ENTIRE CHROMATIC NUMBER AND △-MATCHING OF OUTERPLANE GRAPHS

Let G be an outerplane graph with maximum degree A and the entire chromatic number Xvef（G）. This paper proves that if △ ≥6, then △＋ 1≤Xvef（G）≤△＋ 2, and Xvef （G） = △＋ 1 if and only if G has a matching M consisting of some inner edges which covers all its vertices of maximum degree.     

Optical Waveguide Formed in RbTiOPO4 Crystal by 6.0 MeV O^3＋ Implantation

A planar optical waveguide was formed in RbTiOP04 crystal by 6.0-MeV oxygen ion implantation with the dose of 2 × 10^15 ions/cm2 at room temperature. Annealing at 200℃ for 30min in air is performed to improve the thermal stability of the waveguide. The dark modes of the waveguide are measured at wavelengths 633 and 1539 nm, respectively. The refractive index profiles in the guiding layer are reconstructed by using the reflectivity calculation method. TRIM＇98 code was carried out to simulate the damage profiles caused by the implantation process to obtain a better understanding of the waveguide formation.     

化学分析中的某些现象

叙述了日常化学分析中所遇到的某些特殊现象,提出了一些解释并展开了讨论     

Ion－Implanted Waveguides in a Nd^3＋－Doped Silicate Glass

Monomode enhanced-index Nd^3 -doped silicate glass waveguides fabricated by ion implantation are reported.The Nd^3 -doped silicate glass was implanted by 3.0 MeV B^ ions, 3.0 MeV 0^ ions and 4.5 MeV Ni^2 ions,respectively. A prism-coupling method was carried out to measure dark modes in the Nd^3 -doped silicate glassusing a model 2010 prism coupler. The moving fibre method was applied to measure the waveguide propagationloss. After a moderate annealing, the 3.0-MeV B^ -ion implanted waveguide loss is about 3.54 dB/cm; the 3.0-Me V O^ -ion implanted waveguide loss is about 5.36 dB/cm; and the 4.5-MeV the Ni^2 -implanted waveguide lossis about 7.55dB/cm. The results show that with the increasing ion mass, the loss in implanted waveguide isincreased.     

Intra-beam scattering studies for low emittance at BAPS

The target parameters of modern ultra-low emittance storage ring light sources are entering into a regime where intra-beam scattering (IBS) becomes important and, in the case of the Beijing Advanced Photon Source (BAPS), which is being designed at the Institute of High Energy Physics (IHEP), even a limitation for achieving the desired emittances in both transverse planes at the diffraction limit for X-ray wavelengths (≈10 pm). Due to the low emittance, the IBS effect will be very strong. Accurate calculations are needed to check if the design goal (ε_h+ε_v=20 pm) can be reached. In this paper, we present the results of numerical simulation studies of the IBS effect on a BAPS temporary design lattice.     

影响激光加热运动圆柱体的加热线型的分析

 采用几何分析的方法研究激光加热运动圆柱体的过程，在说明加热线型的概念和意义后，讨论了在地平面上各点处所具有的加热线型的时间宽度，从而指出，为了激光有效加热运动圆柱体，激光器应当怎样在地平面上放置的原则。即根据激光器有效工作时间与圆柱体抛射时间的比例关系选择一定的相对时间宽度等值线，以此等值线为界在地平面上划出一有效区域，并从中选取距离轨道最近的点作为激光器的放置点。当考虑大气对激光的衰减作用时，激光以小于一定入射角阈值进行动态加热的总能量将出现极大值，在此处放置激光器最有利于动态加热。     

Preparation and Decoherence of Two-Atom Entangled States in a Dissipative Cavity

We present a scheme for generating four pairs of two-atom Einstein Podolsky-Rosen （EPR） states using the simultaneous interaction of the two atoms with a single-mode cavity field under a large detuning condition. The influence of cavity dissipation on the prepared EPR states is investigated by means of the superoperator method and the state fidelity. It is shown that some kinds of the prepared EPR states are robust against cavity dissipation and the intensity of the field, and maintain their entanglement invariance, and the others are fragile and completely destroyed by the action of cavity dissipation and the intensity of the field in the long-time limit. Decoherence time of the fragile entangled states is extremely small for a typical cavity-QED experimental data.     

^229Ra的衰变纲图

用１４ＭｅＶ中子轰击钍靶，通过＾２３２Ｔｈ（ｎ，α）＾２２９Ｒａ反应产季了＾２２９Ｒａ，由放射化学分离技术从被照靶物质中分离出＾２２９Ｒａ活性，利用γ（Ｘ）谱学方法，首次观测到了＾２２９Ｒａ的能量为１４．５，１５．６，１８．８，２１．８，２２．５，４４．０，４７．５，５５．０，６３．０，６９．６，９３．６，９４．１，９８．５，１０２．２，１０４．５，１０６．１，１６１．１和１７１．５ｋｅＶ的１８条