钾原子4S-6S双光子共振的实验研究

利用YAG激光抽运的染料激光器将钾原子由基态 4S双光子共振激发到 6S态 ,研究了钾原子 4S 6S双光子共振三光子电离的电离谱与温度、激光强度的关系 ,发现电离流的强度随着温度的升高而增强 ,当温度在 370℃附近时达到最大值 ,此时温度继续升高电离流强度减弱。在温度不变的情况下 ,电离流强度随着激光能量的增强而增强 ,当激光强度为 4 5× 10 5W /mm2 时到达最大值 ,继续增加激光强度 ,电离流强度趋于饱和。实验中观测到对应于 6S 4P的自发辐射     

230—245nm范围内Cl原子共振增强多光子电离光谱

利用共振增强多光子电离－－时间飞行质谱技术获得了Ｃｌ原子在２３０－２４５ｎｍ范围内的代振增强多光子电离光谱,共观察到２６条谱线,其中５条是作者新观察到的,这些谱线对应从Ｃｌ原子基态到激发态的双光子跃迁。从中还观察到Ｃｌ原子在强电场中的Ｓｔａｒｋ效应,发现在强场条件下,Ｃｌｄ原子绵基太＾２Ｐ１／２＾０和＾２Ｐ３／２＾０两能级之间的能工位移１．３５ｃｍ＾＝１。而各电子激发态的Ｓｔａｒｋ位移则大致相等,     

激光场中锂原子发射的电离阈值以下低阶谐波的研究

利用单电子近似下锂原子精确的模型势,通过数值求解三维含时薛定谔方程的方法,研究了锂原子在激光场中发射低阶谐波的性质,研究结果表明,对于锂原子电离阈值以下的低阶谐波,除了通常的奇次谐波外,还有侧峰结构出现,运用同步压缩变换技术(SST)分析这些低阶谐波的辐射特性,我们发现这些侧峰是由原子在激光场中的缀饰态之间的跃迁和无场下激发态到基态的跃迁组成的,如果当激光脉冲结束后,仍有发射的侧峰,其位置与主峰之间的能量差可以用来估算原子激发态在激光场中的最大Stark移动.     

对氟甲苯分子四光子电离过程的分析

根据量子力学微扰理论给出了相干扰激发电离情形下双光子共振三光子近共振和双光子近共振三光子共振这两种两光子电离过程的电离截面表达式，表明这两种过程的离子强度与它们的起始能级有关，根据这一结论分析了实验测得的对氟甲苯分子的多光子电离谱，结果表明获得该电离谱的过程为三光子共振四光子电离过程。     

钠蒸气中的双光子共振三光子电离和双光子混合共振三光子电离

在钠原子－分子混合样品中，分别运用双光子共振三光子电离以及双光子混合共振三光子电离，测得了钠原子４Ｄ态的电离流时间衰减曲线。由电离流与多光子动力学参数的关系，得到了４Ｄ态的光电离截面。     

原子自电离态的研究

用适当的能量激发原子的某一电子时,电子被激发到能量高于基态的激发态.当外部作用与原子实(原子核加其他电子)的作用相等时,电子的能量E=0,电子脱离原子,发生电离.使该电子电离的最小能量叫做它的电离极限.在电离极限之上的原子态是连续态,因为这时原子实际上是离子加自由电子,自由电子的能量可以是任意的,所以这时是连续态.所有连续态的总体叫连续区.显然外层电子的电离限比内层电子的电离限低,即电离内层电子比电离外层电子需要更大的能量.这样,当激发一个内层电子时会出现这样一些分离态,这些态在一个外层电子的电离极限之上,在该电子…     

钠蒸气中的双光子共振三光子电离和双光子混合并振三光子电离

在钠原子－分子混合样品中，分别运用双光子共振三光子电离以及双光子混合共振三光子电离，测得了钠原子４Ｄ态的电离流时间衰减曲线。由电离流与多光子动力学参数的关系，得到了４Ｄ态的光电离截面。     

