955 resultados para Slow highly charged ion (SHCI)


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The cross-section ratios of double-, triple-, quadruple-, and the total multi-electron processes to the single electron capture process sigma(DE)/sigma(SC), sigma(TE)/sigma(SC), sigma(QE)/sigma(SC) and sigma(ME)/sigma(SC)) as well as the relative ratios among reaction channels in double-electron active, triple-electron active and quadruple- electron active are measured in C-13(6+) -Ne collision in the energy region of 4.15-11.08 keV/u by employing position-sensitive and time-of-flight coincident techniques. It is determined that the cross-section ratios sigma(DE)/sigma(SC), sigma(TE)/sigma(SC), sigma(QE)/sigma(SC) and sigma(ME)/sigma(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.

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The commissioning of the cooler storage rings (CSR) was successful, and the facility provides new possibilities for atomic physics with highly charged ions. Bare carbon, argon ions, were successfully stored in the main ring CSRm, cooled by cold electron beam, and accelerated up to 1 GeV/u. Heavier ions as Xe44+ and Kr28+ were also successfully stored in the CSRs. Both of the rings are equipped with new generation of electron coolers which can provide different electron beam density distributions. Electron-ion interactions, high precision X-ray spectroscopy, complete kinematical measurements for relativistic ion-atom collisions will be performed at CSRs. Laser cooling of heavy ions are planned as well. The physics programs and the present status will be summarized.

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The status of the HIRFL (Heavy Ion Facility in Lanzhou) - Cooler Storage Ring (CSR) at the IMP is reported. The main physics goals at the HIRFL-CSR are the researches on nuclear structure and decay property, EOS of nuclear matter, hadron physics, highly charged atomic physics, high energy density physics, nuclear astrophysics, and applications for cancer therapy, space industries, materials and biology sciences. The HIRFL-CSR is the first ion cooler-storage-ring system in China, which consists of a main ring (CSRm), an experimental ring (CSRe) and a radioactive beamline (RIBLL2). The two existing cyclotrons SFC (K=70) and SSC (K=450) are used as its injectors. The 7MeV/u12C6+ ions were stored successfully in CSRm with the stripping injection in January 2006. After that, realized were the accelerations of C-12(6+), Ar-36(18+), Kr-78(28+) and Xe-129(27+) ions with energies of 1GeV/u, 1GeV/u, 450 MeV/u and 235 MeV/u, respectively, including accumulation, electron cooling and acceleration. In 2008, the first two isochronous mass measurement experiments with the primary beams of Ar-36(18+) and Kr-78(28+) were performed at CSRe with the Delta p/p similar to 10(-5).

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We report the measurements of relative cross sections for single capture (SC), double capture (DC), single ionization (SI), double ionization (DI), and transfer ionization (TI) in collisions of Xe23+ ions with helium atoms in the velocity range of 0.65-1.32 a.u. The relative cross sections show a weak velocity dependence. The cross-section ratio of double-(DE) to single-electron (SE) removal from He, sigma(DE)/sigma(SE), is about 0.45. Single capture is the dominant reaction channel which is followed by transfer ionization, while only very small probabilities are found for pure ionization and double capture. The present experimental data are in satisfactory agreement with the estimations by the extended classical over-barrier (ECB) model..

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Molybdenum L-shell X-rays were produced by Xeq+ (q = 25-30) bombardment at low energies from 2.65 to 4.55 keV/amu (350-600 keV). We observed a kinetic energy threshold of Mo L-shell ionization down to 2.65-3.03 keV/amu (350-400 keV). The charge state effect of the incident ions was not observed which shows that the ions were neutralized, reaching an equilibrium charge state and losing their initial charge state memory before production of L-shell vacancies resulted in X-ray production. The experimental ionization cross sections were compared with those from Binary Encounter Approximation theory. Taking into account projectile deflection in the target nuclear Coulomb field, the ionization cross section of Mo L-shell near the kinetic energy threshold was well described. (C) 2010 Published by Elsevier B.V.

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We studied the characteristic X-ray spectra produced by the interaction of highly charged ions of X-129(q+) (q =25, 26, 27) with surface of metallic Mo. The experimental result shows that highly charged ions can excite the characteristic X-ray spectra of L-shell of Mo when the beam' s intensity is not more than 120 nA. The X-ray yield of single ion reaches a quantitative level of 10(-8) and increases with the increment of the ion' s kinetic energy and ionic charge (potential energy). By measuring the X-ray spectra of Mo-L alpha(1) the M-level lifetime of Mo atom is estimated by using Heisenberg uncertainty relation.

