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.     

激光分离同位素过程中的布居囚禁

采用辍饰原子模型研究了四光子三步共振离化过程的布居囚禁，发现了一种与离化速率无关的布居囚禁。通过数值求解裸原子表象的含时薛定谔方程发现，适当选取激光频率与跃迁的失谐量，可以解除这种布居囚禁。     

在双色共振激光场中电子原子碰撞的自由-自由跃迁过程

研究了双色共振激光场中电子原子碰撞的自由-自由跃迁过程. 利用三能级模型和旋转波近似得到了靶原子的波函数, 在波恩近似的基础上进一步导出了多道碰撞的微分截面公式. 利用此公式计算了共振激光场中的激发碰撞对整个的碰撞贡献.     

Sr2准分子吸收离化及混合跃迁的研究

Ｎｄ－ＹＡＧ激光器三倍频泵浦的染料激光激发Ｓｒｌ原子,热二极管探共振离化信号,获得Ｓｒｌ高Ｒｙｄｂｅｒｇ５ｓｎｄＤ２系列双光子激光共振电离谱。实验发现激光汉长调４４０ｎｍ附近时,存在一Ｓｒ２准分子吸收光谱带,同时还观测到了５ｓ５ｐ＾１Ｐ１－５ｓ１１ｄ＾１Ｄ２,５ｓ５ｐ＾１Ｐ１－４ｄ＾２３Ｐ１混合共振跃迁现象。并对这种瞬态准分子的连续吸收光电离背景的形成和混合共振跃迁的机制作了初步探讨,同时对缓冲气     

碘化铯分子的光离解及生成物铯原子的共振电离研究

利用脉冲激光束与分子的相互作用，对ＣｓＩ分子进行了光离解。同时，用另一束可调谐激光对ＣｓＩ分子离解后产生的中性铯原子进行共振激发，然后把处在激发态的铯原子进行光电离。对Ｃｓ＋的飞行时间质谱进行了分析，并对光离解及光电离过程中可能存在的多光子电离（ＭＰＩ）进行了讨论。     

Sn激光共振电离质谱分析中电离通道理论探讨

Sn激光共振电离质谱同位素分析中电离通道的选择非常关键.采用Dirac–Hartree–Fock(MCDHF)方法和相对论组态相互作用的Grasp VU原子结构计算程序,计算了Sn、Te原子的低激发态能级结构、光谱跃迁几率.通过对Sn质谱分析用灯丝样品进行热蒸发实验,确定了Sn原子在蒸发条件下基态能级粒子布局.结合理论计算跃迁数据和布局数据,从选择性电离角度出发,推荐了Sn激光共振电离质谱分析中Sn电离光谱通道.     

钙、锶、钡和汞离子激光中的共振辐射俘获效应

根据Holstein的共振辐射俘获理论，讨论了气体温度和辐射俘获下能级粒子数密度对辐射俘获上能级有效辐射寿命的影响，显示辐射俘获下能级粒子数密度是辐射俘获效应中的主导因素.计算了钙，锶，钡和汞四种离子七条共振-亚稳能级跃迁激光在不同电离率下产生共振辐射俘获效应的阈值条件，发现当电离率为5%时这类激光的出光温度与共振辐射俘获的阈值温度相一致，这与实验得出的电离率为3%—5%相符合.表明达到共振辐射俘获阈值条件是该类激光实现粒子数反转的重要因素.     

受限氦原子的共振增强现象

本文用B样条方法计算了受限氦原子的能级与波函数,并在此基础上研究了氦原子的跃迁谱特性,发现了在限制势的作用下,氦原子跃迁谱有非常强的共振增强现象出现.     

Al原子共振双线跃迁几率实验研究

我们用Nd：YAG脉冲激光烧蚀金属Al靶产生等离子体，利用时间分辨技术摄取Al等离子体辐射时间分辨谱，获得Al原子共振双线辐射谱；通过积分谱线下的面积，计算共振双线强度；根据共振双线强度比，推断Al原子共振双线跃迁几率比，并与理论计算结果比较。结果发现，实验结果与理论计算符合的很好。     

碘原子共振多光子电离光谱研究

用可调谐的染料激光(4600～5000(?)),共振(3+2)和(4+1)多光子电离探测了I(5p~2P_(3/2)~0)和1~#(5p~2P_(1/2)~0).碘原子是由碘分子(I_2)经激光解离而产生的.在上述激光波段中共观察到12个原子跃迁,其中,(4+1)多光子电离跃迁是首次观察到的.     

Analytic continuation of sturmian expansions for two-photon ionization

We show that the sturmian expansions of transition amplitudes for two-photon ionization may be handled as ordinary (single variable) power series, and we describe a simple method for performing their analytic continuation above the photoelectric threshold. Numerical results are presented for the hydrogenic states 1s, 2s, and 2p.     

Photoelectron angular distributions from two-photon ionization of atoms near ionization threshold

Photoelectron angular distributions(PADs) from two-photon ionization of atoms in linearly polarized strong laser fields are obtained in accordance with the nonperturbative quantum scattering theory.We also study the influence of laser wavelength on PADs.For two-photon ionization very close to the ionization threshold,most of the ionized electrons are vertically ejected to the laser polarization.PADs from twophoton ionization of atoms are determined by the second order generalized phased Bessel function at which the ponderomotive parameter plays a key role.In terms of dependence of PADs on laser wavelength,corresponding variations for the ponderomotive parameter are demonstrated.     

