共查询到20条相似文献,搜索用时 11 毫秒
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D. M. Bhardwaj D. C. Jain S. Dalela Ravi Kumar N. L. Saini K. B. Garg 《Physica B: Condensed Matter》2004,350(4):366-374
We have made the XAFS measurements at the Cr–K-edge on natural Indian ruby single crystals (corundum) and its two irradiated samples with fluence 1×1012 Ni6+ and 5×1012 Ni6+ ions/cm2. Irradiated samples show interesting changes in their physical appearance. XANES measurements show progressive decrease in Δoct value on increase of Ni fluence in irradiated samples. EXAFS measurements on these samples show decrease in Cr–O distance on increase of Ni fluence. Lowering of Δoct value is correlated with the increase of Cr–O distance. 相似文献
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The averaged jet charge characterizes the electric charge of the initiating parton and provides a powerful tool to distinguish quark jets from gluon jets.We predict,for the first time,the medium modification of the averaged jet charge in the heavy-ion collisions at the LHC,where jet productions in p+p collisions are simulated by PYTHIA6,and the parton energy loss in QGP is calculated with two Monte Carlo models of jet quenching:PYQUEN and JEWEL.We found that the distribution of averaged jet charge is significantly suppressed by initial state isospin effects due to the participation of neutrons with zero electric charge during nuclear collisions.The considerable enhancement of the averaged jet charge in central Pb+Pb collisions is observed relative to peripheral collisions,since the jet quenching effect is more pronounced in central collisions.The distinct feature of the averaged jet charge between quark and gluon jets,along with the sensitivity of medium modifications on the jet charge to flavor dependence of the parton energy loss,could be very useful to discriminate the energy loss pattern between quark and gluon jets in heavy-ion collisions. 相似文献
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Nuclear reactions induced by 3·65 A GeV12C-ions and 3·65 GeV protons on target elements55Mn,59Co,nat Ni andnatCu were investigated by using the foil stack activation technique and Ge(Li) gamma-ray spectroscopy. Charge dispersions and mass-yield distributions of radioactive residues were obtained from the parametrization of measured spallation cross sections. Discussion of results from this and other radiochemical reactions of high-energy protons and12C-ions with complex nuclei is presented in terms of the concepts of limiting fragmentation and factorization. 相似文献
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研究了快速双原子分子离子在固体中穿行时,尾流效应对各离子电荷态以及库仑爆炸过程的影响.借助于线性介电响应理论和局域介电函数,离子之间的动力学相互作用势可以表示成对称的屏蔽库仑势和非对称的尾势.通过对分子离子上所有束缚电子的总能量进行变分和求解单个离子的运动方程,自洽地确定出分子离子中每个离子的电荷态.数值结果表明,由于尾流效应的影响,在初始穿行阶段,分子离子中导航离子的电荷数随穿行深度的增加而单调递增,而尾随离子的电荷数则随穿行深度的增加而振荡.但当穿行深度很大时,两个离子的电荷数都趋于具有相同速度的孤立离子的电荷数.此外,还发现分子轴的取向朝入射速度方向偏转 相似文献
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We examine the possibility that one could measure partonic charge symmetry violation (CSV) by comparing neutrino or antineutrino production through charged-current reactions induced by electrons or positrons at a possible electron collider at the LHC. We calculate the magnitude of CSV that might be expected at such a facility. We show that this is likely to be a several percent effect, substantially larger than the typical CSV effects expected for partonic reactions. 相似文献
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A model is proposed that treats electrons at surfaces as a combination of two-dimensional and three-dimensional degrees of
freedom. This yields a simple formula for the surface state induced resonant enhancement of the transfer of electrons through
a surface. The model also yields analytic approximations for the transition between two-dimensional and three-dimensional
distance laws in the correlations between electrons in surface states.
Received 6 August 2002 Published online 31 October 2002
RID="a"
ID="a"e-mail: rainer@sask.usask.ca 相似文献
8.
