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1.
The BES barrel shower counter prototype was tested with electron and pion beam in the momentum range from 0.2 to 2.0GeV/c at 12GeV PS test beam line of KEK, the preliminary results were reported. Four types of gas mixtures which were used in prototype have been tested: 40% Ar/60% Isobutane, 44.5% Ar/44.5%CH4/11% Methylel, 47%Ar/47%%CH4/6% Methylel, 49.3%Ar/49.3%CH4/1.4% Ethyl alcohol. The results show that using SQS tube as sampling means in BES shower is feasible way for BEPC region.  相似文献   

2.
Based on the electroweak unified standard model,the probability Pi for the production of i-quark jet (i=u,d,c and b)in e+e annihilation has been studied.The probability Pi is a function of energy s.The calculated component ratios of Pu:Pd:Ps:Pc:Pb are 4:1:1:4:1 for s<30GeV.7:9:9:7:9 for s=mz=91.16GeV and 1:1:1:1:1 for s=78 and 117GeV,respectively.Using Pc and Pb,we whave calculated the yields of charmed and beautiful mesons in e+e annihilation at s=10—178GeV.  相似文献   

3.
The scale for visible jets produced in e+e Collisions is studied in some details using Monte Carlo method. It is demonstrated, based on the historical fact that the 3-jet events were firstly observed in e+ e- experiments at √S=17—30GeV,and the relative transverse momentum for visible jets is in the region kt,~5—10GeV/c. It is further shown, using a concrete example, that the number of jets in an event could be correctly evaluated only when kt is in this region. The dynamical fluctuations inside jets determined through different values of kt are compared carefully. It turns out that only when kt,~5—10GeV/c the dynamical fluctuations inside jets will possess the best anomalous scaling property. The relation between the scale 5-10GeV/c of visible jets and the scale 1-2GeV of perturbative QCD is discussed.  相似文献   

4.

In the framework of T2HDM, we calculated the new physics contributions involving neutral Higgs bosons to the branching ratios of B0s,d→l+l (l=e, μ) decays. Comparing the theoretical predictions with the experimental upper-limits, we found that (a) The data of Br(B0d→l+l) give the upper bound on tanβ: tanβ≤22, while Br(B0s→l+l) give tanβ≤12 for fixed δ=0°, mH+=350 GeV, mH0=160 GeV, mh0=115 GeV and mA0=120 GeV; (b) A light neutral Higgs boson mass mh0 (mA0) less than 50 GeV (120 GeV) is excluded by the data of branching ratios for B0s,d→l+l(l=μ) decays with tanβ=10; (c) The bounds on mh0 and tanβ, or mA0 and tanβ are strongly correlated: a smaller (larger) tanβ means a lighter (heavier) neutral Higgs boson.

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5.
Masses of the Ds(0^±) mesons are investigated from a view-point of ordinary light-heavy system in the framework of the Gaussian sum rules, which are worked out by means of the Laplacian transformation to the usual Borel sum rules. Using the standard input of QCD non-perturbative parameters, the corresponding mass spectra and couplings of the currents to the Ds(0^±) mesons are obtained. Our results are mDs(0-) = 1.968±0.016±0.003 GeV and mDs(0+) = 2.320 ±0.014 ± 0.003 GeV, which are in good accordance with the experimental data, 1.969 GeV and 2.317 GeV.  相似文献   

6.
With data collected by the Beijing Spectmmeter (BES) in the J/ψ,ψ′, and Ds energy region, a lot of e+e final state evenb are selected in the solid angle region covered by the endcap shower counters (ESC). Some characteristics of the ESC are analysed, such as the spectrnun of pulse height for, a single counter cell, the hit nwnbers in the ESC and in every reading layer of the ESC, the shower energies deposited in the ESC and in every layer of the BSC. The energy resoiudon of the ESC in obtained to be about 22%/E(GeV) Based on the odginal frame of SOBER, a Monte Carlo simulation program for the ESC is developed with a dual Gaussian pulse height spectrtun of the single counter cell. The electromagnetic cascades are calculated by the EGS4 package and a three-dimension magnetic field in the BES is included. The simulation results agree with experimented data well.  相似文献   

