Structural,energetic and thermodynamic analyses of Ca(BH4)2·2NH3 from first principles calculations

Ca(BH₄)₂·2NH₃ is a relatively new compound with potential application in hydrogen storage. Here the fundamental properties of the compound, such as electronic structure, energetic and thermodynamic properties, were comprehensively studied using first-principles calculations. Results from electronic density of states (DOS) and electron localization function (ELF) indicate the covalent bond nature of the N–H bond and the B–H bond. Charge density analyses show weak ionic interactions between the Ca atom and the NH₃ complexes or the (BH₄)^? complexes. The calculated vibration frequencies of B–H and N–H are in good agreement with other theoretical and experimental results. Furthermore, we calculated the reaction enthalpy and reaction Gibbs free energy at a range of temperature 0–700 K. Our results are in good agreement with experimental results in literature. Possible reaction mechanism of the decomposition reaction is proposed.     

Reversible Control of Fluorescence Based on the Interaction Among CdTe QDs, CHA and Ang I

在水相中合成了巯基丙酸( MPA)包覆的CdTe量子点(QDs),采用透射电子显微镜和原子力显微镜对其进行表征.利用荧光光谱、紫外-可见吸收光谱和红外光谱研究了CdTe QDs与绿原酸(CHA)的相互作用.结果表明,CHA可显著猝灭CdTe QDs的荧光,在一定的浓度范围内,荧光猝灭值与CHA的浓度呈现一定的线性关系.推断其主要猝灭机理为动态猝灭,并实现了荧光光谱法测定CHA.向CdTe QDs-CHA体系中加入血管紧张素Ⅰ (Ang Ⅰ)后,CdTe QDs荧光在一定浓度范围内逐渐恢复,从而实现了CdTe QDs的荧光可逆调控.CdTe QDs荧光的猝灭与恢复过程对于荧光传感的设计以及荧光可逆调控机理的研究具有指导意义.     

高效液相色谱-质谱联用法检测免疫抑制剂及其合并用药

建立高效液相色谱-质谱联用法同时测定人血浆中免疫抑制剂及合并用药12种药物浓度的方法.选用Kromasil-C18色谱柱(50 mm× 4.6 mm×5 μm),以甲醇-乙腈-1mmol/L乙酸铵溶液为流动相,采用梯度洗脱进行分离,样本用甲醇沉淀蛋白后进样,流速:1.1 mL/min;柱温:35℃;进样量:20μL.选用3200QTrap型液相色谱-串联质谱仪的多反应监测(MRM)扫描方式进行检测.12种药物的线性范围为0.2～1000μg/L;定量下限为0.2 μg/L.准确度与精密度结果显示方法日间、日内RSD均小于15％;相对偏差-13％～9.33％,稳定性较好.本方法快速、灵敏,专属性强、重现性好,可用于人体血浆中免疫抑制剂及其常用合并用药共12种药物浓度的测定.     

Y_2O_2S:Eu~(3+)空心微球的制备与性能

以单分散的碳球为硬模板,采用均匀共沉淀法合成了Y_2O_2S:Eu~(3+)心微球.通过XRD、SEM、TEM、荧光光谱对其进行表征.X射线衍射测试表明所制备的Y_2O_2S:Eu~(3+)空心微球为单相,六方晶.扫描电子显微镜(SEM)和透射电子显微镜(TEM)测试表明所制备的Y_2O_2S:Eu~(3+)空心微球粒径小,分布均匀.激发和发射光谱测试表明Eu~(3+)离子能有效地掺入硫氧化钇基质中,并具有良好的发光性能.     

Y2O2S∶Eu3+空心微球的制备与性能

以单分散的碳球为硬模板,采用均匀共沉淀法合成了Y2O2S:Eu3+心微球.通过XRD、SEM、TEM、荧光光谱对其进行表征.X射线衍射测试表明所制备的Y2O2S:Eu3+空心微球为单相,六方晶.扫描电子显微镜(SEM)和透射电子显微镜(TEM)测试表明所制备的Y2O2S:Eu3+空心微球粒径小,分布均匀.激发和发射光谱测试表明Eu3+离子能有效地掺入硫氧化钇基质中,并具有良好的发光性能.     

2D Green’s functions for semi-infinite orthotropic thermoelastic plane

Based on the 2D general solutions of orthotropic thermoelastic material, the Green’s function for a steady point heat source in the interior of semi-infinite orthotropic thermoelastic plane is constructed by three newly introduced harmonic functions. All components of coupled field in semi-infinite thermoelastic plane are expressed in terms of elementary functions. Numerical results are given graphically by contours.     

石墨烯层间纳米摩擦性质的第一性原理研究

基于密度泛函理论的第一性原理计算方法研究了纳米尺度下石墨烯层间摩擦现象, 探讨了对称和非对称两种情况下双层石墨烯层间沿不同方向的摩擦性质. 研究发现对于对称的双层石墨烯, 层间摩擦沿不同方向同性; 摩擦因数依赖于正压力, 随正压力增大, 摩擦因数的变化曲线分为三个阶段, 在较小以及较大压力下, 摩擦因数遵循Amonton法则不随压力变化而变化; 而在中间3-6 nN阶段, 摩擦因数随压力增加线性增加. 整个研究压力范围内摩擦因数在0.05-0.25之间. 对于非对称性双层石墨烯层间摩擦, 不同压力下摩擦因数在0.006上下波动, 摩擦因数较两层对称性石墨烯大大降低. 上述研究结果与实验一致.     

ZnO压敏陶瓷的介电谱

在-160℃-200℃温度范围内、0.1 Hz-0.1 MHz频率范围内测量了 ZnO压敏陶瓷的介电频谱, 发现可以采用电导率谱低频端的类直流特性来表征晶界Schottky势垒的电子输运过程, 获得的Schottky势垒高度为0.77 eV. 基于背靠背双Schottky势垒模型, 提出当存在直流偏压时, 势垒高度将随直流偏压线性增大. 基于此势垒模型计算了ZnO压敏陶瓷单晶界的直流偏压大小, 进而计算出晶粒平均尺寸为6.8 μm, 该理论值与通过扫描电子显微镜断面照片获得的测量值的偏差在5%以内. 可见采用介电谱不但可以获得势垒高度实现电气性能的表征, 还能获得晶粒尺寸实现显微结构的表征.     

弹性薄壳的建模与控制研究进展

介绍近十几年来薄壳的建模与控制研究所取得的一系列重要进展.主要内容包括对具有任意形状中面以及不同物理背景的3种经典薄壳——浅壳、Naghdi壳和Koiter壳的坐标卡无关的数学模型的建立以及这些模型的边界精确能控性、边界反馈镇定和适定正则性方面的研究成果.     

Reduced linewidth enhancement factor due to excited state transition of quantum dot lasers

The carrier induced refractive index change and linewidth enhancement factor α due to ground-state (GS) and excited-state (ES) transitions have been compared by measuring the optical gain spectra from an InAs/GaAs quantum dot (QD) laser structure. It is shown that the ES transition exhibits a reduced α-factor compared to the value due to the GS transition. This result can be explained by the α-factor due to the ES transition having a smaller increase from the non-resonant carriers in the combined state of the wetting layer and InGaAs strain reducing layer than the α-factor increase due to the GS transition, since the relaxation time for carriers from the combined state of the wetting layer and InGaAs strain reducing layer to the ES is shorter than to the GS. The result reported here shows another advantage of using ES QD lasers for optical communication, in addition to their higher modulation speed.