1,3,5,7-四甲基-2,6,8-三乙基吡咯甲川-BF2络合物的合成及晶体结构

合成了标题化合物 ,借助于元素分析、红外光谱、核磁共振氢谱、质谱以及X 射线单晶衍射等分析方法确定了它的结构。该化合物属于三斜晶系 ,空间群为P-1(No 2 ) ,化学式 :C19H2 7BF2 N2 。晶胞参数 :a =1 2 2 5 7( 2 ) ,b=1 7830 ( 8) ,c=0 8877( 2 )nm ,α =10 0 2 6 ( 2 ) ,β =10 7 5 7( 1) ,γ =76 96 ( 2 )°,V =1 7892( 9)nm3 ,Mr=332 2 4,Z =4,Dc=1 2 33g·cm-3 ,μ(MoKα) =0 86cm-1,F( 0 0 0 ) =712 0 0 ,R =0 0 5 1,Rw=0 0 6 0。化合物中除 2 ,6 ,8位的三个甲基 (C( 12 ) ,C( 15 ) ,C( 18) )和氟原子 (F( 1) ,F( 2 ) )外 ,其余非氢原子近似组成一个大平面结构。在对其晶体结构进行详细分析的基础上 ,我们还初步讨论了它的分子结构与光谱及激光性能的关系。     

温度对晶体中稀土离子(E)-型能级电磁感应透明的影响

运用产经典理论，在Pr^3 ：YSO晶体Pr离子E－型三级级系统中，求解了探测光吸收在不同光跃迁驰豫速率与自旋跃迁驰豫速率下的瞬态及稳态解，得到了电磁感应透明现象，分析了两种驰豫对电磁感应透明的,人而揭示了掺稀土离子晶体中电磁感应透明对温度的依赖性。     

Femtosecond laser-inscribed waveguides in Nd3^＋：y3^＋：SrF2 crystals

Optical waveguides are fabricated in Nd3^＋：y3^＋：SrF2 crystals by a 1-kHz femtosecond laser using the double-line approach. Waveguides with different separations （10, 15, and 20 μm） between two consecutive optical breakdown tracks are produced, and their optical performances are explored by end-fire coupling to 780-and 532-nm lasers. Propagation loss of the waveguide with 20-pro separation is estimated. The micro- photohmlinescence and micro-Raman spectra indicate that the original fluorescence and lattice structure of the Nd3^＋：y3^＋：SrF2 crystals are well preserved in the waveguide. Therefore, the obtained waveguide structures are promising candidate for application in integrated waveguidc lasers.     

飞秒激光诱导自组织纳米周期结构及其光学特性的研究进展

飞秒激光具有超快、超强的特点.飞秒激光微纳加工发展非常迅速. 本文综述了近十年来利用飞秒激光在金属、半导体、介质等各类材料中制备的纳米周期结构, 阐述了若干关于飞秒激光诱导纳米周期结构的物理机理的观点.讨论了基于偏振调制的多光束 干涉在半导体表面制备纳米周期结构,简要叙述了周期结构对材料光学特性的影响. 关键词： 飞秒激光 纳米周期结构 多光束干涉 光学特性     

8位取代吡咯甲川-BF2化合物的光物理行为

Six novel pyrromethene BF2 complexes,of which five compounds have not been reported,were synthesized and characterized.Their relationships between st ructure and photophysical behavior were studied with the aid of fluorescence and triplet state absorption spectra.The results indicate that,compared to 8 alkyl pyrromethene BF2 complexes,the compounds containing 8 aryl exhibit high fluore scence quantum yield and rather low triplet state absorption.     

Pr3+:Y2SiO5中的反斯托克斯荧光谱及其对基态Stark分裂能级的确定

掺杂在晶体Y2 SiO5(YSO)中的Pr3 ,运用脉冲激光激发 3H4 → 1 D2 跃迁 ,粒子通过非辐射能量转移从能级 1 D2 转移到能级 3P0 ,测得了对应于 3P0 → 3H4 跃迁的反斯托克斯荧光光谱 ,由此可确定 3H4 的Stark分裂能级以及 3P0 能级的能量高度。与运用激光激发 3H4 → 1 D2 跃迁 ,通过观察 1 D2 → 3H4 斯托克斯荧光光谱确定3H4 的Stark分裂能级方法相比 ,该过程避免了不同晶点位置中 (Crystallographicsite)Pr3 的 1 D2 能级间的能量转移影响 ,从而具有较高的确定性。同时 ,我们观察了反斯托克斯荧光的时间特性     

Enhancement and modulation of terahertz radiation by multi-color laser pulses

We study theoretically intense terahertz radiation from multi-color laser pulse with uncommon frequency ratios. Comparing the two-color laser scheme, of which the uncommon frequency ratio should be set to be a specific value, we show that by using multi-color harmonic laser pulses as the first pump component, the lasers as the second pump component can be adjusted in a continuous frequency range. Moreover, these multi-color laser pulses can effectively modulate and enhance the terahertz radiation, and the terahertz yield increases with the increase of the wavelength of the uncommon pump component and is stable to the laser relative phase. Finally, we utilize the electron densities and velocities of ionization events to illustrate the physical mechanism of the intense terahertz generation.     

抽运-自旋定向-探测技术及其应用

抽运-自旋定向-探测是最近发展起来的一种新型瞬态测量技术,该技术在胶体纳米结构电荷分离超快动力学探测中具有独特的优势.本文在比较传统的两光束载流子抽运-探测以及自旋抽运-探测的基础上,深入分析了三光束抽运-自旋定向-探测技术的特点、光路配置及其在胶体量子点光致负荷电、正荷电探测中的应用.最后对三光束抽运-自旋定向-探测技术的更多应用前景作出展望.     

亚10 fs激光脉冲产生中的受激拉曼散射与四波混频效应

自行搭建的自锁模钛宝石激光器工作在下稳区的上边界附近,采用熔融石英棱镜对在激光器谐振腔的腔内和腔外同时进行群速度色散补偿.随着腔内棱镜对提供色散补偿的变化,输出激光脉冲的频谱会突然展宽至664—840nm,其空间模式也由基横模变化至衍射环状结构,这是受激拉曼散射和四波混频效应导致锁模激光脉冲频谱进一步展宽的结果.在此状态下自锁模钛宝石激光器可实现670—865nm范围的波长调谐.如此宽的频谱为钛宝石激光器产生亚10fs激光脉冲提供了必要的条件. 关键词： 飞秒激光脉冲 受激拉曼散射 四波混频 群速度色散     

Selective excitation and suppression of coherent anti-Stokes Raman scattering by shaping femtosecond pulses

Femtosecond coherent anti-Stokes Raman scattering (CARS) suffers from poor selectivity between neighbouring Raman levels due to the large bandwidth of the femtosecond pulses. This paper provides a new method to realize the selective excitation and suppression of femtosecond CARS by manipulating both the probe and pump (or Stokes) spectra. These theoretical results indicate that the CARS signals between neighbouring Raman levels are differentiated from their indistinguishable femtosecond CARS spectra by tailoring the probe spectrum, and then their selective excitation and suppression can be realized by supplementally manipulating the pump (or Stokes) spectrum with the $\pi $ spectral phase step.