7.
We discuss about the nature of f0(400-1200) which we decompose into three parts, i.e., t-channel ρ meson and f2(1270) meson exchange plus an additional s-channel resonance f0(X). Below 1.2GeV of ππ invariant mass, t-channel ρ meson exchange can explain the I=2 ππ S-wave scattering very well. However, the f2(1270) meson exchange must be considered for the ππ invariant mass above 1.2GeV. With the t-channel ρ meson and f2(1270) meson exchange fixed by the isotensor ππ→ππ S-wave scattering, we re-fit the CERN-Mülich(CM) data on ππ scattering to get parameters for the f0(X). We find that it is necessary to introduce a broad 0++ resonance with a pole about 1.6-1.7GeV.  相似文献   

8.
In this paper the experimental value of radiative correction Δr was derived from the new data of sin 2θw and W boson mass Mw given by LEP,CDF and other collaborations.A careful comparison of (Δr)exp with the standard model expectation was carried out.We first calculated the Δr at full one-loop level,and then the main two-loop contributions were included.More stringent upper bounds on Mt were obtained from the analysis of probability distribution:Mt175GeV at 95%C.L. for a given MH=100GeV.The effects on Nt from other experimental and theoretical errors were also computed.  相似文献   

9.
In this paper I summarize some results obtained from analyses of hadronic final state events. The analyzed data sample comes from Mark-J collaboration and covers an energy range from √S=12GeV to √S =46.78GeV. The integrated luminosity is 128.06Pb-1. We can search for production of open top quarks and toponium by measuring the total hadronic crossection R =3.85±0.02±0.12 was measured in the above mentioned energy range. It is consistent with R≈3.9 as expected from QCD for five different quark flavors. We search for the narrow bound states of the toponium from 39.79GeV to 46.78GeV. The most prominent resonance signal is at a c.m. energy √S=45.12±0.04GeV and results in an upper limit of Bh.Γee≤3.00keV(95% C.L.).  相似文献   

10.
The Compact Linear Collider (CLIC) is a future e+e- linear collider. The CLIC study concentrated on a design of center-of-mass energy of 3 TeV and demonstrated the feasibility of the technology. However, the physics also demands lower energy collision. To satisfy this, CLIC can be built in stages. The actual stages will depend on LHC results. Some specific scenarios of staged constructions have been shown in CLIC Concept Design Report (CDR). In this paper, we concentrate on the main linac lattice design for Ecm=1 TeV CLIC aiming to upgrade from Ecm=500 GeV CLIC and then to Ecm=3 TeV one. This main linac accelerates the electron or positron beam from 9 GeV to 500 GeV. A primary lattice design based on the 3 TeV CLIC main linac design and its optimization based on the beam dynamics study will be presented. As we use the same design principles as 3TeV CLIC main linac, this optimization is basically identical to the 3 TeV one. All the simulations results are obtained using the tracking code PLACET.  相似文献   

11.
We have examined the electroweak radiative corrections in the LEP precision data in view of the new measurements of MW and mt as well as the recent progress in the higher order radiative corrections. From the minimal L2-fit to the experimental Z-decay parameters (with the aid of a modified ZFITTER program), we predict that MW=80.29(4)(2)rGeV where the first error is due to the uncertainty in the fitted mt for a fixed mH and the second error comes from the mH in the range 60􊖸rGeV, which is to be compared with the current world average MW=80.23(18)rGeV. The current world average value of MW and the 1994 LEP data definitely favor nonvanishing electroweak radiative corrections and are consistent with a heavy mt as measured by the recent CDF report but with a heavy Higgs scalar of about 400rGeV within the context of the minimal standard model. The sensitivity of and the errors in the best fit solutions due to the uncertainties in the gluonic coupling !s(MZ) and !(MZ) are also studied carefully. In addition we discuss how the future precision measurements of MW can provide a decisive test for the standard model with radiative corrections and give a profound implication for the measurement of t-quark and Higgs masses.  相似文献   

