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Table of contents

    20 April 1993, Volume 2 Issue 4 Previous issue    Next issue
    GENERAL
    ASYMPTOTIC EXPANSION OF GREEN FUNCTION OR HEAT KERNEL IN SPACE WITH TORSION
    XU DIAN-YAN (许殿彦), XU XIAO-FENG (许晓风)
    Acta Physica Sinica (Overseas Edition), 1993, 2 (4):  241-247.  DOI: 10.1088/1004-423X/2/4/001
    Abstract ( 1244 )   PDF (113KB) ( 342 )  
    An algorithm for asymptotic expansion of Green function or heat kemel in space with torsion is proposed. The De Witt-Seeley-Gilkey coeffcient E2(x) is calculated.
    A DEMONSTRATION OF 1×8 LINEAR ARRAY YBCO TRANSITION EDGE IR BOLOMETER
    LIU XIN-TIAN (刘心田), SHI BAO-AN (石保安), YANG DE-JIA (杨德嘉), CHEN ZHAO-JIA (陈兆甲)
    Acta Physica Sinica (Overseas Edition), 1993, 2 (4):  248-251.  DOI: 10.1088/1004-423X/2/4/002
    Abstract ( 1093 )   PDF (91KB) ( 437 )  
    A high-Tc superconducting array microbolometer has been fabricated by using a YBCO film. Optical measurements gave moderate performance as individual detector, but singnificant improverment appears possible.
    CLASSICAL AREAS OF PHENOMENOLOGY
    ATOMIC-COHERENCE-INDUCED ENHANCEMENT OF REFRACTIVE INDEX
    LUO ZHEN-FEI (罗振飞), XU ZHI-ZHAN (徐至展), ZHOU JIAO-YANG (周骄阳)
    Acta Physica Sinica (Overseas Edition), 1993, 2 (4):  252-259.  DOI: 10.1088/1004-423X/2/4/003
    Abstract ( 963 )   PDF (180KB) ( 379 )  
    The influences of lower-level coherence in atomic medium of $\Xi$-type energy-level scheme on the absorption and dispersion are studied in dressed states. It is found that a weak probe light of a certain fre-quency can be free of atomic absorption, and at the same time has a large index of refraction.
    PHYSICS OF GASES, PLASMAS, AND ELECTRIC DISCHARGES
    RESISTIVE EFFECT ON ION FISHBONE MODE IN TOKAMAK PLASMA
    SHI BING-REN (石秉仁), J.W.VANDAM, R.CARRERA, Y.Z.ZHANG
    Acta Physica Sinica (Overseas Edition), 1993, 2 (4):  260-269.  DOI: 10.1088/1004-423X/2/4/004
    Abstract ( 1157 )   PDF (221KB) ( 469 )  
    A consistent theoretical description of the resistive internal mode is presented to discuss the effect of resistivity on fishbone mode for different parameter regimes of bulk and hot components. We find that the ideal fishbone mode theory ceases to be correct for the low frequency fishbone branch, the so-called ion fishbone mode, which has a real frequency very dose to $\omega$*i (the diamagnetic frequency) in marginal state. The stability domain analysis in ($\hat{\beta}$h, $\hat{\gamma}$mhd) space based on the resistive dispersion relation shows that the transition between the stable and unstable regions is much more complicated than predicted by the ideal limit theory. Another salient feature of the resistive fishbone mode is the existence of a weakly unstable regime. For high frequency fishbone with $\omega$≈$\omega$dm (the toroidal precession frequency of the hot ions), resistivity has negligible effect and the ideal theory is correct.
    CONDENSED MATTER: STRUCTURAL, MECHANICAL, AND THERMAL PROPERTIES
    STUDIES ON THE RELATIONSHIPS BETWEEN THE STRUCTURE AND THE LOCALIZED ENERGY STATES OF POLY (ETHYLENE TEREPHTHALATE) ELECTRETS
    ZHANG XING-YUAN (张兴元), ZHOU YI-QIN(周漪琴)
    Acta Physica Sinica (Overseas Edition), 1993, 2 (4):  270-279.  DOI: 10.1088/1004-423X/2/4/005
    Abstract ( 1083 )   PDF (302KB) ( 405 )  
    A series of poly(ethytene terephthalate) (PET) films with different degrees of planar orientation [$\Delta$(xy)z], crystallinity (Xc) and molecular weights were prepared by drawing biaxially, annealing at 110℃ and $\gamma$-imadiation of 0.5-4MGy. The peaks of localized energy states were separated from the detrapping cur-rent curves by means of poling temperature scanning method of themally stimulated current. The depth of localized energy levels enlarged with the rise of $\Delta$(xy)z, Xc and $\gamma$-inadiation dose. The kinds of structural defects increased because of the changes of orientation structure of chains, crystalline structure and molecular chain structure, which caused the number of localized states to increase from 2 to 6 and the distribution width of the depth of localized levels to broaden.
