The v-v energy transfer of highly vibrationally excited states (I)

The relaxation of the highly vibrationally excited CO (v = 1–8) by CO₂ is studied by timeresolved Fourier transform infrared emission spectroscopy (TR FTIR). 193 nm laser photolysis of the mixture of CHBr₃ with O₂ generates the highly vibrationally excited CO(v) molecules. TR FTIR records the intense infrared emission of CO(v→v-1). The vibrational populations of each level of CO(v) have been determined by the method of spectral simulation. Based on the evolution of the time resolved populations and the differential method, 8 energy transfer rate constants of CO(v = 1–8) to CO₂ molecules areobtained: (5.7±0.1), (5.9±0.1), (5.2±0.2), (3.4±0.2), (2.4±0.3), (2.2±0.4), (2.0±0.4) and (1.8±0.6) (10¹⁴ cm³ · molecule⁻¹ · s⁻¹), respectively. A two-channel energy transfer model can explain the feature of the quenching of CO(v) by CO². For the lower vibrational states of CO, the vibrational energy transfers preferentially to the u³ mode of CO² For the higher levels, the major quenching channel changes to the vibrational energy exchange between CO(v→v-1) and the u¹ mode of CO².     

The v-v energy transfer of highly vibrationally excited states (II)

The vibrational energy transfer from highly vibrationally excited CO to H₂O molecules is studied by time-resolved Fourier transform infrared emission spectroscopy (TR FTIR). Following the 193 nm laser photolysis of CHBr₃ and O₂ the secondary reactions generate CO(v). The infrared emission of CO(v → v−1) is detected by TR FTIR. The excitation of H₂O molecules is not observed. By the method of the spectral simulation and the differential technique, 8 rate constants for CO(v)/H₂O system are obtained: (1.7 ±0.1), (3.4 ±0.2), (6.2 ±0.4), (8.0 ±1.0), (9.0 ±2.0), (12 ±3), (16 ±4) and (18 ±7) (10¹³cm³ · molecule^-1· s^-1). At least two reasons lead to the efficient energy transfer. One is the contributions of the rotational energy to the vibational energy defect and the other is the result of the complex collision. With the SSH andab initio calculations, the quenching mechanism of CO(v) by H₂O is suggested.     

皮秒激光在充气毛细管中四波混频的理论描述

建立了描写皮秒激光在充气毛细管中四波混频过程的耦合方程组．利用这个耦合方程组对最近的毛细管中差频过程的实验结果给出了新的理论说明．发现采用三阶非线性极化率大的介质是进一步提高信号光强度的重要途径．     

一种新型多元均相时间分辨荧光免疫分析方法的建立

制备出具有光学特异性的3种不同颜色量子点纳米微球和铽螯合物，分别与CEA、AFP和HBsAg的两株抗体偶联，采用双抗体夹心法模式，充分利用两株抗体与抗原的相互作用，通过采集不同量子点发出的荧光信号，根据其信号的强弱判定标记在量子点纳米微球上的抗体结合的抗原的量，从而实现多元待分析物的定性定量分析．结果表明，量子点的荧光信号与CEA、AFP和HBsAg抗原浓度呈线性关系，其函数分别为：lgY-2．79173＋0．915841gX（R-0．99808）、lgY-3．69543＋0．456441gX（R=0．99848）和lgY-4．12898＋0．409451gX（R=0．99845），分析灵敏度分别为：0．44、0．24和0．02ng／mL．     

利用小角X射线散射研究蛋白质在球形聚电解质刷中的吸附

通过小角X射线散射(SAXS)技术研究了牛血清蛋白(BSA)在阳离子球形聚电解质刷(SPB)中的吸附及分布规律。随着BSA质量浓度的增加,其在SPB中的分布均匀递增,直至达到饱和吸附;随着pH的增大,BSA在刷子层中的分布呈现从靠近核逐渐外移扩散到溶液中的变化趋势。此外,用时间分辨SAXS技术观察到在极短的时间(12s)内BSA在SPB中的动态吸附及再分布的显著变化过程。研究结果表明:SAXS技术在原位表征蛋白质在SPB中的动态分布方面具有其他表征技术不可替代的优势。     

Excitation energy transfer mechanisms in allophycocyanin (I)

The mechanisms of excitation energy transfer within allophycocyanin monomer with the theory of generalized master equation (GME) and the technique of time-resobed fluorescence anisotropic spectroscopy are studied. In the case of known information of its structure and spectra, the theory applied is based on the assumption that the coupling interaction between two chromophores is fairly weak. The theory correctly predicts the experimentlly observed rate for excitation energy transfer in allophycocyanin monomer. Based on the results, the energy transfer mechanism can be described as Förster and these processes cannot take place from the high vibrational levels of donor to acceptor.     

相变存储器单元皮秒测试信号完整性研究

针对相变存储器皮秒测试系统由于矩阵开关电路分布参数以及信号通道中阻抗突变所引起的反射,严重影响了皮秒脉冲信号的完整性,使施加在相变单元上的皮秒脉冲信号严重失真,为了消除失真,改善信号完整性,从2个方面提出了解决方案：一是采用性能优良的高频继电器构成矩阵开关;二是减小反射,采取了源端阻抗匹配、负载分支端阻抗补偿、菊花链双线拓扑结构等措施,使得反射的影响减小到最小.理论分析与仿真结果表明：皮秒脉冲信号波形质量良好,满足测试要求.本测试系统为研究皮秒编程脉冲作用下相变存储器的存储机理、速度、可靠性等提供了良好的平台,也可作为电阻式随机擦写存储器单元测试系统.     

微纳米薄膜材料中激光皮秒超声的数值模拟

基于双温模型和热弹性耦合理论,采用有限元方法,针对A1/Si3N4和A1/Si3N4/Si两种层状薄膜材料中激励皮秒超声,建立激光飞秒超声的有限元数值模型,得到A1薄膜中电子和晶格的温度场,进而分析薄膜内部的应变和表面位移响应.对比研究了双温模型理论和傅里叶热传导理论的计算,结果表明皮秒超声研究采用双温模型求解温度场更为合适,数值分析得到应变具有幅值较小且波形展宽的结果.表面位移响应峰的形成是超声波在薄膜材料界面处发生反射引起的.