Guiding of 150 keV O6+ ions through nanocapillaries in an uncoated Al2O3 membrane: special time dependence of the transmission profile width

This paper reports that the transmission of O6+ ions with energy of 150keV through capillaries in an uncoated Al2O3 membrane was measured, and agreements with previously reported results in general angular distribution of the transmitted ions and the transmission fractions as a function of the tilt angle well fitted to Gaussian-like functions were observed. Due to using an uncoated capillary membrane, our c is larger than that using a gold-coated one with a smaller value of E-p/q, which suggests a larger equilibrium charge Q(infinity) in our experiment. The observed special width variation with time and a larger width than that using a smaller E-p/q were qualitatively explained by using mean-field classical transport theory based on a classical-trajectory Monte Carlo simulation.

高电荷态离子与Si(110)晶面碰撞的沟道效应研究

不同电荷态低速离子(Arq+，Pbq+)轰击Si(110)晶面，测量不同入射角情况下的次级粒子的产额. 通过比较溅射产额与入射角的关系，证实沟道效应的存在. 高电荷态离子与Si相互作用产生的沟道效应说明溅射产额主要是由动能碰撞引起的. 在小角入射条件下，高电荷态离子能够增大溅射产额. 当高电荷态离子以40°—50°入射时，存在势能越高溅射产额越大的势能效应.

Study of n=2, Delta n=0 transition of Be-, B-, C-, N- and O-like sequence in the beam-foil spectrum of titanium

The foil-excited the spectrum of highly stripped titanium ions between 12-40 nm has been studied. Titanium ions of 80 and 120 MeV were provided by the HI-13 tandem accelerator at the China Institute of Atomic Energy. GIM-957 XUV-VUV monochromator was refocused to get highly-resolved spectra. Our experimental results and the published spectral data of laser-produced plasma show agreement in nearly all cases within +/- 0.03 nm. The spectra contained some weak or strong lines previously unclassified. These spectral lines mainly belong to 2s2p(2) for TiXVIII, 2p(3) for TiXVIII, 2s2p(3) for TiXVII, 2p(6)4p for Ti XII and 2p(6)3d for Ti XII transitions.

TIME-DEPENDENT DENSITY FUNCTIONAL STUDY OF MULTIELECTRON TRANSFER IN Cq+-Na-4 COLLISIONS

The process of multielectron transfer from a Na-4 cluster induced by highly charged C6+, C4+, C2+ and C+ ions is studied using the method of time-dependent density functional theory within the local density approximation combined with the use of pseudopotential. The evolution of dipole moment changes and emitted electrons in Na-4 isobtained and the time-dependent probabilities with various charges are deduced. It is shown that the Na-4 cluster is strongly ionized by C6+ and that the number of emitted electrons per atom of Na-4 is larger than that of Na-2 under the same condition. One can find that the detailed information of the emitted electrons from Na-4 is different from the same from Na-2, which is possibly related to the difference in structure between the two clusters.

近玻尔速度高电荷态离子与表面作用诱发的溅射离子能谱

近玻尔速度高电荷态离子在物质表面诱发的溅射离子能谱研究在理论和实验上尚是一片空白。本工作针对溅射离子能谱测量，设计、建立了一台径向位置灵敏127o柱形静电离子能谱仪。该谱仪结合位置灵敏探测器，克服了传统静电谱仪只能通过扫描电场单次、单能量点取谱的缺陷，实现了分段取谱——单次可获取宽为0.85Ec ≤ E ≤ 1.15Ec的能谱，极大提高了实验测量效率。利用该谱仪，首次获得了0.8至1.8倍玻尔速度Ar7，8，9+离子与金属铍靶和高定向性石墨靶碰撞产生的溅射离子能谱（入射角45o ，出射角135o）。结果表明：1）能谱分布很宽，其峰值位于130eV至600eV之间，远大于线性级联碰撞区的几到十几eV；且峰位随入射离子速度增加向高能方向略有移动。2）铍靶的溅射能谱呈一个极不对称的峰分布——高能部分有很长的尾巴，下降趋势服从E-n分布；其能谱与入射离子速度关联很大，小于vBohr时指数n与线性级联碰撞接近，而大于vBohr时非线性贡献明显。3）石墨靶的能谱峰位与入射离子动能、势能相关；其谱形在上升到最大值后均出现一个很宽的平台，表明该系列碰撞系统中，非线性效应占主导