    ORDER ALLOY IN GexSi1-x/Si(100) STRAINED-LAYER SUPERLATFICES
    YU SHI-DONG (余是东), LI QI (李齐), FENG DUAN (冯端), YU MING-REN (俞鸣人), CHU YI-MING (褚一鸣)
    Acta Physica Sinica (Overseas Edition), 1993, 2 (4):  280-285.  DOI: 10.1088/1004-423X/2/4/006
    Abstract ( 1289 )   PDF (206KB) ( 440 )  
    The GexSi1-x/Si(100) strained-layer superlattices have been investigated by means of the transmission electron microscopy of the cross-sectional specimen (XTEM) and the high resolution electron microscopy (HREM), The order alloy with a period of modulation twice as large as the lattice constant alongzone axis has been found in the alloy layers of the superlattices with x≈0.4-0.5. This order struc-ture makes the superlattices inhomogeneously strained. The result of the compuler simulation shows that the order alloy exhibits an altemating stack of 2 monolayers of Ge atoms and 2 monolayers of Si atoms along thezone axis. Thc calculated elastic strain energy of the disorder alloy reported in the litera-ture is very close to that of the order alloy alongzone axis. Thus, during the MBE growth of the alloy layers, both the disorder and order alloys can be formed alongzone axis.
    CONDENSED MATTER: ELECTRONIC STRUCTURE, ELECTRICAL, MAGNETIC, AND OPTICAL PROPERTIES
    PROPERTIES OF PROPAGATION OF GUIDED ELECTRON WAVES IN COUPLED ASYMMETRIC QUANTUM WELLS
    YUAN SHI-QI (袁世齐), GU BEN-YUAN (顾本源)
    Acta Physica Sinica (Overseas Edition), 1993, 2 (4):  286-299.  DOI: 10.1088/1004-423X/2/4/007
    Abstract ( 1001 )   PDF (411KB) ( 318 )  
    In this article we investigate the properties of the propagation of guided electron waves in the coupled asymmetric quantum wells. By decomposing the eigenfunctions of electron in the coupled double quantum wells in terms of the basis eigenfunctions of the individual wells, the expression of the mode amplitude func-tions for various bare states in wells has been given. By setting up appropriate boundary conditions one can simulate different injecting manners of electron into the system and study how the electron waves trans-fer among various states. The major electron wave transfer happens between the matching bare states in wells. The particular pattern of the transfer depends on the injecting manner and the energy of the inci-dent electron. We also show the influence of the presence of the multimodes on the variatinn of the mode amplitude functions. It leads to producing some oscillations imposed on the original sinusoidal-like func-tions and causing incomplete transfer between a pair of states in channels due to the beating frequency effect or the interference among various modes.
    SIZE EFFECT OF INNER RADIUS ON CIRCULARLY SYMMETRIC SOLITON STATES IN ANNULAR JOSEPHSON JUNCTIONS
    XU KUN-MING (徐昆明), LU DAO-FANG (陆道芳), YAO XI-XIAN (姚希贤)
    Acta Physica Sinica (Overseas Edition), 1993, 2 (4):  300-310.  DOI: 10.1088/1004-423X/2/4/008
    Abstract ( 1027 )   PDF (295KB) ( 434 )  
    The effect of the inner radius of an annular Josephson junetion on the excitation of circularly symmetric soliton states is explored by direct numerical simulation. In a circularly symmetric annular Josephson junction (CSAJJ hereafter), the phase difference in the order parameters $\Phi$ across the junction bar-rier obeys the modified sine-Gordon equation (SGE) in which there is a perturbation term $\Phi$p/$\rho$ inversely proportional to the radial coordinate $\rho$. and this term does not appear in the case of a 1D in-line junc-tion. The effect of the $\Phi$p/$\rho$ term becomes prominent when $\rho$ is small. It turns out that for junctions of grven dissipation and annular width, there is a lower limit of the inner radii for the junctions to support stable soliton motion, while the lower limit depends strongly on the dissipation coefficient $\alpha$. For example, for a CSAJJ with inner radius 5$\lambda$J, outer radius 10$\lambda$J, no stable soliton states would exist when $\alpha$=0.01 or $\alpha$=0.02. However, for 0.06≥$\alpha$≥0.03, there are ring-shaped solitary wave solutions, presumably because the dissipation suppresses the effect of the $\Phi$p/$\rho$ term. Finally, the behaviour of the seliton states and the rele-vant I-V characteristics are also disscussed.
ISSN 1674-1056   CN 11-5639/O4
, Vol. 2, No. 4

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