Mycielski图的BBC染色

基于图G的Mycielski图M（G）,研究xb（G,TG）与xb（M（G）,T’）之间的关系以及xb（G,TG）与xb（M（G）,T＂）之间的关系,其中Tc为G的生成树,T’,T＂分别为M（G）的两类特殊生成树．并给出当G为二部图,完全图以及Halin图时,Xb（M（G）,T＂）的值．     

JSOG中水蒸汽含量的模拟计算

氧碘化学激光（简称 COIL）系统中，水是影响激光功率输出的最重要的原因之一。气流中的水不仅对激发态碘原子有严重的猝灭作用，另外对碘分子解离、超音速流动特性也有很坏的负面作用。单重态氧发生器的BHP（Basic Hydrogen Peroxide ）溶液是最主要的水蒸汽源。利用传质模型对射流式单重态氧发生器（简称JSOG）中产生的水蒸汽进行了计算，所得的数值结果与实验测量结果基本相符。根据模拟结果，对发生器的设计及实验条件进行了优化。     

电化学在ICF靶制备中的新应用

报道了近年来在电解加工技术制备理论密度金属薄膜和电沉积技术制备金属纳米丝阵列材料等领域取得的进展。采用硫酸+甲醇电解液体系获得了表面粗糙度小于30nm的钛膜。采用阳极氧化铝模板电沉积技术制备出长度约10μm、直径约300nm的金纳米丝阵列。主要讨论了电解液配方及电解加工参数的选择,金属纳米丝直径与长度的控制等问题。     

薄膜-泡沫复合平面调制靶的制备

利用浇注法制备了具有正弦波调制图纹的溴代聚苯乙烯薄膜,并在此基础上将低密度聚-4-甲基-1-戊烯(PMP)泡沫溶胶浇注在薄膜调制图纹的表面,从而得到了薄膜-泡沫复合平面调制靶样品。较为详细的讨论了具有正弦波调制图纹的复合平面调制靶的制备方法并通过台阶仪、显微镜观测了薄膜表面条纹的起伏以及薄膜-泡沫截面的复合情况,实验结果发现,采用此种方法得到的复合平面调制靶样品,其薄膜厚度、泡沫密度易于控制,薄膜、泡沫调制界面清晰,易于微靶的加工与装配。     

高质量多孔氧化铝模板的制备

在草酸电解液中研究了阳极氧化法制备多孔氧化铝模板(AAO模板)。采用场发射扫描电子显微镜对多孔模板的形貌进行表征,结果表明:模板孔的分布均匀有序,孔径在40~70 nm;电解液浓度、氧化电压、氧化温度和氧化时间都会影响模板的形态;不经过高温退火及抛光也可以制得规则排布的多孔AAO模板。X射线衍射分析表明:氧化铝膜的主要成分为非晶态Al2O3。     

Linear optical implementation of optimal unambiguous discrimination among quantum states

In this paper, we present a linear optical scheme for optimal unambiguous discrimination among nonorthogonal quantum states in terms of the multiple-rail and polarization representation of a single photon. In our scheme, discriminated quantum states are expressed by using the spatial degree of freedom of a single photon while the polarization degree of freedom of the single photon is used to act as an auxiliary qubit. The optical components used in our scheme are only passive linear optical elements such as polarizing beam splitters, wave plates, polarizers, single photon detectors, and single photon source.     

超低密度琼脂-明胶复合泡沫的研制

在探讨体系凝胶温度、冷冻速率、干燥温度及真空度等影响泡沫微观结构诸因素的基础上，确定出了琼脂－明胶复合泡沫制备工艺参数。以水作溶剂，成功地制得了密度≤1.0mg/cm^3,孔径≤100μm的琼脂－明胶泡沫；以水／1，4－二氧环己烷作混合溶剂，成功地制得了密度≤2mg/cm^3,孔径≤30μm的琼脂－明胶泡沫。热重－差热（TG－DSC）分析发现，琼脂－明胶复合泡沫的热稳定性可达－200℃。     

Linear Optical Implementation of Quantum Clock Synchronization Algorithm

We propose optical implementation for the quantum clock synchronization （QCS） algorithm by using only linear optical elements. Our method is based on the single photon representation of qubits. Two kinds of linear optical realization schemes, i.e,, the location-plus-polarization-qubit scheme and the all-location-qubit scheme, are proposed, respectively. Linear optical realizations of three-qubit and four-qubit QCS algorithm are explicitly presented.     

气袋靶制备技术

为了研究柱腔内气体对激光-等离子体相互作用及内爆对称性的影响,详细给出了气袋靶制备及其在神光-Ⅱ靶场的应用情况。对气袋靶的靶型设计、靶材料选择及薄膜制备和充气工艺进行了系统的研究。制备的气袋靶主要由厚度为400 nm的聚酰亚胺薄膜和厚度为400 m的铝支撑环构成,利用装配在支撑环上的充气管实现对气袋靶的充气,当充气完成后,整个气袋靶膨胀为球状。     

Fringe visibility for two qubits interacting with a macroscopic medium

We study both the two-particle and single-particle fringe visibility in the generalized version of the Nakazato–Pascazio model where two qubits interact with a finite length one-dimensional array.Both the two-particle and single-particle fringe visibilities are investigated with different initial states of the particles spin.For different initial states of the particles spin,the two-particle fringe visibility either decreases or increases over time,and may even decrease first and increase later.Due to the interaction between the particles and the one-dimensional array,the single-particle fringe visibility increases over time when the initial state of the two particles spin is independent.The single-particle fringe visibility is equal to 0 as the two-particle spin is initially in the completely entangled state or in the singlet state.