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高电荷态离子与固体表面相互作用的研究是目前国际上广受关注的热点研究领域之一。本论文详细介绍了在兰州重离子加速器国家实验室ECR离子源上建成的高电荷态离子表面物理实验平台;着重叙述了在实验平台上完成的高电荷态离子在固体表面引起的离子溅射和电子发射的研究。我们用初动能Ek=216~720keV的高电荷态Pb36+离子和初动能为Ek=144~288keV的Arq+(q =11~16)离子以不同入射角度(Ψ=15º~80º)作用于Nb、Si和SiO2表面,通过研究离子溅射产额与入射离子初动能、势能(电荷态)和入射角度的关系,得到了以下结论:离子溅射产额与炮弹离子的势能沉积和动能作用有关;对Ar离子,电荷态从11增加到16时,离子溅射产额是随之增长的。而对Pb36+离子,表面离子溅射产额随入射离子初动能的变化关系跟核阻止能损随入射离子初动能的变化关系是一致的,离子溅射产额与核阻止能损是线性相关的。认为高电荷态引发的表面离子溅射过程是势能沉积作用与线性级联碰撞过程协同作用的结果。我们还测量了Heq+(q=1,2, Ek=12keV~48keV),Neq+(q=2~8, Ek=18~192keV),Arq+(q=3~12, Ek=72keV)离子垂直作用于Si, W, Au表面产生的电子发射产额。得到了纯粹势能电子发射产额与入射离子势能的定量关系,势能电子产额随入射离子势能的增加而线性增加,势能每增加1eV,单离子电子发射产额增加0.0088(以初动能为42keV的Neq+入射到W表面为例)。势能电子发射增量跟靶的性质有关,W表面对势能变化的响应最剧烈,其次是Si表面。通过引入纯粹动能电子产额与电子能损的比值B分析和研究了动能电子发射,随着入射离子原子序数和初动能的增加,B因子有缓慢降低的趋势;B因子与靶材料密切相关,Au靶的B因子明显大于Si靶和W靶;我们还首次把B因子的研究扩展到高电荷态离子领域,认为B因子与入射离子的势能(电荷态)无关

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本文详细论述了三种各具特色的高电荷态ECR离子源的设计与研制,它们分别是:14.SGHz全永磁高电荷态ECR离子源LAPEC咫、传统常温ECR离子源GTS、混和超导ECR离子源HECRIS。另外,还从理论与实验两个方面对ECR离子源多电荷态离子束流的引出进行了详细研究。设计研制了一台高性能14.SGHz全永磁ECR离子源LAPECRZ,该离子源的设计尺寸为杯50mm*560mm,重量可达9ookg以上,为目前世界上体积与重量最大、设计参数最高的全永磁ECR离子源。全永磁离子源的尺寸增大一些,其加工与研制所存在的难度将会有质的变化。研制LAPEC形所存在的技术难度大大超过了以往所有全永磁ECR离子源。LAPECR2的磁场参数为:注入磁场1 .4T,如果加注入端辅助铁扼,磁场可达2.6T;引出磁场为1 .1T;六极永磁体在弧腔内壁产生的最大径向磁场的设计值为1.22T,实际加工得到的磁场大小为1.2T,与计算结果基本一致。该离子源的设计采用了多种特殊技术与方法以提高引出高电荷态离子束流强度,如:双层含铝衬底的等离子体弧腔、铝制等离子体电极、冷阴极电子枪(注入端负偏压电极)、旁轴微波直接馈入与等离子体位置相对于磁场可调等等。目前,我们已开始源体的组装。GTS离子源为目前世界上运行性能最好的常温ECR离子源之一。它的设计指导思想是ECR离子源的经验结论scaling Laws,高磁场、高磁镜比,高磁场梯度是该离子源磁场设计的主要特点。设计时充分考虑了多频加热机制,允许多频功率同时馈入弧腔:IOGHz+14GHz+18GHz+ZSGHz。良好的磁场约束、灵活的磁场结构设计、高频率大功率微波馈入、大体积弧腔、足够的冷二次电子注入、优良的真空抽气系统、以及有效的束流引出系统等等都是该离子源高性能表观的原因。经过近一年半的优化与调试,该离子源运行性能优良,能产生很多领先国际伺类ECR源的离子束流,如:1.95emAO6+,O·semAArll”,o.15e拜AArl犷,31Oe瘩建叙e,哪se拼A豁岁”与0.4eμAXe39+为18GHz时调试的结果:1.OemAAr8+,1.8eμAAr17+24OeμAXe20+ ,20eμAxe30+与0.3oe从Axe38+为在14GHz调试的最好结果。该离子源已多次为原子物理实验提供了Ar17+与Ar18+等高电荷态离子束流。HECRIS是一台高性能混和超导ECR离子源,其各项设计参数均高于GTS源,以保证该离子源能具有比GTS更好的性能。它的最小B场型设计继续沿袭现在ECR离子源设计惯用的Scaling Laws设计思想。该离子源采用较高频率的微波馈入,设计运行范围为18GHz-24GHz。该离子源着重于在运行调试中实现对轴向最小磁场Bmin的调节与匹配,这里采用两组超导线包进行辅助调节。径向磁约束由一个能在弧腔内壁产生1.6T径向磁场的六极永磁体提供,它强磁场设计与部分磁块存在的退磁问题的解决也是该离子源的一大特点与难点。文中还详细讨论一个高性能的Halbach结构六极永磁体的设计方法。分别从永磁材料选取、物理尺寸优化、结构选择等角度,结合理论分析与PolssON,PERMAG和TOscA3D程序的模拟计算结果,对六极永磁体的性能进行了全面的分析,提出两种确定六极永磁体中存在退磁磁块的办法,并且提出了一种用高极化矫顽力永磁材料替代退磁磁块中所采用的永磁材料的解决办法。对多电荷态ECR离子源的引出进行了理论与实验两方面的研究。利用PBGUNS程序,对ECR离子源的引出系统进行了一定的理论分析。通过模拟计算,详细地论述了引出系统的各主要物理参数对ECR离子源引出离子束流品质的影响。这些得到的结果,对设计一套高性能的ECR离子源引出系统具有一定的指导意义。结合理论分析,我们还设计完成了一系列关于ECR离子源引出系统的实验,来研究多电荷态离子束流的引出与短距离传输。采用电扫描发射度测量系统(ESS)探测离子束流在x与y方向的发射度,用两个荧光靶分别在束运线不同位置探测束流的束斑形状,并利用一个亮度探测器对束斑相对亮度进行探测。通过多组实验结果的处理,分别分析了离子源的几个主要参数如磁场、微波、掺气、偏压等对引出束流品质的影响并结合相关理论给予了解释,通过对混合多电荷态离子束流的三电极引出实验结果的讨论,建立了一个关于高电荷态ECR离子源束流引出的较为清晰的物理图象。