P. Sigmund L.G. Glazov 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2003,23(2):211-215
The electronic energy loss of a dressed ion penetrating through matter is commonly considered as being synonymous with the
sum of the excitation energies of the target and the projectile in atomic collisions undergone during the passage. We show
that this is not justified in projectile-ionizing collisions and discuss some consequences.
Received 23 October 2002 / Received in final form 1st December 2002 Published online 18 February 2003 相似文献
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Iwona Gulaczyk 《Journal of Molecular Spectroscopy》2009,256(1):86-2394
The Hougen’s formalism of group-theoretical effective Hamiltonian has been extended to include the resonances between the wagging, ν9, and third or fourth excited torsional, 3ν15 and 4ν15, states in methylamine. The presented Hamiltonian treats explicitly these couplings. For each of these bands the rovibrational sublevels belong to all symmetry species of the G12 group of methylamine. On the other hand the vibrational states for ν9 and 4ν15 are symmetric with respect to reflection in the symmetry plane of the NH2 group, and antisymmetric for 3ν15. We have shown that the coupling terms between the ν9 and 3ν15 states are limited to Coriolis-like coupling, and no Fermi-type interactions are allowed. For the coupling between the ν9 and 4ν15 states all kind of interaction terms are possible. 相似文献
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通过测量可见光谱段的轫致辐射(λ=535.1nm)强度,结合等离子体电子密度和电子温度,HL-2A 相似文献
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The electronic energy loss of swift heavy ions (MeV/amu) within a solid results in a highly excited cylindrical zone of some
nm in diameter, within which all atoms may be in motion for some tens of ps (transient local melting). After cooling down,
a defect-rich or even amorphous latent track is left in many cases, especially in insulating materials. The resulting property
alterations (density, micro-structure, morphology, phase composition, etc.) have been investigated for many bulk materials,
while only very few experiments have been carried out with thin-film systems. In the present paper, a summary will be given
of our studies on the transport of matter in thin-film packages induced by irradiation with high-energy ions. These is, on
the one hand, atomic mixing at the interfaces, which is especially pronounced in ceramic systems and which seems to occur
by interdiffusion in the molten ion track. On the other hand, we have discovered a self-organisation phenomenon in swift-heavy-ion-irradiated
NiO layers, which at low fluences first showed periodic cracking perpendicular to the projected beam direction. After application
of high fluences, the NiO layer was reorganised in 100-nm-thick and 1-μm-high NiO lamellae of the same separation distance
(1–3 μm) and orientation as found for the cracks. Both effects can be attributed to transient melting of the material surrounding
the ion trajectory.
Received: 11 November 2002 / Accepted: 12 November 2002 / Published online: 4 April 2003
RID="*"
ID="*"Corresponding author. Fax: +49-711/6853-866, E-mail: bolse@ifs.physik.uni-stuttgart.de 相似文献
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An intense laser radiation (1012 to 1011 W/cm−2) focused on the solid target creates a hot (≥1 keV) and dense plasma having high ionization state. The multiple charged ions
with high current densities produced during laser matter interaction have potential application in accelerators as an ion
source. This paper presents generation and detection of highly stripped titanium ions (Ti) in laser produced plasma. An Nd:glass
laser (KAMETRON) delivering 50 J energy (λ=0.53 μm) in 2.5 ns was focused onto a titanium target to produce plasma. This plasma
was allowed to drift across a space of ∼3 m through a diagnostic hole in the focusing mirror before ions are finally detected
with the help of electrostatic ion analyzer. Maximum current density was detected for the charge states of +16 and +17 of
Ti ions for laser intensity of ∼1011 W/cm−2. 相似文献
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针对国产锗硅异质结双极晶体管(SiGe HBTs), 采用半导体器件模拟工具, 建立SiGe HBT单粒子效应三维损伤模型, 研究影响SiGe HBT单粒子效应电荷收集的关键因素. 分析比较重离子在不同位置入射器件时, 各电极的电流变化和感生电荷收集情况, 确定SiGe HBT电荷收集的敏感区域. 结果表明, 集电极/衬底结内及附近区域为集电极和衬底收集电荷的敏感区域, 浅槽隔离内的区域为基极收集电荷的敏感区域, 发射极收集的电荷可以忽略. 此项工作的开展为下一步采用设计加固的方法提高器件的抗辐射性能打下了良好的基础.
