钡原子6p3/2ns自电离里德伯态的研究

用激光多步激发技术研究了处于6p1/2电离限以下的6p3/2ns自电离态的光谱。 并利用最新的R矩阵的计算结果, 结合多通道量子亏损理论进行了理论分析。 理论结果与实验光谱相符合。     

钡原子6p3/2ns自电离里德伯态的研究

用激光多步激发技术研究了处于６ｐ１／２电离限以下的６ｐ３／２ｎｓ自电离态的光谱。并利用最 Ｒ矩阵的计算结果,结合多通道量子亏损理论进行了理论分析,理论结果与实验光谱相符合。     

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。     

Ca和Sr原子nˊdnl自电离态在低电场中的线性Stark效应

用激光多步激发技术观察了Ca和Sr原子n’dnl双电子激发自电离态的电场效应。Stark光谱显示,在F<1/3n~5的低电场中,Stark能级分裂与外电场强度线性相关。也观察了近简并l亚能级的Stark混合使自电离共振谱线在外电场中的增宽。这一效应在高温等离子体中对双电子复合速率的增加起重要作用。     

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。     

Ca和Sr原子n′dnl自电离态在低电场中的线性Stark效应

用激光多步激发技术观察了Ca和Sr原子n′dnl双电子激发自电离态的电场效应。Stark光谱显示,在F<1/3n⁵的低电场中,Stark能级分裂与外电场强度线性相关。也观察了近简并l亚能级的Stark混合使自电离共振谱线在外电场中的增宽。这一效应在高温等离子体中对双电子复合速率的增加起重要作用。 关键词：     

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：     

n(Zn)∶n(Ga)比值对合成ZnGa_2O_4结构及光致发光性能的影响

以ZnO和HGaO2为原料,用不同配比合成出系列ZnGa2O4,并对其晶体结构和发光性能进行了研究。用荧光分光光度计检测了ZnGa2O4的激发和发射光谱,用X射线衍射仪检测了ZnGa2O4的衍射图谱,用热重差热仪绘制了TGA-DAT曲线。对检测结果分析认为:1·ZnGa2O4属于尖晶石结构,稍过量的Zn或Ga能进入ZnGa2O4结构中,并对ZnGa2O4的晶格常数产生一定影响。2·ZnGa2O4存在两个自激发光中心,当Ga稍过量时,自激发光中心是四面体镓氧键[Td(Ga—O)],最大激发波长约248nm,最大发射波长约367nm;当Zn稍过量时,自激发光中心是八面体镓氧键[Oh(Ga—O)],最大激发波长约270nm,最大发射波长约441nm。当n(Zn)∶n(Ga)在理论值附近,激发和发射光强度最大,而且光谱峰位发生了红移。3·ZnGa2O4的热稳定性能非常好。上述结论对研究ZnGa2O4基质或掺杂的发光材料具有一定意义。     

电子离子碰撞过程中的共振激发双自电离

利用相对论修正扭曲波玻恩近似, 计算了类钠离子Ti11+ 和Cr13+ 的电子碰撞直接电离, 激发自电离和共振激发双自电离截面. 理论数据与实验结果在整个能区内很好符合. 共振激发双自电离截面对总截面的贡献约为20%-30%, 对速率系数的影响较大, 不可忽略.     

spin-Peierls系统低能量激发谱的理论研究

用玻色化技术和量子自洽方法研究了spin-Peierls系统的低能量激发谱,计算了二聚化相的基态、单粒子激发态和双粒子束缚态的能量、阻挫对其低能量行为的影响及其各自的自旋-自旋关联函数.结果表明,随着阻挫的增大,spin-Peierls系统中的基态能会逐渐减小,单粒子激发态能隙和双粒子束缚态能隙却会增大.双粒子束缚态和基态的关联函数具有类似的短程关联,而单粒子激发态的关联函数具有长程关联.因此导出,单粒子激发态为自旋三重态,双粒子束缚态与基态类似为自旋单态,它存在于双粒子连续激发态的下边.该结果与Ain等 关键词： spin-Peierls系统 束缚态 关联函数     