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本工作采用散射离子位置灵敏探测和反冲离子飞摘.时问符合技术,在小于一300keV的能量范围内,研究了高电荷态Xe离子(q=15,17,19,21,23)与He原子碰撞中双电子转移截面与单电子转移截而比与入射离子电荷态的关系;研究了入射离子电荷态q=4,5,6,7的等电荷态序列Cq+、Nq+、Oq+、Neq+与He原子碰撞中,电子转移截面比与入射离子原子序数的关系。对Xeq++ He碰撞体系,主要研究了靶原子完全转移两个电子(σ2)与完全转移一个电子(σl)的截面比σ2/σl与入射离子电荷态的依赖关系。对靶原子双电子过程提出一步过程假定,修正了ECB模型。通过与已有绝对截面的比较,得到了很好的符合结果。使用修正模型计算的截面比解释了本实验的截面比测量结果。对等电荷态序列Cq+、Nq+、Oq+、Neq+与He原子的碰撞,主要研究了转移电离与单俘获截面比与入射离子原子序数的依赖关系。在统计模型的理论框架下,引入势能参数。Ω研究发现,等电荷序列的转移电离与单俘获截面比与碰撞系统的。有很强的依赖关系,说明单电子俘获形成的能量沉积是引起转移电离的主要因素。本工作还研究了势能参数几对碰撞系统的转移电离与双俘获之间的相互关系的影响。结果表明,。对转移电离和双俘获在靶原子双电子过程中的比率权重起着决定性作用。

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Ferric uptake regulator (Fur) is a global regulator involved in multiple aspects of bacterial life. The gene encoding the Vibrio harveyi Fur (Fur(vh)) was cloned from a pathogenic V. harveyi strain isolated from diseased fish. Furvh shares 77% overall sequence identity with the Escherichia coli Fur (Fur(Ec)) and could complement a mutant of Fur(Ec). Like Fur(Ec), Fur(Vh), possesses two cysteine residues at positions 92 and 95, yet unlike Fur(Ec), in which these cysteine residues constitute part of the metal ion coordination site and hence are vital to the repressor activity, C92 and C95 of Fur(Vh) proved to be functionally inessential. Further study identified a Vibrio Fur signature sequence, which is preserved in all the ten Vibrio Fur proteins that have been discovered to date but in none of the non-vibrio Fur proteins. Site-directed and random mutation analyses of the signature residues, the cysteine residues, and seven highly charged amino acid residues indicated that D9, H32, C137, and K138 of Fur(vh) are functionally important but D9, C137, and K138 can be replaced by more than one functional substitutes. Systematic deletion analysis demonstrated that the C-terminal 12 residues of Fur(Vh) are functionally inessential. These results (i) indicated that the activation mechanism, or certain aspects of which, of Fur(Vh) is possibly different from that of Fur(Ec); and (ii) suggested that it is not very likely that the C-terminal 12 residues play any significant role in the activation or stability of Fur(Vh); and (iii) provided insights into the potential function of the local structure involving C137 and K138.

