飞秒啁啾脉冲放大系统中折叠反射式望远镜对脉冲波前的影响

推导出飞秒激光啁啾脉冲放大系统中使用的折叠反射式望远镜对脉冲波前的影响. 分析和计 算了波前倾斜与反射式望远镜参数之间的关系.结果发现：当脉冲宽度小于100 fs时，波前 倾斜对光束质量的影响不可忽略，并提出了抑制这种脉冲波前倾斜的有效方法. 关键词： 飞秒激光啁啾脉冲放大 波前倾斜 反射式望远镜     

用力敏传感器测液体表面张力系数的误差分析

分析了采用力敏传感器测量液体表面张力系数实验误差的主要来源，给出了计算公式和测量结果，并提出了改进建议．     

Near threshold photodetachment cross section of negative atomic oxygen ions

A 40-target state close-coupling calculation for the photodetachment cross section of negative atomic oxygen near threshold is carried out with core－valence electron correlation by using the R-matrix method. It was shown that after considering the excitations of two electrons from the 2s shell, the electron affinity of O^- (2s^22p^5{}^2P°) agrees with the experimental result much better than that just considering the excitations of electrons only from the 2p shell as well as only one electron from the 2s shell. Total cross section as well as the main contribution of the ionization channels to the partial cross section are illustrated to show the structure near threshold clearly.     

溶胶-凝胶SiO2薄膜氨热两步后处理

 以正硅酸乙酯为前驱体,氨水作催化剂,采用溶胶-凝胶法提拉镀制SiO₂双面膜,对薄膜进行氨处理和热处理。采用椭偏仪、分光光度计、红外光谱、扫描探针显微镜、静滴接触角测量仪表征薄膜的特性。研究表明：经氨热两步后处理,膜厚持续减小,折射率经氨处理先增大了0.236,再经热处理又减小了0.202,膜层透光性变好,透过率峰值持续向短波方向移动;经两步后处理的膜面平整度明显变好,与水的接触角先增大到58.92°后减小到38.07°。     

枯草杆菌在淀粉液态培养基中生产α-淀粉酶

以枯草杆菌(Bacillus subtilis BF7658)为实验菌株,以淀粉为主要原料,采用液态培养基发酵,生产α-淀粉酶。结果表明:在23℃至44℃内,培养基起始pH值为自然pH值,产酶最佳培养温度为37℃;枯草杆菌在淀粉液态培养基中控制温度为37℃,振荡培养,其产酶最适宜淀粉与水组成比例为:75∶100;在最佳温度37℃下,淀粉∶水为75∶100时,最佳培养时间为36h。     

激发态Cs原子间碰撞能量转移截面

在Cs蒸气密度为1013?cm-3量级范围内,研究了6P3/2+6P3/2→6DJ+6S碰撞能量合并过程.利用单模半导体激光器共振激发6P3/2态,利用另一与泵浦激光束反向平行的单模激光束作为吸收线探测激发态原子密度及其空间分布,吸收线调至6P3/2→8S1/2跃迁,并可平行于泵浦激光束移动.由激发态原子密度和谱线的荧光强度比得到碰撞能量合并的截面.碰撞转移到6D5/2和6D3/2的截面分别是(4.1±1.8)×10-15和(2.2±1.0)×10-15?cm2.与其它实验结果进行了比较.     

碱木素的近红外光谱吸收机理的研究

通过碱木素模型物对醌、邻醌和香兰素的溶液在800～900 nm的近红外光谱波段内的吸收谱图的对比发现,对醌和邻醌在此波段产生较强的吸收,而香兰素基本上没有吸收,证明了碱木素的醌型结构在800～900 nm波段内产生特征吸收。对银杏和夹竹桃磨木木素碱处理前后的溶液在800～900 nm波段内的吸光度的差别分析,发现夹竹桃的磨木木素的吸光度的相对变化更大,这是由于夹竹桃磨木木素经碱处理后产生了更多的醌型结构。这也是在硫酸盐法蒸煮过程中在800～900 nm波段内阔叶材的蒸煮液吸光度大于针叶材的蒸煮液吸光度的主要原因。     

Rb（5PJ）＋Rb（5PJ）→Rb（5JS）＋Rb（nl=5D，7S）碰撞能量合并

研究了Rb(5PJ)+Rb(5PJ)→Rb(nlJ')+Rb(5S)碰撞能量合并过程,利用单模半导体激光器分别共振激发Rb原子的5P1/2或5P3/2态,利用另一与泵浦激光束反向平行的单模激光束作为吸收线探测激发态原子密度及其空间分布,吸收线分别调至5P1/2→5D3/2和5P3/2→7S1/2跃迁.由激发态原子密度和谱线荧光比得到碰撞能量合并过程的截面,对5P3/2激发,碰撞转移得到5D5/2,5D3/2和7S1/2的截面分别是(1.32士0.59)×10-14,(1.18士0.53)×10-14和(3.21士1.44)×10-15cm2;对5P1/2激发,碰撞转移到5D5/2和5D3/2的截面分别是(6.57士2.96)×10-15和(5.90士2.66)×10-15cm2.与其他的实验结果进行了比较.     

Improved data analysis method of single-molecule experiments based on probability optimization

To extract the dynamic parameters from single molecule manipulation experiments, usually lots of data at different forces need to be recorded. But the measuring time of a single molecule is limited due to breakage of the tether or degradation of the molecule. Here we propose a data analysis method based on probability maximization of the recorded time trace to extract the dynamic parameters from a single measurement. The feasibility of this method was verified by dealing with the simulation data of a two-state system. We also applied this method to estimate the parameters of DNA hairpin folding and unfolding dynamics measured by a magnetic tweezers experiment.     

磁瓶式光电子能谱和速度成像光电子能谱对APS-(A=C14H10,蒽)的研究:电子结构,APS·的自旋轨道耦合和APS-的自旋偶极态

Gaseous dibenzo-7-phosphanorbornadiene P-sulfide anions APS^-(A=C₁₄H₁₀ or anthracene) were generated via electrospray ionization, and characterized by magnetic-bottle photoelectron spectroscopy, velocity-map imaging (VMI) photoelectron spectroscopy, and quantum chemical calculations. The electron affinity (EA) and spin-orbit (SO) splitting of the APS^· radical are determined from the photoelectron spectra and Franck-Condon factor simulations to be EA=(2.62±0.05) eV and SO splitting=(43±7) meV. VMI photoelectron images show strong and sharp peaks near the detachment threshold with an identical electron kinetic energy (eKE) of 17.9 meV at three different detachment wavelengths, which are therefore assigned to autodetachment from dipole-bound anion states. The B3LYP/6-31++G(d,p) calculations indicate APS^· has a dipole moment of 3.31 Debye, large enough to support a dipole-bound electron.