乙基苯的振动光谱和量化计算

用单色双光子共振电离方法研究了乙基苯的第一激发态的振动光谱. 从基态跃迁到第一激发态的带源位置出现在37586 cm^-1处.获得的第一激发态振动光谱超过了2000 cm^-1,并观察到了几个乙基取代基的扭转振动和与苯相似的正则振动. 同时,用含时密度泛函理论和单组态相互作用(CIS)方法计算了第一激发态的跃迁能量,用Hartree-Fock和CIS方法优化了基态和第一激发态分子结构,预测了振动频率. 基态和激发态结构的优化结果均显示为顺式结构,即乙基取代基的对称面垂直了苯基平面.     

测定硅原子共振谱线精细结构相对强度

原子光谱实验应主要了解谱线波长和谱线强度两个问题。前者涉及原子能级结构,后者涉及原子能级之间跃迁概率;二者紧密联系,是了解原子结构的二个方面。原理共振谱线是指从最低激发态直接跃迁到基态的谱线。硅原子基态是[Ne]3s~23p~2[~3P],三重态的最低激发态是[Ne]3s~23p4s[~3P],共振跃迁如右图所示。当精细分裂不大时,温度对ν~4影响很小,则A可视为常数。对于L→L跃迁,精细结构强度的理论计算为经计算,获得的硅原子共振线精细结构强度列表如下。     

Gd原子的共振多光子电离研究

本文首次报道了用共振多光子电离(RMPI)技术探测到四条在可见光范围内的Gd原子强双光子跃迁线.观察到双色三光子Gd原子激光同位素分离.研究了高分辨率Gd原子电离谱,并解释了电离谱的线型.     

叠加态下3色场波形优化增大谐波辐射截止能量及强度

在He~+离子1s态和2s态的叠加态作为初始态时,提出一种优化3束激光场来增大谐波截止能量和强度的方法.结果表明:在叠加初始态下,谐波强度要比基态初始态下增强3个数量级以上.随后,在3色场波形优化下,谐波截止能量又得到增大,进而获得一个高强度、高光子能量的谐波光谱连续区.通过叠加光谱连续区上最后100次的谐波可以获得一个27 as的孤立阿秒脉冲.     

Generation of intense water window X-ray pulses by superposition of an initial state of the helium atom driven by a three-color field

We theoretically study the generation of high-order harmonics and attosecond pulses from the superposition of an initial state in helium atom driven by a three-color laser field. It is shown that when the initial state is chosen to be a single electronic state, due to the rapid depletion of the ground state, the efficiency of the spectral continuum will be decreased as the initial state increases. When the initial state is chosen to be the coherent superposition of the ground state and an arbitrary excited state, the efficiency of the spectral continuum can be enhanced compared to that from the single initial state. Further, with the optimization of the three-color laser beam, not only can the harmonic cutoff be extended to the water window X-ray region but also the spectral continuum is contributed by the single harmonic emission peak with the dominant short quantum path. Consequently, two combinations of the laser parameters can be found to generate the water window spectral continuum. By properly superposing some harmonics on the spectral continuum, a number of intense water window pulses with the duration of sub-35 as can be produced.     

势函数对强激光辐照下原子高次谐波辐射的影响

理论上研究了中红外强激光分别与长程库仑原子和短程势模型原子相互作用产生的高次谐波辐射.发现在相同激光参数条件下,与长程库仑原子的谐波辐射相比,短程原子具有更低的辐射效率,但在高频区域(接近cutoff位置),二者效率相似.通过对谐波辐射的时间频率分析发现,在短程模型原子谐波辐射中,长轨道发挥更重要的作用.利用其产生的高次谐波辐射,可以产生孤立阿秒脉冲.     