12.
At an altitude of 3220 meters above sea level in Yunnan Province, we measured, by using a G-M counter-magnetic spectrometer, the vertical integratted momentum spectrum of the cosmic muon with momentum larger than 4 GeV/c. The spectrum obtained from this experiment is expressed by a power function in the form of I(>p)=Qp+4)-1.86±0.06(cm-2·sr-1·s-1), where p is in GeV/c and Q is a constant. We also measured the charge ratio of muon in the 4—23 GeV/c momentum range. The result is Nμ/Nμ-=1.26±0.11. The error in the momentum measurement with spectrometer has been discussed and calculated.  相似文献   

13.
Angular distributions of projectile fragments P,Si,Al and Mg produced in collisions of 200A GeV 32S beam with Cu are measured.The range of σpt deduced is within 130—270MeV/c.  相似文献   

14.
A general parametrization of the symmetric KM matrix is given.The unitarity triangle is discussed,which embodies the unitarity of the symmetric KM matrix and CP violation.It is shown that the symmetric KM matrix is consistent with the directly measured values of the KM matrix elements,CP violation parameter │ε│ of K-K system,and B0d-B0d mixing parameter χd,provided the t-quark mass is large,mt≥160GeV.If │V12│=│V21│is confirmed by further experiments,KM matrix will turn out to be symmetric,so that a parameter is reduced in the standard model.  相似文献   

15.
The differential cross section of deuteron-deuteron elastic scattering at Pd=5.76 GeV/c is calculated based on the Glauber multiple scattering theory in nucleus-nucleus collision. The theoretical result is compared with the experimental data and the agreement is satisfactory. In addition, the influence of the input amplitude is discussed.  相似文献   

16.
According to the perturbative QCD method,we have calculated the P distributive cross sections,the Y distributive cross sections of the large P jets and the final state meson productivities in 800GeV/c Proton-Nucleus (Be,C,Al,Cu and Pb) collisions.The A dependence of the cross section at a given P was discussed by the EMC effect. The dσ/dP differential cross sections vs .P for various PA collisions are consistent with the new data.  相似文献   

17.
Absolute measurement of branching fractions of purely leptonic decay, semi-leptonic decay and φπ+ decay of the Ds meson at a c.m. energy of 4.03 GeV were completed from the BES experiment at the BEPC electron-positron collider. The method by using combined confidence level for pion and kaon separation, the Ds single and double tagging technology, and the maximum likelihood functions in the estimate of the Ds branching fractions are described in details. Discussion and comments on these physics results are made. Prospect for improved measurement of Ds physics in future is also given.  相似文献   

18.
Metal-tip/Pr0.7Ca0.3MnO3/Pt devices possess two types of I-V hysteresis: clockwise vs counter clockwise depending on the tip materials. The criteria for categorization of these two types of devices can be simply based on whether the Gibbs free energy of oxidation for the metal tip is lower or higher than that of PCMO, respectively. While the clockwise hysteresis can be attributed to electric field induced oxidation/reduction, the counter clockwise hysteresis can be explained by oxygen vacancy migration in an electrical field. Alternating-current conductance spectra also reveal distinct hopping barriers between these two categories of devices at high resistive states.  相似文献   

19.

The combination of partition temperature with Bose-Einstein statistics is generalized to describe the proton nucleus collision. The rapidity distribution of pp, p-Ar and p-Xe at PL=200GeV/c have been calculated and compared with experiment. The interesting possibility of observing pion condensation in p-A collision is investigated.

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20.
We suggest that the heavy neutral lepton in a specific version of SU(3)L×U(1) model can not only act as dark matter but also provide with a source of anomalous positrons in the cosmic rays above 10GeV.  相似文献   

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