线聚焦激光辐照Al靶所产生的紫外X射线谱线

本文叙述了采用线聚焦激光幅照Al靶所产生的高离化态离子的紫外X射线(XUV)谱线。利用Cowan的原子能级程序计算了不同离化态的离子谱线的波长和振子强度gf,辨认出140条离子谱线,其中有82条新谱线。 关键词：     

聚合反应制备键合型纤维素-三(4-甲基苯基甲酸酯)衍生物类手性固定相

合成了带有甲基丙烯酰基的纤维素-三(4-甲基苯基甲酸酯)衍生物(CTMB),并通过聚合反应将其键合在具有双键的硅胶表面,得到手性固定相(CSP)。用所得到的CSP对9种对映体化合物(丁苯酞、酮基布洛芬、反-2,3-二苯环氧乙烷、安息香、安息香类似物、托葛尔碱、华法令、4,4′-二甲氧基-5,6,5′,6′-二次甲二氧基-2,2′-羰甲基甲酯联苯、4,4′-二甲氧基-5,6,5′,6′-二次甲二氧基-2-羰甲基甲酯-2′-羰甲基乙酯联苯)进行了拆分。考察了CSP制备过程中甲基丙烯酰氯的用量、键合方式以及硅胶     

压力诱导发光未来可期

科技创新的根源是基于基础科学研究的提升,而"从0到1"的突破是需要长期的积累和灵感的。本文讲述了发现压力诱导发光这一新现象的思想和材料设计。     

电子顺磁共振“AsGa”的光淬灭行为与EL2亚稳态机理

根据Goltzene等人最近关于原生LEC,HB,压缩变形和中子辐照GaAs中电子顺磁共振(EPR)“As_Ga”谱低温光淬灭实验结果,结合Baraff和Schlüter最近关于EL2亚稳态的理论计算,本文认为可进一步证实作者之一在1981年提出的EL2(As_GaV_AsV_Ga)缺陷模型,同时还对Wager和Van Vechten最近提出的EL2(As_GaV_AsV_Ga)的亚稳态机理加以评述和修正。 关键词：     

低能离子注入形成氮化硅薄膜特性的研究

低能离子束与表面相互作用主要呈现溅射、注入等现象。本文研究了在1.35keVN₂⁺离子注入形成氮化硅的特性,并研究了注入和溅射的并存过程。在高剂量、低能(<10keV)注入的情况下,提出了有效剂量的概念,并建立了刻蚀速率、射程与有效注入剂量的关系。还用俄歇电子能谱(AES)、X射线光电子能谱(XPS)、透射电子显微镜(TEM)、背散射分析(RBS)测定了薄膜的有关特性。 关键词：     

靶丸支撑膜对ICF内爆性能影响的模拟研究

使用二维多群辐射扩散流体力学程序LARED-S,模拟研究靶丸支撑膜在惯性约束聚变氘氘（DD）气体靶内爆过程中的扰动演化过程及其对内爆性能的影响.二维模拟表明：靶丸支撑膜显著降低DD气体靶内爆的中子产额,二维模拟产额为一维结果的55.2%.内爆性能下降的主要物理机制是支撑膜使靶壳生成大幅度的尖钉深入DD气体区,使烧蚀层与DD气体之间物质界面处的电子热传导漏失功率显著增大,导致DD核反应速率显著降低,中子反应速率峰值时刻（bang-time时刻）提前.相比一维理想内爆的模拟结果,支撑膜引入的扰动显著降低bang-time时刻DD气体压强与内爆动能转化为DD气体内能的效率,壳层剩余动能相应大幅增加.     

大鼠肝微粒体中盐酸度洛西汀的RP-HPLC测定

建立大鼠肝微粒体中盐酸度洛西汀的RP-HPLC测定方法,为其体外代谢研究奠定基础.盐酸度洛西汀与大鼠肝微粒体共孵育后,用甲醇沉淀蛋白.离心上清液,采用HP1100色谱系统,以甲醇-0.025mol·L-1磷酸二氢钾缓冲盐(62∶38,V/V,pH 3.5)为流动相,流速0.9mL·miD -1,进样量20μL,经Hedera ODS-2(4.6mm×250mm,5μm)色谱柱分离,检测波长290nm.盐酸度洛西汀在0.4-16μg·mL-1范围内线性关系良好(r=0.9992),检测限为40ng·mL-1,定量限为0.2μg·mL-1,方法回收率在94.4％-105.0％之间,日内、日间精密度分别＜5％和＜10％(n=5).本方法较为快速,灵敏,准确,可用于盐酸度洛西汀在大鼠肝微粒体中的体外代谢研究.     

单摆摆球运动轨迹控制装置

设计了单摆摆球运动轨迹控制装置,该装置由摆线指针、摆线定位板组成.使用控制装置可以准确、快速调节单摆的平衡位置和摆动角度,保证摆球在平行于角度尺的铅垂平面内运动.     

Generation of Entanglement Between Two Noninteracting Qubits via Interaction with Nonclassical Radiation Field

We study the interaction between a single-mode quantized field and a quantum system composed of two qubits. We suppose that two qubits initially be prepared in the mixed and separable state, and study how entanglement between two qubits arises in the course of evolution according to the Jaynes-Cummings type interaction with nonclassical radiation field. We also investigate the relation between entanglement and purity of qubit subsystem. We show that different photon statistics have different effects on the dynamical behavior of the qubit subsystem. When the qubits are initially prepared in the maximally mixed and separable state, for coherent state field we cannot find entanglement between two qubits; for squeezed state field entanglement between two qubits exists in several short period of time; for even and odd coherent state fields of large photon number, the dynamical behavior of the entanglement between two qubits shows collapse and revival phenomenon. For odd coherent state field of small photon number, the entanglement with both qubits initially prepared in maximally mixed state can be stronger than that with both qubits initially prepared in pure states. For fields of small photon number, the entanglement strongly depends on the states they are initially prepared in. For coherent state field, and odd and even coherent state fields of large photon number, the entanglement only depends on the purity of the initial state of qubit subsystem. We also show that during the evolution the unentangled state may be purer than the entangled state, and the maximum degree of entanglement may not occur at the time when the qubit subsystem is in the purist state.     

Ab initio calculations on the ground and excited states of InI

Potential energy curves (PECs) of the ground and the low-lying excited states of the InI molecule are computed using the internally contracted multireference singles and doubles configuration interaction with the Davidson correction (ic-MR-CISD + Q) method based on the relativistic effective core potentials (RECPs). The spectroscopic constants are obtained, including the excitation energy (T _e), the equilibrium bond distance (R _e), the dipole moment (μ_e) and the vibrational constants (ω_e and ω_e). Finally, we predict the transition dipole moments, the radiative lifetimes, and the Franc-Condon factors for the transitions of A³Π₀+ ? X¹Σ₀ ⁺ and B³Π^l ? X¹Σ₀ ⁺,. The results reveal that A³Π₀+ and B³Π_l are long-lived states with the lifetimes being of the order of microseconds.