CS_2分子激发态的紫外多光子电离——双色激光单共振离化的功率密度关系

本文报道气相CS_2紫外双色激光单共振离化的功率密度关系和对高激发态(1~Ⅱg),共振离化特性的研究结果,实验指出通过中间共振态(1~Ⅱ_g)的双光子共振激发三光子离化具有比通过中间共振态((?)A_2)的单光子共振激发三光子离子为高的总离化率,在10~7W/cm~2的功率密度下,观察到饱和效应.实验显示了双色激光单共振离化功率密度关系的研究提供了一种新的光谱学分析方法.这对研究分子高激发态的结构是很重要的.     

Resonant two-photon ionization with high-order continuum states

In this paper,the resonant two-photon ionization of atoms with high-order con-tinuum state is studied.It's found that the C-C coupling among the continuum states enhancesthe two-level atomic Rabi oscillation,and the direct transition from the intermidiate excitedstate to the continuum weakens the Rabi oscillation.Therefore the photoelectron energy spec-tra and the population are changed.     

The effects of self-induced resonance in multiphoton ionization

The ionization of atoms in the presence of an intermediate two-photon resonance is considered. The ionization probability and spectral distribution of the ionized electrons are obtained for the case when the resonant is turned on adiabatically. The limiting cases of small and large ionization widths are investigated. At sufficiently large intensities of the resonant field an essential asymmetry in the ionization probability depending on the sign of the two-photon detuning is obtained.     

Efficient three-step,two-color ionization of plutonium using a resonance enhanced 2-photon transition into an autoionizing state

Resonance ionization mass spectrometry (RIMS) has proven to be a powerful method for isotope selective ultra-trace analysis of long-lived radioisotopes. For plutonium detection limits of to atoms have been achieved for various types of samples. So far a three-step, three-color laser excitation scheme was applied for efficient ionization. In this work, a two-photon transition from an excited state into a high-lying autoionizing state, will be presented, yielding a similar overall efficiency as the three-step, three-color ionization scheme. In this way, only two tunable lasers are needed, while the advantages of a three-step, three-color excitation (high selectivity, good efficiency and low non-resonant background) are preserved. The two-photon transition has been characterized with respect to saturation behavior and line width. The three-step, two-color ionization is a possibility for an improved RIMS procedure.Received: 6 January 2004, Published online: 24 February 2004PACS: 82.80.Ms Mass spectrometry (including SIMS, multiphoton ionization and resonance ionization mass spectrometry, MALDI) - 32.80.Rm Multiphoton ionization and excitation to highly excited states (e.g., Rydberg states) - 32.80.Dz Autoionization     

Ar原子序列双光双电离产生光电子角分布的理论计算

基于多组态Dirc-Fock方法和密度矩阵理论,给出了原子序列双光双电离光电子角分布的计算表达式,发展了相应的计算程序.利用该程序对Ar原子3p壳层序列双光双电离过程进行了理论研究,给出了光电离的总截面、磁截面、剩余离子取向以及光电子角分布的各向异性参数与入射光子能量的函数关系.结果显示在光电离截面的Cooper极小位置附近取向参数出现极大值,而光电子角分布的各向异性参数在该位置附近出现极小值.进一步给出了33.94和55.34 eV光子能量下序列双光双电离过程中第一步的Ar原子和第二步的Ar^+离子3p壳层光电子角分布,分析了序列双光双电离光电子角分布与单光电离光电子角分布的差异.将计算结果与文献已有的数据进行了比较,具有很好的一致性.本文的研究结果对揭示光与物质相互作用的非线性动力学机制具有重要的参考价值.     

Multiphoton ionization spectra in lithium vapour

The two-photon absorption spectrum to high-lying states of Li vapour has been obtained using ion-cell detection. ²S states are observed to n = 32 and the ²D series to n = 49. Simple heating techniques circumvented the problem of absorption by the blue-green band system of Li₂ which overlaps the series limit at 4600 Å. The order of the ionization process was examined and found to vary as the square of the laser intensity for two-photon transitions. A conflict with data obtained with a space-charge-limited diode is examined and possible ionization mechanisms are discussed.     

Multiphoton double ionization of barium

The multiphoton double ionization of Ba from ~280 to 700 nm was investigated using laser pulses 5 ns long of peak intensity ~10¹⁰ W/cm². The spectrum consists of a number of strong resonances, which can be assigned to Ba⁺ transitions. Most of the assignments have been verified by pump-probe techniques. Thus, the Ba⁺⁺ observed is due to sequential ionization. The multiphoton ionization probability is highest for λ~500 nm, which matches a series of strong Ba and Ba⁺ transitions leading to double ionization     

Quasiclassical calculation of the chemical reaction Ba+CH3I

This paper reports the quasiclassical trajectory (QCT) calculations on extended London–Eyring–Polanyi–Sato (LEPS) potential energy surface (PES) for the reaction of Ba atom with CH₃I. In the calculations, the Sato parameters needed in construction of the reaction PES are obtained from simulation of experimental results of BaI product vibrational distributions. The parameters obtained are further tested by comparison of the calculated BaI vibrational distributions with another research group's experimental results at different collision energy. In addition, the reaction cross-section versus collision energy, product BaI angular distribution and alignment are obtained by QCT calculations on the PES. The possible reaction configurations are also discussed upon the calculations.