高电荷态离子与固体表面作用的研究

高电荷态离子与固体表面相互作用研究不仅在原子结构和能级寿命，量子电动力学效应和等离子体物理等方面具有重要的基础研究价值，而且在表面分析和加工，短波辐射源开发等方面也有着潜在的应用价值。论文介绍了在兰州重离子加速器国家实验室ECR离子源上建成的用于高电荷态离子与固体表面作用研究的物理实验终端，研究了高电荷态离子与固体表面作用中的可见光和X射线发射以及高电荷态离子在固体表面引起的离子溅射产额和电子发射产额。研究了固体表面靶原子特征可见光谱和X射线的激发机制；分析了空心原子X射线谱的重要特征以及高电荷态离子动能沉积和势能沉积在表面离子溅射和表面电子发射中的作用

高电荷态238Uq+在碳膜中电荷平衡时间的研究

离子通过物质过程中与靶原子发生碰撞，碰撞中大量电子被俘获和电离。当电子俘获截面与电离截面达到平衡时，出射离子的电荷态分布达到一个平衡的分布，这个分布与入射离子的核电荷数、速度、壳层结构以及靶材料的性质有关。研究离子通过物质后的电荷态分布和电荷平衡时间对于研究高电荷态离子穿越物质层时的电荷转换及平衡过程具有重要意义。 本文论述了能量为0.8 MeV/u 238Uq+离子通过不同厚度碳膜后的电荷态分布，并对铀离子在碳膜中的电荷平衡时间进行了研究。 实验中束流采用兰州重离子加速器国家重点实验室（HIRFL）首次加速出的能量为0.8 MeV/u 238U26+离子束。本实验是首次在兰州放射性次级束流线（RIBLL）实验终端进行，采用的实验方法新颖。为了研究不同初始电荷态的铀离子通过不同厚度碳膜后的电荷态分布，实验中采取让初级束流 238U26+通过0.1µm厚度碳膜后形成一个电荷态分布，通过调节二极磁铁的控制电流从中选择某一电荷态轰击碳靶，进行电荷态分布研究。 实验对0.8 MeV/u 238Uq+(q=26，29，34，39)通过不同厚度碳膜（5µg/cm2，15µg/cm2，26µg/cm2和225µg/cm2）后的电荷态分布进行了研究。结果发现：能量为0.8 MeV/u的铀离子通过5µg/cm2厚度碳膜后，出射铀离子的电荷态分布未达到平衡；同样铀离子通过15µg/cm2厚度碳膜后，出射铀离子的电荷态分布已达到平衡，平衡平均电荷态为33.72+；由此通过计算得到铀离子在碳膜中的电荷平衡时间为1/3×5.4fs<=t<=5.4fs

