双布里渊放大池放大控制脉冲波形的研究

提出一种主放大池与修整放大池相结合的双布里渊放大池放大控制脉冲波形的新方法.在主放大池中，通过调节抽运光与种子光的延迟时间，完成对脉冲波形的整体控制；而在修整放大池中，通过调节双池间距，完成对脉冲波形、尤其是对脉冲前沿的微调.实验研究了双池间距对脉冲波形的影响，得到脉冲波形随双池间距的变化规律.结果表明：相遇时间及双池间距是控制脉冲波形最重要的参数.此双布里渊放大池系统可以方便地控制脉冲波形，尤其可以微调脉冲前沿. 关键词： 受激布里渊散射 布里渊放大 脉冲波形控制     

抽运光对双布里渊放大池放大控制脉冲波形的影响

在传统的独立双池结构的受激布里渊相位共轭镜中,引入修整放大池,采用主放大池与修整放大池相结合的双布里渊放大池结构控制脉冲波形,主放大池控制脉冲的整体波形,而修整放大池对脉冲波形进行微调. 研究了抽运光功率密度对双布里渊放大池放大控制脉冲波形的影响,得到了不同抽运光功率密度下,脉冲波形随双池间距的变化规律. 研究表明,抽运光功率密度决定了种子光的放大效率,是控制脉冲波形的重要参数. 关键词： 受激布里渊散射 布里渊放大 脉冲波形控制     

储存环自由电子激光相干谐波实验的同步系统

 为了获得短波长自由电子激光(FEL),可以使储存环中的相对论性电子与外加强激光脉冲在光学速调管中充分耦合,从而产生高次谐波的相干辐射。为使耦合充分,必须使电子束团与激光脉冲在时间和空间上完全同步。其中空间上的同步可通过调节外激光的光路来实现,给出了实现时间上同步的一种方案。     

新型部分相干光束的产生及其相干特性

利用相干理论,研究了新型部分相干光束的相干特性.用激光光束透过旋转的特殊毛玻璃,产生一种相干性分布特殊的新型部分相干光束.实验上经双孔干涉,记录了该光束经不同小孔间距双孔产生的干涉条纹,计算得出所对应的相干度,并获得了该光束在不同传输距离下的相干度分布情况,发现该光束的相干度分布与高斯-谢尔模型光束的相干度分布不相同,其相干度随着传输距离的增大而变强.     

储存环自由电子激光相干谐波实验的同步系统

为了获得短波长自由电子激光(FEL),可以使储存环中的相对论性电子与外加强激光脉冲在光学速调管中充分耦合,从而产生高次谐波的相干辐射。为使耦合充分,必须使电子束团与激光脉冲在时间和空间上完全同步。其中空间上的同步可通过调节外激光的光路来实现,给出了实现时间上同步的一种方案。     

原子—分子混合激发及所产生的受激和相干辐射

用适当波长的激光混合激发原子－分子样品，和通过原子－分子碰撞能量转移，可产生从紫外到红外宽波段范围内的受激和相干辐射，其中包括固定波长辐射，可调谐辐射以及宽带辐射以及宽辐射。这是一个物理涵义极为丰富并具有应用前景的研究领域。     

钾原子中由四波,六波混频过程产生的相干辐射

当双光子共振激发钾原子于６Ｓ能级时，由光泵受激辐射，串级受激辐射参与的四波、六波混频以及电离复合的布居过程，产生了位于可见区的诸多相干辐射，文中对混频机制进行了分析和讨论，并对所测得的相干辐射进行了标识。     

相干谐波辐射的测量方法和系统

研究了光学速调管自发辐射谱,其调制率已达0.80,即将进行相干谐波辐射实验。介绍了相干谐波辐射实验的主要考虑因素、相干增强因子的测量方法和测量系统以及种子激光与电子束的准直和同步。     

相干谐波辐射的测量方法和系统

 研究了光学速调管自发辐射谱,其调制率已达0.80,即将进行相干谐波辐射实验。介绍了相干谐波辐射实验的主要考虑因素、相干增强因子的测量方法和测量系统以及种子激光与电子束的准直和同步。     

由基模群聚产生的相干谐波的时间剖型和线宽

本文中得到由基模群聚产生的相干谐波的功率表达式,并且解释了它们的时间剖型和线宽。 关键词：     

采用适宜靶原子提高高次谐波的转化效率

通过对影响谐波转化效率因素的分析,提出选择适宜的靶原子对象,即选择在高能区具有较强连续态-基态耦合强度的靶原子,可以优化高次谐波的发射条件.本文的数值实验结果表明,利用该方案,可以把平台区尾部谐波的转化效率提高两个数量级.     

Phase-matched high harmonic generation for the study of rotational coherence molecular dynamics

We report the observation of periodic modulations in the high order harmonic radiation from diatomic molecules in a semi-infinitive gas cell when a preceding femtosecond laser beam, which is off-axis to the high-harmonic generation beam, modifies the phase-matching condition through the field-free alignment of the molecules. The observed modulations of the high harmonic radiation versus the time delay between the pulses result from periodic changes in the nonlinear refractive index associated with rotational Raman coherence. This opens up a new potential technique for studying rotational coherence dynamics in the ground states of molecules.     

