LD预泵浦条件与Cr4+,Nd3+:YAG微片激光器的输出特性

 建立了LD预泵浦的被动调Q平平腔Cr⁴⁺,Nd³⁺:YAG微片激光器模型,分析了预泵浦参数与激光脉冲时间特性的关系,设计了LD预泵浦的Cr⁴⁺,Nd³⁺:YAG微片激光器实验,测量了不同预泵浦参数下激光单脉冲以及脉冲序列的时间特性。实验结果与数值计算结果基本符合：调节预泵浦参数使每个泵浦脉冲刚好对应输出单个激光脉冲时,固定脉冲泵浦宽度,脉冲泵浦速率随连续泵浦速率的增加呈一次函数减小;固定连续泵浦速率,脉冲泵浦速率随脉冲泵浦宽度的增加呈非线性函数减小。结果还表明,激光脉冲半高全宽随整体泵浦速率的增加而减小,峰值功率随整体泵浦速率的增加而增加;当整体泵浦速率在阈值附近变动时,激光单脉冲时间特性的变化最为明显。     

Demonstration of three-dimensional electrostatic trapping of state-selected Rydberg atoms

A three-dimensional trap for Rydberg atoms in selected Stark states has been realized experimentally. H atoms seeded in a supersonic expansion of Ar are excited to the low-field seeking n=30, k=25, |m|=0, 2 Rydberg-Stark states, decelerated from a mean initial velocity of 665 m/s to zero velocity in the laboratory frame and loaded into a three-dimensional electrostatic trap. The motion of the cold Rydberg atom cloud in the trap and the decay of the trapped atoms have been studied by pulsed electric field ionization and imaging techniques.     

Enhancement in Thermoelectrical Power Factor of N-Type Si80Ge20 Alloys

Influences of the carrier concentration and mobility of heavily doped n-type Si80 Ge20 alloys on the thermoelectrical power factor are investigated. The experimental results indicate that thermoeleetrieal power factors of 32- 36μWem-1K^-2 eouM be consistently achieved with carrier concentrations of 2.1-2.9 × 10^20cm^-3 and carrier mobilities of 36-40 cm^2 V^-1s^-1. However, many samples with suitable carrier concentrations do not always have high mobilities and high power factors. Some possible explanations for this behaviour are discussed.     

Conical Emission Patterns by Femtosecond Pulses with Different Spectral Bandwidths

Different conical emission （CE） patterns are obtained experimentally at various incident powers and beam sizes of pump laser pulses with pulse durations of 7fs, 44fs and 100fs. The results show that it is the incident power but not the incident power density that determines a certain CE pattern. In addition, the critical powers for similar CE patterns are nearly the same for the laser pulses with the same spectral bandwidth. Furthermore, as far as a certain CE pattern is concerned, the wider the spectral bandwidth of pump laser pulse is, the higher the critical power is. This will hopefully provide new insights for the generation of CE pattern in optical medium.     

How to test atom and neutron neutrality with atom interferometry

We propose an atom-interferometry experiment based on the scalar Aharonov-Bohm effect which detects an atom charge at the 10{-28}e level, and improves the current laboratory limits by 8 orders of magnitude. This setup independently probes neutron charges down to 10{-28}e, 7 orders of magnitude below current bounds.     

迁移时间归一化法改善毛细管电泳表征中药大黄的重现性

探讨了迁移时间归一化法改善中药毛细管电泳分析迁移时间重现性的原理,并将其应用于实际样品的分析。迁移时间归一化法认为,在相同的操作电压、缓冲液组成和温度条件下,多次电泳实验中迁移时间产生差别的主要原因是多次电泳实验中电渗流产生了差异。迁移时间归一化法就是通过选择电泳谱图中的一个或两个峰作为标记峰,将各次电泳实验的迁移时间都归一到第一次电泳实验中的迁移时间。比较多次电泳实验中迁移时间(t)的相对标准偏差(RSD)、经单峰归一化处理的迁移时间(t′)的RSD、经双峰归一化处理的迁移时间(t″)的RSD、迁移时间比(t/tistd,istd代表所选择的标记物)的RSD,发现RSD(t″)相似文献   

氮的氧化物系列实验再探究与再思考

从教二十多年,我们发现人们对氮的氧化物一些重要实验的认识,还不十分到位;某些经典实验的设计和操作,需要进行再反思.现将一些认为有益的想法和做法,付诸文字,与同仁作探讨和交流.     

戊二醛交联前后明胶微球热转变研究

在空气和氮气气氛中,对未交联的明胶微球(GMs)和戊二醛交联明胶微球(CGMs)进行了受热转变研究,并利用250℃热处理的明胶球制备出具有多孔内核的明胶基结构.经过热重分析(TGA)、差示扫描量热法(DSC)、扫描电子显微镜(SEM)和付里叶变换红外光谱(FTIR)等分析测试表明:戊二醛交联明胶微球300℃后热失重略大于未交联明胶微球,两者的熔化温度Tm都为228℃;在空气中250℃热处理7 h的未交联明胶微球经过稀硫酸处理后可以得到多孔内核结构,多孔内核含碳、氧元素,外壳以碳元素为主;105℃和190℃热处理的明胶球化学成分基本相同,250℃热处理使明胶分子中的酰胺键减少、并发生三级结构的转变.     

2-苯基-5-芳基-1,3,4-噁二唑的合成与表征

苯甲酸乙酯与水合肼反应制得苯甲酰肼(1),1再分别与芳酰氯反应制得N、N′-二酰基肼(3a～3i),3a～3i在POCl3作用下脱水环化生成2-苯基-5-芳基-1,3,4-噁二唑(4a～4i)。其结构经元素分析,IR,^1H NMR和MS表征,并对其裂解途径进行了探讨。     

THE MULTI-FOLD COMMUTATOR OF VARIATION OF POTENTIAL IN CHIRAL MODEL AND SDYM FIELD

The multi-fold commutaror representation of hidden symmetry algebra in principal chiral model and the self-dual Yang-Mills field is explicitly shown. All the variations are taken with respect to the potential A_ξ other than field quantity g for principal chiral model in defining the usual operator Q(ξ,η) to give the G⊗c(t) algebra.