高电荷态氩离子与原子碰撞中的多电子转移过程研究

本工作建立起了符合关联测量实验装置，包括反冲离子飞行时间谱仪、散射离子位置灵敏探测器、差分拉瓦型气体喷嘴、基于微机的多参数数据获取系统以及数据分析和处理程序。在入射离子能量在80KeV～240KeV范围内，利用该装置系统研究了Arq++He，Arq++Ne和Arq++Ar（q=8，9，11，12）碰撞体系中的多电子转移规律，实验鉴别了反应中发生的各种多电子转移过程，测量了反应截面，获得了一批新的实验数据。 对于Arq++He碰撞体系，本工作主要研究了He原子的转移电离相对截面与入射离子能量和电荷态的规律，发现相对截面在所研究能区基本与入射离子能量无关，并利用核间势垒和复合分子的经典图象，描述了此碰撞体系转移电离过程发生的两种可能途径，估计了相对截面的经典上限，发现在此碰撞体系中，转移电离过程中电子关联作用起着重要的作用。 本工作系统研究了Arq++He和Arq++Ar碰撞体系中多电子转移反应截面与入射离子能量、电荷态和反冲离子电荷态的变化规律，以及反冲离子电荷态分布。研究发现，在低能高电荷态离子与多电子靶原子碰撞反应中，碰撞系统的相对运动动能对碰撞体系中的电子转移过程基本没有贡献；系统所具有的势能是碰撞体系中电子转移和靶原子电离的主要因素；在相同的入射离子条件下，靶原子电离能对电子转移有重要影响；碰撞反应中单电子过程占主要地位，而在多电子转移过程中，转移电离过程发生的几率一般大于纯的多电子俘获几率；入射离子单电子俘获截面、总电荷交换截面与入射离子电荷态成正比关系；入射离子电荷交换截面随离子俘获电子数目的增加而单调减小；入射离子俘获一个电子时，转移电离截面随反冲离子电荷态的升高而单调下降，而入射离子俘获电子数多于一个时，转移电离截面存在极大值分布现象，而且分布宽度随入射离子电荷态的升高具有增加的趋势。 本工作在分析实验现象和分子经典库仑过垒模型MCBM的基础上，提出基于MCBM描述，把高电荷态离子与原子碰撞反应中的电子转移过程分为四阶段描述的新想法，即：入射过程中的分子化→复合分子形成→复合分子解离和中间态离子的形成→多电子激发态散射离子和靶离子向末态的自电离衰变。并依据能量守恒原理，规范了处理多电子激发态离子发生自电离衰变的规则。在此基础上，对Arq++He和Arq++Ar碰撞体系中的电子转移截面进行了理论计算，通过与实验结果的对比研究发现，对在中间态形成的多电子激发态散射离子，根据这些规则进行自电离衰变修正后计算得到的结果与实验符合很好，因此，对多电子激发态离子的自电离修正是合理的，而且多电子激发态离子的自电离衰变是低能高电荷态离子与原子碰撞反应中转移电离过程发生的主要因素。

A STUDY ON 2E SPECTRA OF BIPHENYL DERIVATIVES

A study of doubly charged ion mass spectra (2E spectra), the substituents effect and the target gas pressure deppendence of biphenyl derivitives was presented in this work. The decomposition of doubly charged ion formed in the ion source is dominant by the losses of H, C2H2, C2H4 and HR(R represents substituent). [C12H8]2+, [C12H6]2+ and [C10H6]2+ among others are the most stable product ions. The substituents effect is Various in different decomposition reactions, and in some cases it can not be predicted by Hammett equition. While the TIC of 2E spectra was markedly influenced by the target gas pressure, but the fragmentation pattern of the 2E spectra is independent of it.

On the adsorption of hexaammineruthenium (III) at anionic self-assembled monolayers

The binding of the electroactive hexaammineruthenium (III) complex ions to anionic self-assembled monolayers (SAMs) has been investigated by means of chronocoulometry and ac voltammetry. From chronocoulometric data recorded in 10-2 M LiClO4 containing different [Ru(NH3)6]3+ concentrations, we have established the adsorption isotherm of [Ru(NH3)6]3+ on a compact monolayer of 2-mercaptobenzimidazole-5-sulfonate (MBIS) self-assembled on Au(1 1 1). The data were satisfactorily fitted to the linearized Langmuir adsorption isotherm and a binding constant of 4.0 (±0.4) × 106 M-1 has been determined. The electrostatic binding of [Ru(NH3)6]3+ to a dilute PNA-DNA monolayer formed after hybridization on a PNA-modified gold electrode by self-assembly from a mixed solution of mercaptobutan-1-ol and PNA oligonucleotides has been studied by ac voltammetry. The admittance of the PNA-modified electrode after hybridization with complementary DNA was measured in 0.01 M Tris-HCl buffer containing different [Ru(NH3)6]3+ concentrations. Based on these data, a binding constant of [Ru(NH3)6]3+ to the surface-confined PNA-DNA duplex was derived from the Langmuir isotherm and amounts to 2.9 (±0.3) × 105 M-1. As the interactions between [Ru(NH3)6]3+ and the immobilized PNA-DNA hybrids on the gold surface are essentially electrostatic, the adsorption of the highly charged cationic redox complex at low concentrations to the negatively charged PNA-DNA modified surface is in large competition with other monovalent cations present in the electrolyte at higher concentrations. The influence of competing sodium cations was thus studied by adding different NaCl concentrations in the 0.01 M Tris-HCl electrolyte. © 2008 Elsevier Ltd. All rights reserved.

