On the isomorphisms and automorphism groups of circulants

Denote byC _n(S) the circulant graph (or digraph). LetM be a minimal generating element subset ofZ _n, the cyclic group of integers modulon, and In this paper, we discuss the problems about the automorphism group and isomorphisms ofC _n(S). When M S , we determine the automorphism group ofC _n(S) and prove that for any T if and only ifT = S, where is an integer relatively prime ton. The automorphism groups and isomorphisms of some other types of circulant graphs (or digraphs) are also considered. In the last section of this paper, we give a relation between the isomorphisms and the automorphism groups of circulants.     

Almost all Cayley graphs are hamiltonian

It has been conjectured that there is a hamiltonian cycle in every finite connected Cayley graph. In spite of the difficulty in proving this conjecture, we show that almost all Cayley graphs are hamiltonian. That is, as the order n of a groupG approaches infinity, the ratio of the number of hamiltonian Cayley graphs ofG to the total number of Cayley graphs ofG approaches 1.Supported by the National Natural Science Foundation of China, Xinjiang Educational Committee and Xinjiang University.     

Strange Quark Matter and Strangelets in a Strong Magnetic Field

We study the stability properties of magnetized strange quark matter and strangelets under a strong magnetic field in the MIT bag model. The free energy per baryon of strange quark matter feels a great influence from the magnetic field. At the field strength about 10¹⁷G, the magnetized strange quark matter becomes more stable. Considering the finite size effect, the magnetic influence on strangelets becomes complicated. For a given magnetic field, there exists a critical baryon number, below which the magnetized strangelets have lower energy than the non-magnetized strangelets. For the field strength of 5× 10¹⁷G, the critical baryon number is A_c ～ 100. Generally, the critical baryon number increases with the decreasing external magnetic field. When the field strength is smaller than 10¹⁷G, the critical baryon number goes up to A_c～ 10⁵. The stable radius, electric charge, and quark flavor fractions of magnetized strangelets are shown.     

超强激光场物理学

首先,评述了超强激光场的理论结果;其次,描述了超短光脉冲在密的气体和光学介质传播中的自作用;第三,评述了强场离化无碰撞等离子体中高度离化的离子产生,及高功率超短激光脉冲巨大强度的电场可用于电子加速;第四,分析了超短声脉冲和无线电脉冲的产生和应用,讨论了在不同条件下,激光辐射谐波和 Ｘ 射线激光的产生,进一步评述了超强激光脉冲与凝聚靶相互作用可以产生接近星体物质参数的高温、超密、强磁场和巨大压力等离子体;最后,简要叙述了激光激发核、核反应,高能电子─光子相互作用的可能效应及可能进行的实验。     

RIBLL束流诊断

描述了兰州放射性离子次级束流线(RIBLL)上研制并安装使用的放射性束流(RIB)诊断装置的种类、结构、性能及在AIBLL上的位置和功能.重点叙述了以光纤为基础的几种诊断元件,它们探测效率高、响应时间快、制作容易、性能稳定.给出了RIB¹⁷N等高图,说明诊断装置辅助MBLL得到RIB的水平.     

基于CAN 总线技术的PSM 电源远程控制通信系统

为提高HL-2A 装置辅助加热系统脉冲阶梯调制(PSM)电源的运行效率和操作可靠性,设计并实现了一种基于CAN 总线技术的远程控制通信系统。该系统采用载有SJA1000CAN 总线控制器的PCI 板卡以及TMS320F2812 微处理器分别作为上位机和下位机的通信终端,结合用户界面程序,实现了HL-2A 受控核聚变装
置辅助加热电源的远程控制,提高了其整体控制性能和操作效率。     

在立方织构的Ni基带上沉积掺Ag的YBCO超导薄膜

用脉冲激光沉积法在立方织构的Ni基片上成功地外延了YBCO超导薄膜 ,其临界电流密度高达 1 .1 5MA cm² .X射线衍射分析结果表明Ni CeO₂ YSZ YBCO多层结构都是c轴取向 ,CeO₂ 和YSZ缓冲层能有效地改进薄膜织构 ;扫描电子显微镜结果表明Ni CeO₂ YSZ YBCO结构所有生长层面存在类似层状的形貌 ,而薄的一层Ag膜能有效地填充各个生长阶段由于高温下热膨胀系数不匹配形成的微裂缝 ,其结果是改进了薄膜微观结构 ,提高了临界电流密度 .     

熊猫光纤的结构与双折射特性关系研究

本文用微元算法研究了熊猫光纤的结构参量对熊猫光纤双折射特性(拍长)的影响.由实验数据拟合出了计算拍长的熊猫光纤掺杂区的有效热膨胀系数.计算结果表明,熊猫光纤的猫眼半径、猫眼与纤芯的距离、猫眼的不一致等都是影响拍长的因素.所得结果对熊猫光纤的制作提供了理论指导.     

半导体泵浦YAG自锁模谐振腔研究

分析半导体泵浦ＹＡＧ自锁模谐振腔的特性,讨论晶体长度,凸面镜焦距和谐振腔长度对自锁模的影响,获得了对谐振腔设计及腔参数优化有用的结论。     

Widely tunable continuous-wave Raman laser in diatomic hydrogen pumped by an external-cavity diode laser

What is to the authors' knowledge the first experimental demonstration of a nonresonant cw Raman laser pumped by a tunable external-cavity diode laser (ECDL) is presented. The ECDL is phase-frequency locked to a high-finesse Raman laser cavity containing diatomic hydrogen (H(2)) by the Pound-Drever-Hall locking technique. The Stokes lasing threshold occurs at a pump power of 400 +/- 30 muW, and a maximum photon conversion efficiency of 12.0 +/- 1.3% is achieved at 1.6 mW of pump power. A 40-nm tuning range of the cw Stokes emission, 1174-1214 nm, is obtained by tuning of the wavelength of the ECDL pump source.