铕原子4f76p3/2nd自电离态的光谱

利用三步三色孤立实激发技术(ICE),系统地研究了铕原子4f76p3/2 nd自电离态的光谱,同时首次研究了激光偏振对复杂原子的光谱的影响.为了研究铕原子4f76p3/2 nd自电离态的光谱,首先设计并采用了不同的激发路径,分别将原子布居到同一高激发能域并探测它们在该能域的自电离光谱.通过比较这些光谱的异同并结合上述激发路径所对应的跃迁选择定则,便可唯一地确定这些高激发态的总角动量.为了研究激光偏振对铕原子的影响,设计并使用了两种偏振组合:三步激光都是垂直(πππ),三步激光都是平行(σσσ)(激光偏振方向相对于探测器垂直或平行).为了得到有偏振影响的光谱,分别使3部激光器处于同一偏振,依次对铕原子进行激发,激发路径与终态同上.通过对同一路径不同偏振下的光谱的比较,发现仅能确定极少数的高激发态的总角动量,同时在光谱中一些峰独立于另一偏振光谱存在.     

Photoionisationsmessungen an Atomstrahlen

Using a crossed beam photoelectric technique, relative photoionization cross sections have been determined in the spectral region 1200 to 1600 Å. Apart from confirming (and sometimes extending) earlier results obtained by absorption and emission methods, this yielded the profiles of the extremely wide autoionizing lines of AgI.     

Eu原子4f~76p_(3/2)ns自电离态的光谱的研究(英文)

采用孤立实激发技术,对铕原子4f~76p_(3/2)ns(n=7,8)自电离态的光谱进行了系统的研究,同时是首次在不同激光偏振组合下进行的研究。首先,用前两束激光分步将铕原子从基态4f~76s~2经中间4f~76s6p态激发至4f~76sns里德堡态,然后再用第三束激光通过离子实4f~76s~+→4f~76p~+_(3/2)的跃迁将其进一步激发至4f~76p_(3/2)7s自电离态或4f~76p_(3/2)8s自电离态。对铕原子4f~76p_(3/2)ns(n=7,8)自电离态复杂的光谱分别给出了详细的解释,从中我们可以获得一些重要的光谱信息,比如自电峰的能级位置和线宽等,同时还可以观察到收敛于不同离子限的自电离系列之间的组态相互作用。最后,通过比较不同激光偏振组合下的自电离光谱,确定了一些自电离态的总角动量的值。     

铕原子4f76pns系列自电离态的光谱和动力学过程

通过共振激发技术和速度影像法对铕原子4f⁷6pns（n=7,8）自电离态进行了系统性的研究。首先采用三步共振激发技术探测光谱,通过前两步固定波长的激光将铕原子激发到4f⁷6p²态上后扫描第三步激光的波长,使得三步激光的能量总和位于铕原子4f⁷6pns（n=7,8）自电离态能域附近,从而得到该自电离态的光谱;然后采用速度影像法对其动力学过程进行探测,经过数据分析得到铕原子4f⁷6pns（n=7,8）自电离态的衰变分支比和弹射电子的角分布。不仅从光谱中观察到了强烈的组态相互作用并且确定了部分能态的总角动量,从自电离弹射电子角分布中观察到铕原子4f⁷6pns（n=7,8）自电离态复杂的物理机制,还在该能域内观测到了粒子数反转。最后,本文还对孤立实激发技术在探测低n值自电离态光谱的适用性进行了讨论。     

Saturation effects on Ba 6phi （l=0, 2） and 6pnk （｜M｜= 0, 1） autoionization spectra

Using a three-step laser saturation excitation technique, the saturation effects on the Ba 6pns （J = 1） and 6pad （J = 1, 3） autoionization spectra are observed systemically in zero field. These saturation spectra are introduced to determine the high n members of 6pnl （l = 0, 2） autoionizing series and are used to analyse the channel interactions among the autoionizing series in zero field. Furthermore, the saturation excitation technique is applied to the electric field case, in which the saturation spectra of Ba 6pnk （｜M｜= 0, 1） autoionizing Stark states are measured. Most of these saturation spectra are observed for the first time so far as we know, which indicate the mixing of the autoionizing states in the electric fields.     

