激光场中正电子对氢原子的电离反应

本文在一级Bom近似下，研究了激光场中正电子对基态氢原子的碰撞电离反应，并与入射粒子为电子的（e，2e）反应进行了对比．激光场中正电子态和敲出电子态分别采用Volkov波函数和Coulomb-Volkov波函数，靶原子的缀饰波函数由含时微扰论给出．计算结果显示激光缀饰的三重电离截面明显依赖于入射粒子电荷符号．激光越强，二者差距越大．     

激光场中正电子对氢原子的电离反应

本文在一级Born近似下,研究了激光场中正电子对基态氢原子的碰撞电离反应,并与入射粒子为电子的(e,2e)反应进行了对比.激光场中正电子态和敲出电子态分别采用Volkov波函数和Coulomb-Volkov波函数,靶原子的缀饰波函数由含时微扰论给出.计算结果显示激光缀饰的三重电离截面明显依赖于入射粒子电荷符号.激光越强,二者差距越大.     

激光辅助的电子偶素对反质子的反氢生成反应

在一级玻恩近似下, 研究了在激光辅助的电子偶素-反质子碰撞中的反氢合成. 发现在小角范围内, 平行于电子偶素入射方向极化的激光使反氢生成截面变小. 在中等角度范围, 截面有一定的增加, 特别当偏振方向垂直于入射方向时, 截面增加比较明显.     

激光辅助的电子对氢原子的自由-自由跃迁

在一级玻恩近似和软光子近似下 ,研究了激光场中电子对氢原子基态的自由 自由跃迁,并考虑入射电子对束缚电子的交换效应 .发现Kroll Watson截面求和规则在大角度遭到明显破坏. In the first Born approximation and the soft-photon approximation, the laser-assisted electron-atomic-hydrogen free-free transition is investigated with taking the exchange effect into acount. We find that the Kroll-Watson sum rule is significantly violated in the backward direction.     

激光场中电子碰撞氢原子电离三重微分截面

本文用CPB(Coulomb-Projected Born)近似和GCPB(Generalised Coulomb-Projected Born)近似对激光场中电子与氢原子碰撞电离的三重微分截面及平均吸收或发射光子数进行了计算,并将结果与P.Cavaliers等(1980)的Born近似结果进行了比较。     

会聚线偏振强激光场中氢原子的能态变化

本文研究氢原子在会聚的线偏振强激光场中原子势的变化以及由此而引起的原子能级移位和波函数的空间扩展问题.结果表明,变化后的原子势等价于半径由外场决定而荷电量为核电荷的振荡球壳的势.在此势下,原子能级将变浅和分裂,波函数的空间分布将增大.     

激光场中电子与氢原子的散射：Ⅱ.低频近似下的计算

本文在多重散射理论的框架下,研究了低频激光场中电子与氢原子的散射。计算了激光场中电子与基态氢原子弹性散射的微分截面,讨论了微分截面随光子数、散射角以及入射电子能量的变化规律,并与别人的结果作了比较。     

激光场中H原子多光子电离速率

建立了激光与原子相互作用的伪分立态模型,并用此模型计算了激光场中Ｈ原子的多光子电离速率。对于光子能量较小的激光,计算结果与其它理论计算结果相符合。     

飞秒强激光场中氢原子团簇的各向异性膨胀

利用LAMMPS程序研究了氢原子团簇在飞秒强激光场下的动力学行为, 讨论了引起小氢原子团簇各向异性膨胀的原因.通过对外电离过程中团簇内部电子的行为以及团簇各个方向上最外层质子距离团簇中心的距离随时间的变化情况的分析, 发现团簇的膨胀呈现各向异性,且引起这种各向异性的根源在于团簇内部电子的抖动以及逃逸.对氢原子团簇与强激光场相互作用过程中质子各能量分量以及各向异性程度随时间变化情况进行了研究,发现各向异性程度是随时间变化的, 这种各向异性程度首先随着激光电场的增强而增加,随后又逐渐减小,直到最后趋于某一大于1的稳定值.分析了激光脉冲结束后质子的平均能量与观测角之间的关系, 并将分析结果与Ditmire小组的实验结果进行了比较,发现我们的模拟结果在定性上与实验相符合.     

反氢原子研究的新结果

由哈佛大学Gerald Gabrielse领导的ATRAP合作组于2002年首次用反质子和正电子生成了冷的反氢原子．他们使用一系列的磁与电冷阱，产生了大约170000个反氢原子，但是并没有测量这种反原子的能量、速度或温度，只是简单地假定它们的温度与禁闭反质子和正电子的设备的温度相同(4．2K)．     

Electron-Helium Atom Collisions in the Presence of a Bichromatic Laser Field

The differential cross section （DCS） for electron-helium atom collisions in the presence of a bichromatic CO2 laser field is investigated as a function of the scattering angle θ by employing first-Born approximation （FBA） with a simple screening electric potential. We discuss in detail the influence of the scattering geometry, the photon energy and the number of photons exchanged on the DCSs. These illustrate that the three factors have important effects on the elastic scattering and the screening electric potential is effective.     

