton single-particle energy difference between the 2s(1/2) and 1d(3/2) orbits in Ca isotopes is investigated for the cases with and without the tensor force. It is shown that the energy difference evolution trends by using different Skyrme interactions without the tensor force are similar to each other. However, the energy differences are obviously influenced by the tensor force. Meanwhile, it is found that the inversion between the two orbits (2s(1/2)-1d(3/2) inversion) induced by the tensor force occurs around Ca-48 (by SLy5+T-omega) as well as in the nuclei very far from the stability. We understand the inversion phenomenon by analyzing the tensor contributions to the spin-orbit potentials and the radial wave functions of the two orbits. Finally, the proton density distributions of Ar-46 and Hg-206 are calculated by using several sets of Skyrme interactions with and without the tensor component. It is found that the parametrization SLy5+T-omega favors the bubble structure of Ar-46 resulting from the 2s(1/2)-1d(3/2) inversion. However, for Hg-206 any tensor parametrizations do not favor its bubble structure.
119217496
Revisiting generalized Chaplygin gas as a unified dark matter and dark energy model
In this paper, we revisit the generalized Chaplygin gas (GCG) model as a unified dark matter and dark energy model. The energy density of GCG model is given as ρGCG/ρGCG0=[Bs+(1−Bs)a−3(1+α)]1/(1+α), where α and Bs are two model parameters which will be constrained by type Ia supernova as standard candles, baryon acoustic oscillation as standard rulers and the seventh year full WMAP data points. In this paper, we will not separate GCG into dark matter and dark energy parts any more as adopted in the literature. By using the Markov Chain Monte Carlo method, we find the results $\alpha=0.00126_{-0.00126- 0.00126}^{+ 0.000970+ 0.00268}$ and $B_{s}= 0.775_{-0.0161- 0.0338}^{+ 0.0161+ 0.0307}$.