Spectroscopic properties of Ba 6pjnk autoionizing Stark series

With a combination of the isolated core excitation (ICE) technique and a proper polarization configuration of three lasers, both the 6p_1/2nk and 6p_3/2nk autoionizing Stark states excited from the 6snk Stark states with have been measured for the first time. The experimental results are analyzed by fitting them to the Lorentzian profiles, from which the positions and widths are determined at various electric-field strengths. The experimental results indicate that the 6p_1/2nk and 6p_3/2nk autoionizing Stark states have different spectroscopic properties due to the difference of their cores.     

Branching ratios of autoionization from Eu 4f~76p_(1/2)6d [J] autoionizing states

The autoionization branching ratios from Eu 4f76p1/26 d [J] autoionizing states to its 4f76s+(9So), 4f76s+(7So), and4f75d+(9Do) final ionic states are investigated with the combination of the three-step laser excitation and the velocity-map imaging technique. These different autoionizing states are excited via 4f76s6d8 DJ [J = 5/2, 7/2, and 9/2] intermediate states, respectively. The experimental photoelectron images are obtained, from which energy distributions of ejected electrons are achieved with the mathematical transformation. Furthermore, the energy dependence of the branching ratio is investigated within the autoionization resonance, by which population inversion is observed as an important characteristic.The J-dependence is also studied systematically. The validity of the well-known isolated core excitation technique used for obtaining the autoionization spectrum is also studied.     

Eu原子4f~76p_(3/2)6d自电离过程的动力学特性

采用孤立实激发技术(isolated-core excitation, ICE)及速度影像技术(velocity-map imaging,VMI),研究了Eu原子4f~76p_(3/2)6d自电离过程的动力学特性.孤立实激发技术用于将Eu原子从基态4f~76s~(2 8)S_(7/2)经中间态4f~76s6p激发到4f~76s6d里德堡态,然后将其进一步激发至4f~76p_(3/2)6d自电离态;速度影像技术用于探测其自电离过程的动力学特性,从而获得自电离衰变的分支比(branch ratio, BR)和弹射电子的角分布(angular distribution, AD).自电离衰变的分支比代表离子的能量分布,从中获得VMI影像的径向信息;而通过各向异性参数描述的弹射电子的角分布揭示了VMI影像的角向信息.此外,讨论了自电离衰变分支比和弹射电子角分布在整个自电离共振能域内的变化情况.基于4f~76s~+和4f~75d~+两个离子态的分支比,讨论了实现Eu离子粒子数反转的可能性.     

Experimental study of autoionizing states of AuI

This paper describes the investigation of the autoionizing states of AuI by exciting the states of 6d ² D _3/2 and 6d D _5/2 with tunable dye lasers by means of a resonance ionization time-of-flight mass spectrometer (RI-TOFMS). Many new autoionizing states were found, a few of which have narrow-linewidths of about 0.1 cm^–1. The photoionization efficiencies for different channels were compared. Among the autoionizing states found so far, the highest photoionization yield is given by two newly obtained states from the state 6d ² D _5/2, 3683.6 cm^–1 and 4636.5 cm^–1 above the first ionization limit. In addition, the Shore-Fano profile parameters of several autoionizing resonances were determined by a nonlinear fitting program.     

The study of autoionizing states of the samarium atom

The investigation of the samarium (Sm) atom autoionizing states, belonging to the 4f⁶ 6pnl and 4f⁵ 5d6snl (l=0, 2) configurations, has been carried out by using a three-step isolated-core-excitation (ICE) scheme. Fifty-seven new autoionizing states of the Sm atom have been observed in the energy region between 60,700 and 66,500 cm^?1. These autoionizing states are classified into five autoionization series in the light of different ionization limits. In most cases, the transition profiles of these autoionizing states are nearly symmetric, from which the peak positions and widths can be easily obtained by Lorentzian-profile-fitting procedure. Some autoionizing states have multi-peak profiles whose spectroscopic properties are analyzed in order to understand the complicated structures.