1,3,5,7-四甲基氟硼二吡咯甲川的合成、晶体结构及密度泛函理论研究

以2,4-二甲基吡咯、原甲酸三乙酯以及对甲苯磺酸为原料,无溶剂下合成了1,3,5,7-四甲基对甲苯磺酸二吡咯甲川(T1);以T1、三氟化硼乙醚以及三乙胺为原料,无溶剂下合成了1,3,5,7-四甲基氟硼二吡咯甲川(F1)。利用1H NMR和X射线单晶衍射对其进行了表征。结果表明:T1属于单斜晶系,P21/c空间群,晶胞参数为a=0.777 3(3)nm,b=1.518 5(5)nm,c=1.612 2(5)nm,β=91.923(12)°,V=1.901 9(11)nm3,Z=4;F1属于单斜晶系,P21/n空间群,晶胞参数为a=0.775 02(1)nm,b=1.444 20(3)nm,c=1.174 35(2)nm,β=107.779 5(9)°,V=1.251 65(4)nm~3,Z=4。在4种不同溶剂中,测定了T1的紫外可见光谱、F1的紫外可见光谱和稳态荧光光谱。将密度泛函计算与前线轨道理论相结合,研究了T1和F1可能的衍生方式。     

芳基噻唑胺类化合物合成及其抑菌活性研究

为了获得低毒、高效、环境友好的小分子植物病原真菌抑制剂,本文合成了22个芳基噻唑胺类衍生物,并采用抑制菌丝生长速率法测试了化合物对九种常见植物病原真菌的抑制作用。活性测试结果表明,目标化合物2p、2q和2s具有优异的广谱性抑菌活性,其抑制率为41.1～99.5%,显著优于商品化抑菌剂噁霉灵(25.4～86.5%)和百菌清(24.7～71.4%)。构效关系研究表明：在噻唑胺结构中引入萘环和含有卤素取代的芳环时有利于其抑菌活性的提高。此研究为后期基于芳基噻唑胺骨架的农用抑菌剂开发提供了理论指导。     

醇系溶剂中冠醚与碱金属离子的配位反应

The enthalpy changes, entropy changes and equilibrium constants of coordination reactions of 18-crown-6 with the alkali ions Na+ and K+ at 298.15K were measured by using RD-496 microcalorimeter with methanol, ethanol, n-propanol and n-butanol as solvents respectively. The results indicated that the enthalpy changes △rHm, entropy changes △rSm, and the stability of the complexes are closely related with the polarity of the solvents, and the order of the stability is ethanol>methanol>n-propanol>n-butanol>H2O for the same complex in the solvents investigated. The stability order was reasonably explained by relating the stability constants of the complexes with the dielectric constants of these solvents, and by using the model of solvated-desolvated ions and ion pair in the coordination reactions.     

酰胺型冠醚液晶的合成及性质研究

冠醚液晶出现至今仅十几年，由于其具有冠醚和液晶的各种性质而受到人们的关注［‘－‘1．我们在已有工作的基础上，设计合成了5种酸胺型冠醚液晶分子（4—8），其中3种分子（4－6）具有液晶性．合成路线如下：1结果与讨论合成样品4－8经IR、MS、‘HNMR和元素分析确证其结构．用DSC和Texture图测定了4－6的液晶性质，其结果见图1．化合物7、8无液晶性，分子长径比分别为5．8：I，满足一般律状向列液晶分子长径比的要求．当在其分子链中增加1个苯环（5、6）时，分子的刚性链比例增大，整个分子的刚性增加，则具有液晶性．双臂型冠醚液…     

长周期波导光栅窄带光滤波器特性的模拟

利用两路平行的刻有长周期光栅(LPWG)波导间耦合的理论模型,研究了LPWG波导光滤波器,利用弱耦合实现高耦合效率和窄带滤波的方法,设计了一个窄带光滤波器。仿真结果表明,在1 530~1 560 nm范围,能实现单一的带通、带阻互补滤波输出,3 dB带宽为1 nm,耦合效率高达98%。     

牛血清白蛋白与金霉素结合反应的机制研究

以光谱技术与微量热技术相结合的方法研究水溶液中金霉素与牛血清白蛋白分子间结合作用的热力学性质 .荧光猝灭法测得该反应的结合常数K =2 .0 9× 10 5L/mol,结合位点数n =1.75 ,微量法测得反应的焓变△rHm=- 17.5 0kJ/mol;依据Forster非辐射能量转移机制 ,得到授体 受体间的结合距离 (r1=1.6 7nm ,r2 =1.4 6nm)和能量转移效率 (E1=0 .4 1,E2 =0 .6 6 ) .金霉素与牛血清白蛋白分子间有较强的结合作用 ,且结合力以疏水作用为主 .     

T1—2212超导薄膜的制备

以铝酸镧晶体为基片，采用两步法制备T1-2212超导薄膜，包括在低温(150℃)下利用激光脉冲沉积(PLD)工艺沉淀Ba2CaCu2Ox非晶前驱体薄膜和在高温(740～830℃)下前驱体薄膜的铊化结晶、取向生长过程，实验结果表明所制得的膜的相组成为T1-2212，表面存在大量均匀分布的成分为T12Ba2CaCu2Ox的亚微米颗粒，其零电阻温度为101K，薄膜与基片之间界面清晰，没有过渡层，薄膜具有良好的c取向外延条纹。     

低杂波波谱的下移和可近性条件

本文利用改进磁面位移计算的射线轨迹Ｃｏｄｅ，研究在射线轨迹的第圈ｎ的下移以及下移量与各等离子体参量的关系。我们发现等离子体密度越高，波的频度越低，ｎ的下移量越大。计算表明：在射线的第一圈ｎ下移量的最大值大致与ｎ＾－ｅ／「ｆ＾１．５ｑ（ｒｃ）」成正比、也与电流、密度的分布和ｎ的初值等有关。     

Broadband chirped InAs quantum-dot superluminescent diodes with a small spectral dip of 0.2 dB

We report on the fabrication and characterization of InAs/GaAs chirped multilayer quantum-dot superluminescent diodes (CMQD-SLDs) with and without direct Si doping in QDs. It was found that both the output power and the spectral width of the CMQD-SLDs were significantly enhanced by direct Si doping in the QDs. The output power and spectral width have been increased by approximately 18.3% and 40%, respectively. Moreover, we shortened the cavity length of the doped CMQD-SLD and obtained a spectral width of 106 nm. In addition, the maximum output power and spectral width of the CMQD-SLD doped directly with Si can be further increased to 16.6 mW and 114 nm, respectively, through anti-reflection coating and device packaging. The device exhibited the smallest spectral dip of 0.2 dB when the spectrum was widest. The improved performances of the doped CMQD-SLD can be attributed to the direct doping of Si in the QDs, optimization of device structure and device packaging.     

Long-Range Interactions between Nematicons

We theoretically and experimentally investigate the long-range interaction between nematicons. It is demonstrated that the interaction becomes strongest when the pretilt angle of liquid crystal molecules is nearly π/4 for a given single-beam input power P0, and that the interaction becomes stronger when the incident power Po increases at a given pretilt angle. In this way, the interaction is still observed when the initial separation is 43 times of the soliton width, much larger than that implemented in lead glasses [Nature Phys. 2 （2006） 769].