会计学季刊
Quarterly Journal of Accounting
主办单位:
香港中文大学会计学院
上海财经大学会计学院
南京大学商学院会计学系
ISSN: 3006-1415
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1984年, 第3卷, 第3期 
刊出日期:1984-05-30
  

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  • 徐永年, 张开明, 谢希德
    理论物理通讯. 1984, 3(3): 269-274.
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    In the present work, the chemisorption of Ge on GaAs(1lO) was studied by a cluster model using the charge self-consistent extended H ückel method (EHT) and the results thus obtained were compared with those derived from the experiments. It was shown from the calculation that after chemisorption, the substrate tends to relax back to the ideal unrelaxed state, after cleavage. The tilted angle of the As-Ga bond was reduced from the well khown 27° to 10°.The gap states which were driven into both the valence band and the conduction band due to relaxation will-be introduced into the gap after chemisorption. From the calculation of the total energy of the cluster, it was found that the Ge atom could bind to both Ga and As atoms although the binding of the latter was somewhat stronger. The gap states were derived from the p states of Ge and the s and p states of Ga and As atoms. The states will serve as donors and acceptors for p and n type materials respectively . From a comparison with the previous results concerning studies of group Ⅲ and Ⅴ metals on GaAs(110) surface, it seems that the change of surface relaxation after chemisorption might be the origin of gap states and the cause for Fermi level pinningr. The explanation was first put forward by Chen et al . from their experimental studies . The present calculation also gives the core shifts of Ga(3d) and As(3d) of the clean relaxation surfaces with respect to that of the bulk as well as the core shifts of Ga(3d) and As(3d) after the chemisorption of Ge atom. A chemisorption induced state which is attributed to a precursor state for a heterojunction interface state is also obtained at a binding energy near 7eV which is in fairly good agreement with the experimental result.
  • 陈鸿, 吴翔
    理论物理通讯. 1984, 3(3): 275-281.
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    A microscopic model of atomic tunneling states in amorphous solids is presented. It is shown that the existence of two-level system (TLS) is closely related to the void-Like structuxe defects and dangling bonds in the amorphous solids. The density of TLS and the distribution function of the barrier height of asymmetric double-well potential are given. Based on the model, the theoretical investigation; on the anomaly of ultrasonic attenuation and thermal conductivity has been made, and the results agree well with experiments.
  • 曾婉贞, 郝柏林, 王光瑞, 陈式刚
    理论物理通讯. 1984, 3(3): 283-295.
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    We calculated the universal scaling function g(x) and the scaling factor a as well as the convergence rate δ for perlodtripling, -quadrapling and-quintuplingLseguences of RL, RL2, RLR2, RL2R and RL3 types. The superstable periods are closely connected. to a set of polynomial Pn defined recursivcely by the original mapping. Some not able properties of these polynomials are studied. Several approaches to solving the renormalization group equation and estimating the scaling factors are suggested.
  • 杨新华, 钟毓澍
    理论物理通讯. 1984, 3(3): 297-311.
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    Using the hybrid chiral bag a formulation is developed for discussing the short range behaviour of the nuclear force. Quarks interact with each other via exchange gluons inside the bag and exchange "pion field" quanta on the bag surface. In terms of the Green's functions for the confined quarks, gluons in the bag and pions outside the bag the second order perturbation interaction energy of the sixquark state is derived. In principle, it can be used for any configurations. To compare with the result without the pion field outside the bag the DeTar's six-quark states are used for the numerical calculation. As estimated, the streagth of the repulsion core will increase. The numerical result will be shown in the succeeding paper.
  • 郑玉明, 华大平, 刘祖华
    理论物理通讯. 1984, 3(3): 313-321.
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    The color-analog Van der Waals force between two hadrons is studied by the coupling channel resonating group method in the framework of the Gaussian-type quark confinement potential. The problem of the boundary values for the two channel coupling differential equations is changed to the problem of the initial values. The equations are solved numerically by the Gill method. The calculated results show that there is no color Van der Waals force between hadrons in the confinement potential model. This indicates that the confinement potential model not only can describe the internal structure of hadrons but also can be used to calculate the hadron-hadron interactions.
