Multi-Electron Processes in ^13C^6＋ Ions with Neon Collisions in Energy Region 4.15-11.08 keV/u

The cross-section ratios of double-, triple-, quadruple-, and the total multi-electron processes to the single electron capture process （σ^DE/σ^SC, σ^TE/σ^SC, σ^QE/σ^SC and σ^ME/σ^SC） as well as the relative ratios among reaction channels in double-electron active, triple-electron active and quadruple-electron active are measured in ^13C^6＋_Ne collision in the energy region of 4.15-11.08keV/u by employing position-sensitive and time-of-flight coincident techniques. It is determined that the cross-section ratios σ^DE /σ^SC, σ^TE /σ^SC, σ^QE /σ^SC and σ^ME /σ^SC are approximately the constants of 0.20 ± 0.03, 0.16 ± 0.04, 0.06 ± 0.02 and 0.42 ± 0.05. These values are obviously smaller than the predictions of the molecular Coulomb over-the-barrier model （MCBM） [J. Phys. B 23 （1990） 4293], the extended classical over-the-barrier model （ECBM） [J. Phys. B 19 （1986） 2925] and the semiempirical scaling laws （SL） [Phys. Rev. A 54 （1996） 4127]. However, the relative ratios among partial processes of DE, TE and QE are found to depend on collision energy, which suggests that the collision dynamics depends on the collision velocity. The limitation of velocity-independent character of ECBM, MCBM and SL is undoubtedly shown.     

Ar16+和Ar17+离子与Zr作用产生的X射线谱

将超导离子源提供的10—20keV/q Ar¹⁶⁺和Ar¹⁷⁺离子入射到Zr金属表面，在相互作用中产生的X射线谱表明，高电荷态Ar¹⁶⁺离子在金属表面中性化过程中有可能存在多电子激发，使Ar¹⁶⁺的K壳层电子被激发形成空穴，在退激过程中发射特征Kα-X射线.空心原子Ar的K层发射X射线强度随入射离子的动能而减弱，靶原子Zr的L壳层发射X射线强度随入射离子动能的增加而增强.Ar¹⁷⁺的单离子的Kα-     

非全裸氟离子与氦原子碰撞中的转移电离过程

采用位置灵敏探测和散射离子 反冲离子飞行时间测量技术 ,测量了强相互作用区氟离子与氦原子碰撞中的转移电离截面与单电子俘获截面之比 .实验发现 ,该比值随作用强度的增加而减小 .在本工作能区 ,转移电离现象可视作一个电子被俘获、另一个电子被电离的两步过程 ;He原子二重电离的主要机制为两步机制. The cross-section ratios of the transfer ionization to the single electron capture of helium induced by fluorine ions in the strong-interaction region were measured by means of the position-sensitive-detecting and the time-of -flight (TOF) technologies. Is is found that the cross section ratios decrease with the increasing of the interaction-strength κ in this work. In the energy range of this work, the transfer ionization can be considered as a two-step process that one electron is captured by projectile...     

Transfer ionization of the isocharge sequence ion and Ar collisions

The ratios of transfer ionization to single capture for isocharge C^{q+}, N^{q+}, O^{q+}, Ne^{q+} ions on Ar atoms are measured by using position-sensitive and time-of-flight techniques. It is found that the ratio R_{1} increases with nuclear charge Z in a q=4 sequence, and the ratio R_{1} sequences have the minimum values at Z=7 and Z=8 in q=5 and q=6 sequences, respectively, and the ratio R_{1} decreases with the increase in the nuclear charge Z in a q=7 sequence. The results may be explained within the frame of the statistical model. It may be concluded that the transfer ionization depends remarkably upon the electronic structure of the projectile. The projectiles used in this study have the same charge state and velocity, but different electronic structures. The dependence of the ratio R_{1} on q is studied for Ne^{q+}-Ar collisions. The ratio R_{1} is found to increase as q increases for Ne^{q+}－Ar collisions. The measured dependence of the ratio R_{1} on q is compared with the calculation using the molecular Coulomb over-barrier model.     

HIRFL-CSR实验环团簇内靶的首批测试实验

内靶装置是兰州重离子冷却储存环(HIRFL-CSR)实验环的一个重要的插入件,也是世界上第一个嵌入在重离子储存环中的内靶装置,它位于HIRFL-CSR实验环的一个直线段.团簇内靶具有传统外靶所不具备的一些优点,如高亮度、高精度和高灵敏度等.这些优点可使我们在内靶实验平台上进行一些高精度的物理实验.为满足不同物理实验的需求,内靶可以有两种工作模式:非极化靶运行模式和极化靶运行模式,用于为实验环内的物理实验提供厚度为1011~1013atoms/cm2的非极化靶和极化靶.团簇靶是属于非极化靶运行模式,它采用超声喷气和冷凝相结合的方法获得团簇粒子束,并在碰撞靶室中与环内束流相碰撞,未反应的团簇束被收集级抽走.团簇内靶可以提供靶密度约为2×1013atoms/cm2的Ne、Ar、Kr、Xe和N2、CH4等团簇束.目前已完成了团簇靶的现场安装和准直,并进行了真空达标、喷嘴冷却和稳定性等首批测试实验.本文主要介绍团簇靶的工作原理和首批测试实验结果.