激光方脉冲作用下强场自电离过程

本文研究了激光方脉冲作用下的强场自电离过程,从而推广了以往包含高阶离化的研究,讨论了基态布居和自电离共振线型在强场下受激光脉宽、光强的影响。结果表明,强场自电离过程及其中的高阶离化不仅与光强有关,而且还和原子与激光相互作用的时间紧密相关。     

用ICE技术观察和测定镁Mg原子3p9d(J=1,3)的自电离谱

用原子束技术—ＩＣＥ分步激发方案—激光共振电离—飞行时间质谱探测离化信号的方法，观察到了原子束中镁Ｍｇ原子３ｐ９ｄ（Ｊ＝１，３）的自电离谱，并对实验结果进行了讨论和分析。     

Yb的激光三步激发自电离谱

用激光三步共振激发研究Yb原子的自电离谱,测得能量在50443一57750cm^-1范围内的16个自电离能级。并用偏振光技术测定两个自电离态的J值。 关键词：     

用ICE技术观察和测定镁Mg原子3p9d（J=1,3）的自由离谱

用原子束技术－－ＩＣＥ分步激发方案－－激光共振电离－－飞行时间质谱探测离化信号的方法，观察到了原子束中镁Ｍｇ原子３ｐ９ｄ（Ｊ＝１，３）的自电离谱，并对实验结果进行了讨论和分析。     

光电子谱的峰开关效应

在文献[12]的基础上研究了强激光场作用下自电离原子的光电子谱,发现了与强场多光子电离中相类似的峰开关效应,从而进一步证实了强场下二阶离化过程和光电子谱中高阶峰的重要作用.本文结果对已有的强场自电离理论作了重要修正. 关键词：     

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.     

双色激光共振增强的气相C_6H_6分子的光电离谱

本文给出了双色激光共振增强的气相苯的光电离谱结果。激发光子首先把分子从基态选择激发到s-1电子单态中一个确定的振动态,然后第二台激光器输出的离化光子把这个激发分子离化。实验证明离子的产额不但与中间电子能级~1B_(2u)的振动态有关,且依赖于离化激光的波长。从所得到的离子谱的结构和强度可以求得离子的电子基态~2E_(1g)的振动频率及分子参数,精度较高。自离化里德堡能级对离化截面的贡献非常显著。某些自离化共振峰可以确认为是这些里德堡态的振动能级。     

强激光场诱导自电离理论

在Fano模型中考虑了在离化限之上额外吸收一个光子的二阶离化过程,重新研究了强激光场诱导自电离的动力学,着重讨论了二阶离化过程对光电子谱的重要影响.     

光滑激光脉冲作用下的强场自电离

本文研究了光滑激光脉冲作用下包含高阶离化的强场自电离过程,导出了其中的基本方程,得到了基态布居和光电子谱的一系列解析表达式。讨论了指数增长脉冲作用时的具体结果,发现高能谱比低能谱更能呈现出光电子谱在脉冲光作用下特有的多峰分裂。     

强场自电离中自发辐射谱的功率增宽

本文在强场自电离模型中计及自电离态的光致离化衰变,重新计算了自发辐射谱,发现了显著的功率增宽现象。这一结果与简单模型下的计算结果有很大差异。     

多光子过程和自发辐射对激光诱导自电离的影响

利用反作用算符的方法,研究了一个单模激光场将原子从束缚能级激发到自电离能级的过程中,双光子过程和自发辐射过程的影响。研究结果表明:自发辐射对这种光电离过程的影响一般情况下是很小的,但光子能谱特性十分明确地表明,辐射主要来源于由态共振加强的喇曼过程;并显示了激光诱导自电离过程中的缀饰(Dressed)原子图像;双光子过程将使光电子能谱和光诱导自电离过程变得非常复杂,单光子和双光子过程所产生的光电子能谱,都具有多极大值结构。     

Threshold photoemission spectroscopy in solids

Threshold photoemission spectroscopy (TPES) is used to measure the Fe 2p spectrum of a stainless steel sample. The obtained spectrum is compared with analogous spectra measured by X-ray photoemission and absorption spectroscopies. The results of this comparison suggest that resonant two-electron autoionization processes, rather than direct photoemission from the core level, are the main mechanisms contributing to the signal. Limits and applicability of this experimental approach to investigate bulk electronic properties in solids are discussed.     

包含自电离过程的阈上离化

多电子原子都存在自电离过程,本文研究了存在自电离时的阈上离化过程,利用一个简化模型得到了光电子谱的解析表达式。结果表明,自电离的存在使阈上离化过程更为复杂,导致许多新现象的产生。 关键词：     

Influence of the helium autoionization structures on the single/double ionization signal

Calculations of intense field (around 10¹⁶ W/cm²) single- and double-ionization processes in helium at XUV wavelengths are presented. The laser wavelength is chosen near the | 2s2p ¹ P autoionization structure and the dynamics are explored. Single and double ionization yields, as well as the photoelectron energy spectrum for photon energies around the autoionization structure are calculated. In the case of a pulse of few femtoseconds duration, no significant enhancement of the double ionization yield has been found in tuning the photon frequency around the peak of the resonance. It is also shown that in the case of a long pulse (and hence narrow compared with the relevant autoionization width), the branching ratio of double to single ionization yield can be relatively enhanced by tuning to the absorption minimum of the resonance. Received 19 February 2002 / Received in final form 2 May 2002 Published online 19 July 2002     

Competition between relaxation and decay of a resonantly excited core-hole state

By a many-body theory it is shown that in general when the time scale of the relaxation from the resonantly excited core-hole state to the fully relaxed core-hole state is much shorter than that of core-hole decay, the autoionization (deexcitation) spectrum is more or less identical to the Auger-electron spectrum by core-hole decay of the fully relaxed core-hole state. Here, the fully relaxed core-hole state is the lowest core-hole state in the X-ray photoelectron spectroscopy spectrum. The present theory explains why the C 1s autoionization spectrum of CO molecule adsorbed on Ni(1 0 0) surface measured at the resonant core-level electron excitation energy is more or less indentical to the Auger-electron spectrum measured at far above the core-level electron ionization limit.     

光学外差法测量Ba原子的自电离态

提出了把三光子共振非简并六波混频(NSWM)和双光子共振非简并四波混频(NFWM)应用于研究Ba原子自电离态的光学外差探测方法。采用该方法测量了Ba原子的6P_３／２19d自电离态,并观察到了三光子共振 NSWM和双光子共振NFWM信号干涉引起的信号增强。该方法是一种纯非线性光学方法,具有优秀的空间分辨率和简单的光路。其中双光子共振非简并四波混频信号作为本地振荡光束,三光子共振非简并六波混频信号作为信号光束,通过 改变信号光束的频率来达到用光学外差探测法研究Ba原子自电离态的目的。该方法中,实现相位匹配所要求的条件不是很严格,可以在很宽的频率范围内实现相位匹配,而一般的六波混频很难做到相位匹配, 并且所测量的信号是相干光, 当用窄带宽的激光时,可以获得消多普勒的分辨率。     

N23-core losses and autoionization emissions of clean and oxygen exposed zirconium

The electron energy loss spectra associated with N₂₃-excitation and the low energy N₂₃VV Auger emission have been studied for both the clean and oxygen exposed zirconium. In the high energy side of the N₂₃VV Auger spectrum, autoionization emission of electrons of the valence band due to the decay of 4p electrons excited to states ≈9eV above the Fermi level has been identified. The excitation process can be also observed in the electron energy loss spectra. This is the first time that an autoionization feature is observed in a electron excited Auger spectrum of a 4d transition metal.