  • 陆中道, 唐学田
    理论物理通讯. 1984, 3(3): 323-343.
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    An analytical solution is obtained for the 2n-dimensiona Fokker-Planck equation (F-P equation for short) with the harmonic oscillator potential. A few steps are involved in the derivation. First,the Lagrangian subsidiary equation is solved; then with its integral constants as new variables of the F-P equation, the diffusion equation is obtained and solved; at last, expressed in the original phase space, the solution of the F-P equation .is finally obtained. The analysis for the solution is made. The solution is a Gaussian type function and a δ-function of time. If a particle moves in a well in ali directions, then as t→∞, the distribution function can reach a stationary nonzero distribution-Maxuwell-Boltzmann type distribution (M-B distribution for short).As an example, the 2-dimensional F-P equation is solved and discussed in detail.
  • 范洪义, 阮图南
    理论物理通讯. 1984, 3(3): 345-357.
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    On the basis of the preceding paper[1]we present some new applications of both the normal rroduct form and the coherent state form of the Wigner operator,which involve deriving some new quantum operator formulas, giving the coherent state generalization of the Moyal theorem, evaluating some quantum operators which correspond to the given classical functions in the weyl manner and vice versa. Were it not for the Wigner operator's coherent state formulation given by us the above-mentioned calculations would be hard to perform.
  • 戴元本
    理论物理通讯. 1984, 3(3): 359-363.
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    A supersymmetrical preon model is proposed. In this model there are Higgs particles which are massless at the scale of confinement of hypercolor due to the supersymmetry and a discrete R symmetry. We show that in this model the low energy gauge symmetry SU(2)L×SU(2)R×U(1)B-L can be broken to U(1)Q at the scale of supersymmetry breaking by coupling to supergravity.
  • R. M. Doria, J. A. Helayel-Neto, 赵万云
    理论物理通讯. 1984, 3(3): 365-372.
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    A thermal Wilson loop for a model with two gauge fields associated with the same gauge group is discussed. Deconfinement appears at high temperature. However the colour of the deconfined matter cannot be specified.
  • 东方晓, 杜东生, 薛丕友, 周咸建
    理论物理通讯. 1984, 3(3): 373-377.
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    A realistic finite grand unified model has to accommodate at least three generations of ordinary fermions. When this criterion is imposed, we found that only few models of SU(N), SO(2N), SO (2N+1) and exceptional groups can survive as candidates for possible realistic finite supersymmetric grand unified models. All possible solutions are obtianed, but the SU(5) model is excluded.
  • 朱重远, 张鉴祖
    理论物理通讯. 1984, 3(3): 379-384.
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    The observation of the excess of Z0→e+e-γ can be explained by assuming that Z0 is radiatively decayed into a new scalar particle P0 which is subsequently turned into an e+e- pair. We argue that this assuhption does not conflict with the present experimental results.
  • Mujahid Kamran
    理论物理通讯. 1984, 3(3): 385-388.
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    It is shown that all known fits to NN scattering based on Van der Waal's model disagree with the recent slope parameter data at 540 GeV.An assessment of the model is made.
  • Mohammad Saleem, Fazal-e-Aleem
    理论物理通讯. 1984, 3(3): 389-391.
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    The recently measured differential, elastic and total cross section for ≡-P elastic scattering at 102 and 135 GeV/c have been fitted by using simple Regge pole model with phenomenological residue fmctions.
  • 胡敏, 何祚庥, 吴礼金
    理论物理通讯. 1984, 3(3): 393-398.
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    The ionized Lifetime of the hydrogen negativeion in a uniform electric field is again calculated by using improved perturbation theory.The choice of the H--ion wave function and the normalization of wave function of continuous state are discussed. The numerical calculations by using Rotenberg-Stein wave function with five parameters are performed. Comparison of our results with experimental results obtained by G. M. Stinson et al. is given.