Research supervision and psychotherapeutic theory: bridging the research-practice-gap

Research supervision in the field of counselling and psychotherapy is a fruitful area for investigation in view of the fact that the research supervisory relationship is powerful and highly charged, whether consciously acknowledged or not. Researchers trained as counsellors and psychotherapists possess the skills to facilitate the emergence of, and work creatively with, impasses and crises, both in the research itself and the supervisory relationship, as a result of their training and experience in dealing with crisis and catharsis in clinical work. This paper will demonstrate these points using a case vignette from my work as a supervisor of research dissertations undertaken by students on a Masters in Therapeutic Counselling course. Drawing on narrative analysis, clinical supervision theory and discursive analysis it will look at the strengths and weaknesses of a 'psychotherapeutic' approach to research supervision.

Secondary threshold laws for multiple ionization of atoms

We propose a physical mechanism that leads to the emergence of secondary threshold laws in processes of multiple ionization of atoms. We argue that the removal of n electrons (n>2) from a many-electron atom may proceed via intermediate resonant states of the corresponding doubly charged ion. For atoms such as rare gases, the density of such resonances in the vicinity of subsequent ionization thresholds is high. As a result, the appearance energies for multiply charged ions are close to these thresholds, while the effective power indices mu in the near-threshold energy dependence of the cross section, sigmaproportional toE(mu), are lower compared to those from the Wannier theory. This provides a possible explanation of the recent experimental results of B. Gstir [Nucl. Instrum. Methods Phys. Res. B 205, 413 (2003)].

Experimental investigation of the processes determining x-ray emission intensities from charge-exchange collisions

Absolute cross sections have been measured for single and double charge exchange and x-ray line emission for highly charged ions of C, N, 0, and Ne colliding with He, H-2 CO2, and H2O at collisions energies of 7q keV. Present results of charge exchange in He and H-2 compare favorably with previous results. For CO2 and H2O, where prior work is scarce, the classical overbarrier model is found to overestimate results by up to a factor of 3. An analysis of the relative intensities of the observed Lyman x-ray transitions indicates that capture into l states is not statistical, as collision velocities are insufficient to populate the highest angular-momentum states. The importance of autoionization following multiple capture is highlighted, and enhanced radiative stabilization following double capture is observed and compared to other studies. Present results are also discussed in terms of mechanisms likely to generate x-ray emission in comets.

Measurement of charge exchange and X-ray emission cross sections for solar wind-comet interactions

X-ray emission from a comet was observed for the first time in 1996. One of the mechanisms believed to be contributing to this surprisingly strong emission is the interaction of highly charged solar wind ions with cometary gases. Reported herein are total absolute charge-exchange and normalized line-emission (X-ray) cross sections for collisions of high-charge state (+3 to +10) C, N, O, and Ne ions with the cometary species H2O and CO2. It is found that in several cases the double charge-exchange cross sections can be large, and in the case of C3+ they are equal to those for single charge exchange. Present results are compared to cross section values used in recent comet models. The importance of applying accurate cross sections, including double charge exchange, to obtain absolute line-emission intensities is emphasized.