Theoretical Study of High-Order Harmonic Generation From a Coherent Superposition State in a Chirp-Free Pulse Combined with a Chirped Control Pulse

In this paper, we theoretically investigate high-order harmonic generation (HHG) from a helium atom prepared in a coherent superposition state in a two-color laser field. Numerical results show that the emission efficiency of the harmonic spectrum in a coherent superposition state is enhanced by approximately eight orders of magnitude compared with the case of the ground state. In addition, the effect of the initial population of the excited state on the HHG is presented to reveal the physical origin of the enhancement of HHG. By adjusting the laser parameters of the driving pulse, such as the chirping parameter, the relative phase, and the intensity of the driving pulse, an ultrabroad continuum with a width of 275 eV can be observed. Finally, an isolated 12-as pulse is generated after phase compensation.     

Quantum path control using attosecond pulse trains via UV-assisted resonance enhance ionization

We theoretically investigate the quantum path selection in an ultraviolet(UV)-assisted near-infrared field with an UV energy below the ionization threshold. By calculating the ionization probability with different assistant UV frequencies, we find that a resonance-enhanced ionization peak emerges in the region Euv < Ip, where Euv is the photon energy and Ip is the ionization energy. With an attosecond pulse train(APT) centered in the resonance region, we show that the short quantum path can be well selected in the continuum case. By performing the electron trajectory analysis, we have further explained the physical mechanism of the quantum path selection. Moreover, we also demonstrate that in the resonance region, the harmonic emission from the selected paths is more efficient than that with the APT energy above the ionization threshold.     

高频激光脉宽对原子光电子发射谱的影响

采用广义含时伪谱方法数值求解原子在激光脉冲作用下的动量空间含时薛定谔方程,研究了高频激光脉宽对原子光电子发射谱的影响.数值模拟表明,随着激光脉冲宽度的增加,光电子谱干涉结构的振荡幅值逐渐减小,其最大峰值的强度和位置取决于产生有效电离的最大即时强度.通过分析光电子谱的变化规律能进一步加深对高频强场电离产生的动力学干涉效应的理解.     

Harmonic Enhancement Mechanism of a Superposition State Atom Irradiated by Short Pulses

We investigate the high-order harmonic generation （HHG） of a model atom whose initial state is prepared in a superposition of its ground state and an excited state irradiated by different duration laser pulses. Compared to the HHG generated from an atom whose initial state is in its ground state, its conversion efficiency obtains some enhancement. The enhancement originates from the higher ionization rate （rather than the ionization yield） of the atom with superposition initial state.     

强激光场中长程势与短程势原子产生高次谐波与电离特性研究

用数值方法求解含时薛定谔方程，研究了具有长程势和短程势的一维原子在强激光场中的高次谐波和电离特性. 在强激光场中，长程势和短程势原子产生的高次谐波具有相似的特性，对应的平台和截止位置相同，但是短程势原子没有低阶的高次谐波，而长程势和短程势原子在激光场中的电离概率明显不同. 研究结果表明，原子的激发态结构对低阶的高次谐波和原子的电离概率有重要影响. 关键词： 强激光场 高次谐波 电离概率     

迭加态原子高次谐波发射的选频提高

本文研究了由体系的基态和较高激发态迭加形成的原子在强激光场作用下的高次谐波发射.观察电离波包的演化过程,阐明了谐波发射效率提高的原因.在给定入射激光条件下,通过选择不同的激发态,可以实现对谐波发射的控制.     

Decoding the electron dynamics in high-order harmonic generation from asymmetric molecular ions in elliptically polarized laser fields

The high-order harmonic generation from an asymmetric molecular ion is theoretically investigated based on the Born-Oppenheimer model with two-dimensional electron dynamics. It is shown that the harmonic intensity changes periodically in elliptically polarized laser fields. The periodical character is ellipticity-dependent. By establishing the physical image, the periodicity of the harmonic intensity can be ascribed to the contributions of the ground state and the excited state. Furthermore, the electron dynamics from different electronic states can be selected via combining the elliptically polarized laser field with a static electric field. The harmonics dominated either by ground state or excited state are emitted once in an optical cycle in the combined laser field.