Theoretical study of the intensity of chemically induce dynamic electron polarization of radical-triplet pairs

Considering the interaction between encited triplet molecule and cloublet radical,based on the second-order perturbation theroy and the motion equation of density matrix,the polarzation intersity of RTPM were theoretically calculated with the overpopulated doublet spin states and quartet spin states of radical0triplet paris as initial conditions the radical result from the zero-field-splitting(zfs)and the multiplet A/E and E/A polarization result from hyperfine (hf) interactions of the triplet molcule,The hyperfine ralated A A/E or E E/A CIDEP on the radical were the overpopulation of the net abscrptive or emissive polarization and multiple A/E or E/A polarization.     

Properties of cat mutually pumped phase conjugation and two-wave mixing gain in doped KNSBN

Cat mutually pumped phase conjugation configuration is discovered and investigated by using two-wave mixing in (KyNa1-y)2z(SrxBa1-x)1-zNb2O6 (KNSBN) crystal. When only one signal or pumped beam does not give birth to phase conjugation, the maximum reflectivity of signal and pumped beam attain 140% and 30% due to two-wave mixing, respectively. The experimental results show that the two-wave mixing can reduce the threshold of incident beams power, extend the incident angle range, and shorten response rate in the process of self-pumped phase conjugator (SPPC) in KNSBN crystal.     

Evolution property of soliton solutions for the Whitham－Broer－Kaup equation and variant Boussinesq equation

Using the standard Painlevé analysis approach, the (1+1)-dimensional Whitham－Broer－Kaup (WBK) and variant Boussinesq equations are solved. Some significant and exact solutions are given. We investigate the behaviour of the interactions between the multi-soliton-kink-type solution for the WBK equation and the multi-solitonic solutions and find the interactions are not elastic. The fission of solutions for the WBK equation and the fusions of those for the variant Boussinesq equation may occur after their interactions.     

Effect of S Substitution for P Point Defects in KDP Crystals： First-Principles Study

The electronic structure and geometric distribution of phosphor replaced by sulfur in potassium dihydrogen phosphate （KDP） are investigated by first-principles calculations. The point defect narrows down the energy gap to about 4.9eV, corresponding to a two-photon absorption of 355nm after correction. This can explain the decrease of the laser damage resistance in KDP crystals. Moreover, the defects twist the crystal structure and weaken bonds, especially the O-H bonds, so these bonds may be the first sites to crack under laser irradiation.     

扰流板结构参数对冲击波衰减特性影响的仿真分析

在坑道内设置扰流板是加速爆炸冲击波衰减的有效方法。为探究扰流板结构参数对冲击波衰减特性的影响,采用ANSYS/LS-DYNA有限元软件进行仿真研究。基于流固耦合算法,建立Schardin实验等比模型,所得仿真结果与实验结果具有良好的一致性,验证了仿真模型的有效性。以某发射井坑道为研究对象,在矩形扰流板宽度一定的情况下,研究了扰流板厚度、倾角及间距对冲击波衰减规律的影响。结果表明:保持其他参数不变,随着扰流板厚度增加,冲击波超压衰减越来越明显;扰流板厚度为40cm时,倾角为105°、间距为6m最有利于冲击波衰减。研究结果可以为坑道防护设计提供有价值的参考。     

引力的"磁性"是怎么回事

爱因斯坦广义相对论的重要结论之一是引力也应有“磁”分量，两个旋转物体之间会有引力“磁”矩的相互作用．而按牛顿引力论，两个物体的引力只决定于二者的质量，并不与二者旋转运动方向有关．因此，检验是否存在引力“磁”分量，乃成为区别牛顿引力论与广义相对论的关键之一．检验的方法是利用旋转物体，例如，在空间放置一个陀螺，按牛顿理论。     

HL-2A装置主机真空性能的改善

HL-2A装置真空室内部件数目繁多，容器本体上的密封部位多达几百个，特别是真空室内多极场线圈真空套从真空室的预装阶段开始，经常会出现一些漏气问题，此问题在原ASDEX运行时就是一个棘手的问题，已进行了多次修补。大部分漏点均发生在厚度仅为约0．2mm的波纹管上，无法采用氩弧焊接，所有这些漏点的修补均采用无铅焊料通过钎焊工艺完成。     

变截面杆共轴撞击数值分析及其应用前景

 为对弹性杆共轴撞击这一应力波基础问题进行扩展研究,基于非线性动力学软件LS-DYNA建立了有限元模型,分析了共轴撞击的变截面杆的形态参数对波形的影响规律,探讨了应力波产生的机理,并对其应用前景进行了展望。结果表明,由于变截面效应,一定形态参数的变截面杆共轴撞击可以得到具备波阵面平滑上升,较长的前沿升时和消除了波形振荡等特性的应力波;该特性是变截面杆撞击这一过程的内在属性,主要由变截面段的最小半径控制,变截面段长度仅对局部形态产生影响,对加载速度的变化不敏感;半无限长的变截面杆共轴撞击规律可在应力波加工等领域应用。由此可见,该规律对基础性理论进行了扩展,应用前景广阔。     

LiNbO3晶体在室温—130℃的锥光干涉及折射率的异常

研究了纯及掺杂LiNbO₃(下简写为LN)晶体z向通光的锥光干涉图。纯LN,在45℃和75℃附近,双折射率均有异常变化,晶体由单轴变为双轴晶。掺杂(Fe,Cr,Cu)LN也有类似的变化,但变化的温度范围被加宽。分别测量了折射率n₀和n_e,在这两个温度附近有异常跳变。通过与x方向加电场的室温锥光图相比较,可以认为在75℃附近的双折射异常变化是相当于离子位移在x方向产生10⁵V/m量级的内电场所引起的。 关键词：     

波导程差透镜的制作与特性研究

<正> 一、引言光波导透镜是基本的光波导元件之一。已经报道过许多处理方法,有的与体光学相联系,有的取自微波学方法。在光波导中,实现聚焦的一个途径是在平面衬底上先做一个球面凹坑,随后在整个衬底表面(包括凹坑部分)上做成波导。这个凹坑区就叫做波导程差透镜。其截面示意图画在图1中。在这种形式的波导透镜中,存在几个问