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The electron impact ionization of highly charged ions is investigated. Using a relativistic distorted wave Born approximation, we explore the possible effects that should be observable in a high-energy electron impact ionization (e, 2e) coincidence experiment involving multi-charged ions. We present calculations of triple-differential cross sections. We will focus on relativistic and distortion effects and consider geometries where these may be easily observed.

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The spectroscopy and metastability of the carbon dioxide doubly charged ion, the CO22+ dication, have been studied with photoionization experiments: time-of-flight photoelectron photoelectron coincidence (TOF-PEPECO), threshold photoelectrons coincidence (TPEsCO), and threshold photoelectrons and ion coincidence (TPEsCO ion coincidence) spectroscopies. Vibrational structure is observed in TOF-PEPECO and TPEsCO spectra of the ground and first two excited states. The vibrational structure is dominated by the symmetric stretch except in the TPEsCO spectrum of the ground state where an antisymmetric stretch progression is observed. All three vibrational frequencies are deduced for the ground state and symmetric stretch and bending frequencies are deduced for the first two excited states. Some vibrational structure of higher electronic states is also observed. The threshold for double ionization of carbon dioxide is reported as 37.340+/-0.010 eV. The fragmentation of energy selected CO22+ ions has been investigated with TPEsCO ion coincidence spectroscopy. A band of metastable states from similar to38.7 to similar to41 eV above the ground state of neutral CO2 has been observed in the experimental time window of similar to0.1-2.3 mus with a tendency towards shorter lifetimes at higher energies. It is proposed that the metastability is due to slow spin forbidden conversion from bound excited singlet states to unbound continuum states of the triplet ground state. Another result of this investigation is the observation of CO++O+ formation in indirect dissociative double photoionization below the threshold for formation of CO22+. The threshold for CO++O+ formation is found to be 35.56+/-0.10 eV or lower, which is more than 2 eV lower than previous measurements. (C) 2005 American Institute of Physics.

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We have studied the dielectronic recombination process in He-like Fe ions and have obtained the resonant strengths of the KLn (3 less than or equal to, n less than or equal to, 5) resonances. This measurement was performed with the use of an electron beam ion trap by measuring the x-ray energy emitted from highly charged ions simultaneously with the electron beam energy scanned during the measurement. The total resonant strengths obtained are 5.0 x 10(-19), 2.1 x 10(-19) and 1.1 X 10(-19) cm(2) eV, for KLM, KLN and KLO, respectively.

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The electron beam ions traps (EBITs) are widely used to study highly charged ions (HCIs). In an EBIT, a high energy electron beam collides with atoms and ions to generate HCIs in the trap region. It is important to study the physics in the trap. The atomic processes, such as electron impact ionisation (EI), radiative recombination (RR), dielectronic recombination (DR) and charge exchange (CX), occur in the trap and numerical simulation can give some parameters for design, predict the composition and describe charge state evolution in an EBIT [Phys. Rev. A 43 (199 1) 4861]. We are presently developing a new code, which additionally includes a description of the overlaps between the ion clouds of the various charge-states. It has been written so that it can simulate experiments where various machine parameters (e.g. beam energy and current) can vary throughout the simulation and will be able to use cross- sections either based on scaling laws or derived from atomic structure calculations. An object-oriented method is used in developing the new software, which is an efficient way to organize and write code. (C) 2003 Elsevier Science B.V. All rights reserved.

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Dielectronic recombination (DR) has been studied in highly charged He-like Ti ions using an electron beam ion trap. X-rays emitted from radiative recombination (RR) and DR were observed as the electron beam energy was scanned through the resonances. Differential DR resonant strengths were determined by normalizing the DR x-ray intensity to the RR intensity using theoretical RR cross sections. KLn (2 less than or equal to n less than or equal to 5) resonant strengths were determined for He-like Ti ions. The differential resonant strengths were calibrated without reference to any theoretical DR calculations while the electron energy scale was derived with reference to the well-known energy for ionization of the He-like and H-like ions from the ground state. Calibration in this way facilitates a more exacting comparison between theory and experiment than has been reported previously. To facilitate this comparison, total and differential theoretical resonance strengths were calculated. These calculations were found to be in good agreement with the measured results.