离散可激发介质中早期后去极化对螺旋波影响的数值研究

通过考虑某些不应态也可以被激发,在离散可激发介质Greenberg-Hasting模型中引入早期后去极化行为,研究了早期后去极化对螺旋波的影响.数值结果表明:在适当选择参数下,早期后去极化对螺旋波有很大影响,这些影响包括使螺旋波漫游、漂移和破碎,导致螺旋波波纹被扭曲和波臂粗细交替变化,以及导致螺旋波的周期在两个值之间交替变化,产生从稳定螺旋波到呼吸螺旋波和反螺旋波的相变等.当不应态的激发阈值很高时,早期后去极化对螺旋波没有影响.对发生上述现象作了简要的讨论. 关键词： 离散可激发介质 螺旋波 早期后去极化     

Enhanced Spin Depolarization and Storage Time in a Rb Vapor

The experiment of measuring the spin depolarized time and light storage time in a Rb vapor under different conditions is performed. Typically, these measurements are accomplished in three different containers： atoms in a bare glass cell, atoms in a buffer gas cell, and atoms in a tetracontane （C4oH82） coating cell. The increasing depolarization and storage times are observed in both the buffer gas cell and the tetracontane coating cell. In the latter case, a storage time greater than 400μs is obtained.     

并联铁电体冲击去极化输出电流实验和计算

 为分析不同数量铁电体的输出电流特征,进行了多片并联PZT95/5铁电体冲击去极化实验,测量了电阻负载下铁电体的输出电流;建立了并联铁电体输出电流的计算模型,计算了并联铁电体的输出电流。通过比较计算和实验结果,分析了铁电体数量和冲击波状态对铁电体输出电流的影响。结果表明：若进入铁电体的冲击波为平面波,铁电体输出电流的波形接近方波,电流峰值随铁电体并联数量的增加成比例增加,冲击波波形和侧向稀疏波对铁电体输出电流波形和去极化率有很大的影响。     

电流反馈示波极谱滴定法

本文提出了电流反馈示波极谱滴定法的原理、仪器装置及操作技术。为了提高去极剂切口的灵敏度, 可将dE/dt信号转换为电流信号后再反馈回电解池以补偿充电电流,一般可将切口灵敏度提高1至5倍, 图形分辨率也较经典方法高, 从而使滴定终点的变化更为敏锐, 扩大了示波极谱滴定的应用范围, 推导了电流反馈的交流电流极化理论公式, 分析了电流反馈对示波极谱图形、去极剂切口灵敏度及切口电位的影响。     

Error Tolerance in Constructing Cluster States

We consider the problem often encountered in constructing large cluster states, that is, the σx measurements in the depolarizing noise, and present a regulation to calculate the error propagation and the accumulation. Rohde et al. first pointed out the question [Phys. Rev. A 75 （2007） 010302（R）]. A quantitative analysis is given on the disadvantage influence of the probabilistic gate and noisy environment on the construction of two-dimensional （213） scalable cluster states. Positivity of partial transpose criteria is used to predict whether the final state is distillable or not. A critical value on the error tolerance in constructing cluster states is determined, which could be used as a test-bed for successful construction of scalable 2D cluster states. Furthermore, our quantitative analysis would also be helpful to find optimal approach to suppress the noise accumulation.     

Effects of Depolarization Field and Interfacial Coupling on the Polarization of Ferroelectric Bilayers

A ferroelectric bilayer model considering depolarization field and interfacial coupling is proposed and the expression of the depolarization field is derived. The spatial profiles of spontaneous polarization and hysteresis loops are calculated using the numerical method with and without considering the depolarization field. The effects of the depolarization field and interfacial coupling on the polarization of second-order ferroelectric bilayers are studied systematically. When interfacial coupling is ferroelectric coupling, the interface spontaneous polarization increases and the area of hysteresis loop becomes larger with increasing coupling. When interfacial coupling is antiferroelectric coupling, the depolarization field makes the central loop become smaller and the shape of the hysteresis loop becomes steep. Meanwhile, as interfacial coupling increases, the outer loops stretch further out horizontally and the size of the central loop widens.     

光子晶体光纤中去极化型声波导布里渊散射频移和散射效率研究

利用矢量有限元法,数值模拟了不同结构参数下光子晶体光纤中空气孔填充率与去极化型声波导布里渊散射频移的关系,以及布里渊散射频移与布里渊散射效率的关系。研究结果表明,空气孔填充率的增大会导致扭转径向模式的去极化型声波导布里渊散射频移下移。空气孔节距或纤芯直径一定时,高阶模式的频移对空气孔填充率的变化更为敏感。扭转径向模式的去极化型布里渊散射效率都随布里渊散射频移的增大而增大。     

光子晶体光纤中去极化型声波导布里渊散射频移和散射效率研究

利用矢量有限元法,数值模拟了不同结构参数下光子晶体光纤中空气孔填充率与去极化型声波导布里渊散射频移的关系,以及布里渊散射频移与布里渊散射效率的关系。研究结果表明,空气孔填充率的增大会导致扭转径向模式的去极化型声波导布里渊散射频移下移。空气孔节距或纤芯直径一定时,高阶模式的频移对空气孔填充率的变化更为敏感。扭转径向模式的去极化型布里渊散射效率都随布里渊散射频移的增大而增大。     

光子晶体光纤中去极化声波导布里渊散射温度及应变响应

数值求解了光子晶体光纤中的去极化型声波导布里渊散射色散方程,研究了光子晶体光纤中的布里渊频移随泵浦波长及空气孔填充率的变化关系,以及去极化型声波导布里渊散射频移随温度、应变、声波导模式、纤芯直径及空气孔层数的关系。结果表明:布里渊频移随着波长的增大而线性减小。对于相同的波长点,增大光子晶体光纤空气孔填充率时,声波横向速度将会减小。去极化型声波导布里渊散射频移随温度及应变的增大而线性增加。同一温度条件下,高阶TR2m模式的去极化型声波导布里渊散射频移对温度的变化更为敏感;而在同一应变条件下,低阶TR2m模式的去极化型声波导布里渊散射频移对应变的变化更为敏感。去极化型声波导布里渊散射频移随纤芯直径的增加而增大,随空气孔层数的增加而减小。