双色场诱导气体产生相干可控的四次谐波

利用钛宝石飞秒激光器输出的基频脉冲ω及其倍频脉冲2ω所构成双色场作用空气, 实验中检测到了中心波长处于真空紫外波段的四阶谐波. 在气体未发生电离的情况下, 四次谐波强度对双色场的能力依赖关系显示其产生是参量过程2ω+ω+ω→4ω的贡献. 当气体发生电离, 四次谐波强度与双色场相对相位有关, 可通过双色场相干控制. 实验研究了四次谐波对双色场相位的依赖性以及与太赫兹波的关联性, 其结果与数值模拟结果相符, 分析发现当气体发生电离时四次谐波的产生过程存在太赫兹辐射Ω_THz的参与, 是参量过程2ω+2ω±Ω_THz→4ω和2ω+ω+ω→4ω的共同贡献.     

Effect of fundamental radiation wave front astigmatism on the process of second optical harmonic generation in uniaxial crystals

Nonlinear processes of conversion of radiation with wave front astigmatism in nonlinear crystals of 6 and 3m symmetry are theoretically analyzed. Spatial-angular and energy structures of the second optical harmonic in lithium niobate and iodate crystals are investigated theoretically and experimentally. Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 11, pp. 72–75, November, 2008.     

利用相位啁啾单色中红外激光场产生高次谐波

本文通过求解薛定谔方程,理论探索了高次谐波及孤立阿秒脉冲在相位调制的单色中红外激光场中的产生.研究结果表明,通过加入含时相位啁啾小量,能够有效的提高高次谐波的产生效率,获得超宽平台谐波谱及超短孤立阿秒脉冲.特别是在相位为0.3π的基础上,同时加入啁啾小量βt,在β=0.3时,可得到带宽为822 e V的超连续高次谐波平台.最后通过叠加第二平台高次谐波,可得到带宽仅为2.7 as的孤立阿秒脉冲.且脉冲强度比没有加入啁啾小量的情况下显著增强.     

用简单方法求解谐振子波包的演化

用简单方法求出一系列谐振子波包的波函数随时间演化的显式．该方法不需用到特殊函数的任何知识。     

Nonadiabatic effects in the molecular high-order harmonic generation from two-center molecular ions

The nonadiabatic effects in the molecular high-order harmonic generation (MHHG) from H₂⁺ and its isotope have been theoretically investigated beyond the Born-Oppenheimer approximations. It is found that (i) due to the asymmetric contributions of the harmonic emission on the rising and the falling parts of the laser field, the frequency red-shifts in the MHHG can be found. As the initial vibrational state or the pulse intensity increases, the red-shifts of the harmonics are decreased and even the blue-shifts of the harmonics can be found in the higher pulse intensity with the higher vibrational state. With the increase of the pulse duration, the frequency red-shifts and the blue-shifts in the MHHG are decreased and enhanced, respectively. The shifts of the harmonics from the heavy nuclei are decreased compared with those from the light nuclei. (ii) Due to the coupling of the electron-nuclear dynamics, the non-odd harmonics can be produced at the larger internuclear distance. With the increase of the initial vibrational state or the pulse duration, the generations of the non-odd harmonics can be enhanced. As the pulse intensity increases, the intensities of the non-odd harmonics are first increased and then decreased at the much larger pulse intensity. Due to the slower nuclear motion, the generations of the non-odd harmonics are decreased as the nuclear mass increases. (iii) With the increase of the alignment angle of the molecule ions, the nonadiabatic effects in MHHG (including the shifts of the harmonics and the generations of the non-odd harmonics) are decreased.     

Off-centre impurity-related nonlinear optical absorption,second and third harmonic generation in a two-dimensional quantum ring under magnetic field

Abstract

The effects of an off-centre donor impurity on the non-linear optical absorption, second and third harmonic generation in a GaAs two-dimensional disc-shaped quantum ring under magnetic field are investigated within the compact density-matrix formalism and the effective mass approximation. The results reveal that: (i) the absorption spectra extend on larger energy intervals at the increment of the magnetic field; (ii) the possibility of generating second harmonic response from the system is demonstrated for an impurity placed on the repulsive part of the confining potential; (iii) both second harmonic and third harmonic coefficients are one order of magnitude larger for an impurity placed on the repulsive part of the potential and are blue-shifted by the increment of the magnetic field regardless the impurity position.     

Supercontinuous high harmonic generation from asymmetric molecules in the presence of a terahertz field

We have investigated high-order harmonic generation from asymmetric molecules. It is found that supercontinuous high harmonics,which are produced from asymmetric molecules by significantly steering the ionization,are broken down when the electric field of the 5-fs driving laser pulse is increased to 0.16 a.u. The high harmonic generation from asymmetric molecules with the presence of a terahertz field is also investigated. This reveals that the terahertz controlled laser pulse significantly increases the energy difference between photons,emitted from the ejected electrons,in the first and second halves of the optical cycle at the centre of the driving laser pulse. In this way,a 200-eV broadband supercontinuum can be produced in the plateau,from which a 60-as pulse with a bandwidth of 60 eV can be directly obtained with a minor post-pulse.     

双曲函数型辅助方程构造具5次强非线性项的波方程的新精确孤波解

在辅助方程法的基础上利用两种函数变换和一种双曲函数型辅助方程，通过符号计算系统Mathematica构造了在力学当中一个重要的模型，有5次强非线性项的波方程的新三角函数型和双曲函数型精确孤波解.这种方法寻找其他具5次强非线性项的非线性发展方程的新精确解方面具有普遍意义. 关键词： 双曲函数型辅助方程 函数变换 具5次强非线性项的波方程 精确孤波解