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.     

Collisional Radiative Involvement of Molecules into Resonance with the IR Laser Field in a Two-Component Molecular Medium

Journal of Experimental and Theoretical Physics - Collisional radiative involvement of molecules not absorbing IR laser radiation into resonance with a laser field has been investigated for the...     

Optical Pumping of Samarium Atoms in a Bichromatic Laser Field in the Presence of Velocity-Changing Collisions

Dark resonances in the ¹⁵⁴Sm -system 4f ⁶6s ²(⁷ F ₀) 4f ⁶6s6p(⁹ F ₁ ⁰) 4f ⁶ s ²(⁷ F ₁) are observed alongside the velocity selective optical pumping. The shape of the resulting spectra strongly depended on the buffer gas (He, Ar) pressure due to velocity-changing collisions (VCC): the sign of the effect could be reversed from the dark to the bright resonance. The observed spectra are interpreted within the framework of the hard-sphere collision model. The role of VCC in the formation of the dark state in the -system is discussed.     

Photon Angular Distribution and Polarization of Radiative Recombination

A systematic study is carried out on the angular distribution and polarization of photons emitted following radiative-recombination of bare and He-like ions of Ne, At, Ni and Mo with a unidirectional electron beam. In order to incorporate the screening effect due to inner-shell electrons, a distorted wave method is used. Scaling rules for polarization of the photon following radiative recombination to both bare and He-like ions are given for the incident energy regions up to six times the ionization threshold energy of the final state.     

Differential Cross Section and Polarization of Radiative Recombination

The formulae of photon angular distribution and polarization degree for radiative recombination are presented to include the contribution of multipoles and their correlations. A fully relativistic code is then developed to calculate the photon angular distribution and polarization. The calculated polarization degree and differential cross-sections agree well with that of Scofild＇s results within 10%. The effects of multipoles on polarization and angular distribution are investigated. The polarization and the angular distribution become asymmetric when the multipoles are accounted as the electron energy increases.     

用于辐射复合与双电子复合实验的低能离子闪烁探测器

为了在CSRm的电子冷却器上进行辐射复合以及双电子复合实验, 需要探测能量小于4 MeV/u的离子, 因此设计了新的置于超高真空环境的CsI(Tl)闪烁探测器, 探测器采用的光电倍增管为R7525(Hamamatsu）。 介绍了新闪烁探测器的结构, 并对其进行了性能测试。 测试结果表明, 该探测器对高、 低能离子均有良好的响应, 探测器的信号十分明显。 探测器的最高计数率可以达到106 ions/s, 并且探测器附近的真空度可达10-10 Pa量级, 能够满足辐射复合与双电子复合实验以及储存环对真空的要求, 为今后在CSRm上进行复合实验打下了良好的基础。 A new CsI(Tl) scintillation detector readout with R7525 PMT(Hamamatsu）is designed to detect low energy (<4 MeV/u) ions in radiative recombination and dielectronic recombination experiments at the main cooler storage ring in Lanzhou. The structure of the scintillator detector is described in this paper. The detector is tested with α source and ion beams, respectively. The signals from background, 200 MeV/u C6+ and alpha radioactive source are recorded and analyzed. The results show that the detector has good response to high and low energy ions. The maximum counting rate of the detector can reach 106 ions/s and the vacuum level near the detector can reach 10-10 Pa, both are good for recombination experiments. The installation of the new detector to CSRm is of great help for future radiative recombination and dielectronic recombination experiments.     

Rigid Motions in the Presence of a Magnetic Field

It is shown that, in the standard framework of non-relativistic quantum mechanics, the presence of a magnetic field implies that there are no operators representing those translations or rotations that do not leave invariant the magnetic field, and the corresponding components of the linear or angular momentum are undefined. Pacs: 03.65.-w. 02.20.-a     

辐射复合截面的扭曲波计算

采用非相对论量子计算方法计算了电子与高电荷态离子碰撞的辐射复合截面, 其中连续态电子的波函数是由扭曲波近似方法(DWBE)获得. 计算了低能电子与中、低核电荷的高电荷态离子(类H和类Li)的辐射复合截面, 并与采用有效电荷的库仑波计算结果进行了比较, 说明了扭曲波计算的重要性.     

Calculation of the Interelectronic-Interaction Correction to Radiative Recombination of an Electron with a Heavy He-Like Ion

We present a calculation of the interelectronic-interaction correction of first order in 1/Z for radiative recombination of an electron with a heavy He-like ion in the ground state. A rigorous relativistic treatment is demonstrated which includes the Coulomb, Breit and retarded parts of the interelectronic interaction. A complete relativistic evaluation is compared with two frequently used approximations. This revised version was published online in July 2006 with corrections to the Cover Date.