关键词:
锗硅异质结双极晶体管
单粒子效应
电荷收集
三维数值仿真 相似文献
14.
John M. Vail 《辐射效应与固体损伤》2013,168(8):321-327
Some point defect properties can be accurately modeled by describing the ions classically, in terms of the shell model. This is particularly the case for point-defect diffusion in strongly ionic crystals. First, we discuss the issue of what ionic charge should be attributed to shell-model ions, including the possibility of partly covalent materials. We then discuss the issue of what defect charge states are likely to be of experimental interest and at the same time amenable to classical modeling. Finally, we discuss the rather common case where the defect charge is not well localized at a single ionic site, and where the electronic charge distribution of the defect and its neighbors will not remain fixed throughout a diffusion step. 相似文献
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A semi-empirical method to describe the electron structure of free many-electron rare-earth ions has been proposed. The method takes into account the spin–orbit interaction as well as relativistic interactions known as Breit’s terms. It is shown that a set of parameters to calculate the electronic spectrum of a free rare-earth ion with accuracy less than 5% can be limited to an effective nuclear charge of the rare-earth ion and a constant related to the Breit’s terms. Using the known experimental spectra of free rare-earth metals these parameters have been calculated for basic terms of all rare-earth ions. 相似文献
17.
Heavy ions and pulsed lasers are important means to simulate the ionization damage effects on semiconductor materials. The analytic solution of high-energy heavy ion energy loss in silicon has been obtained using the Bethe-Bloch formula and the Kobetich-Katz theory, and some ionization damage parameters of Fe ions in silicon, such as the track structure and ionized charge density distribution, have been calculated and analyzed according to the theoretical calculation results. Using the Gaussian function and Beer's law, the parameters of the track structure and charge density distribution induced by a pulsed laser in silicon have also been calculated and compared with those of Fe ions in silicon, which provides a theoretical basis for ionization damage effect modeling. 相似文献
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Heavy ions and pulsed lasers are important means to simulate the ionization damage effects on semiconductor materials. The analytic solution of high-energy heavy ion energy loss in silicon has been obtained using the Bethe-Bloch formula and the Kobetich-Katz theory, and some ionization damage parameters of Fe ions in silicon, such as the track structure and ionized charge density distribution, have been calculated and analyzed according to the theoretical calculation results. Using the Gaussian function and Beer's law, the parameters of the track structure and charge density distribution induced by a pulsed laser in silicon have also been calculated and compared with those of Fe ions in silicon, which provides a theoretical basis for ionization damage effect modeling. 相似文献
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A comparative study of different energy loss formulations viz. Benton and Henke, Mukherjee and Nayak, Zieglar et al. and Hubert et al. has been done at lower energies (0.5 to 5 MeV/n) with the aim to identify their relative validity in this energy range. Calculated results using these formulations have been compared with experimental results available in literature. 相似文献
20.
采用蒙特卡罗方法计算了低温下C,Si,Ar,Au和U等多种重粒子在等物质的量氘氚等离子体密度1000 g/cm3、热斑直径50 m中的电子能量损失,不同点火形式下入射能量和作用时间,以及燃料约束时间为20 ps条件下的束流强度。通过对数据的分析研究了这些重粒子辐照实现氘、氚燃料快点火的可能性。结果表明,重粒子束流加热等离子体实现快点火理论上可行,而且有一定的优势;较重的离子加热聚变等离子体的效果更好。重粒子束流加热等离子体到聚变温度需要的束流强度在MA左右;单个粒子的能量在GeV以上;相互作用时间为ps以下。 相似文献