排序方式: 共有91条查询结果,搜索用时 343 毫秒
41.
双粒子模型的基础是描述原子之间相互作用势为EAM(embedded atom method)势的Monte Carlo模拟. 模型建议:在Ni3Al晶界弛豫时,微量元素原子既被看作为偏析子又被看作为诱发子. 作为偏析子它在晶界偏析(或富集),作为诱发子它诱发Ni原子在晶界偏析(或富集). 可见本模型能解析共偏析(或共富集)现象. 根据正(或诱发子)效应与负(或偏析子)效应的联合影响,模型解释了Ni在Ni3Al晶界最明显富集现象.
关键词:
偏析子与诱发子
基体效应
在晶界共富集
晶界内聚性 相似文献
42.
Rabi Oscillations and Coherence Dynamics in Terahertz Streaking-Assisted Photoelectron Spectrum 下载免费PDF全文
We present an approach,a Terahertz streaking-assisted photoelectron spectrum(THz SAPS),to achieve direct observations of ultrafast coherence dynamics with timescales beyond the pulse duration.Using a 24 fs probe pulse,the THz SAPS enables us to well visualize Rabi oscillations of 11.76 fs and quantum beats of 2.62 fs between the 5S1/2 and 5P3/2 in rubidium atoms.The numerical results show that the THz SAPS can simultaneously achieve high resolution in both frequency and time domains without the limitation of Heisenberg uncertainty of the probe pulse.The long probe pulse promises sufficiently high frequency resolution in photoelectron spectroscopy allowing to observe Autler-Townes splittings,whereas the streaking THz field enhances temporal resolution for not only Rabi oscillations but also quantum beats between the ground and excited states.The THz SAPS demonstrates a potential applicability for observation and manipulation of ultrafast coherence processes in frequency and time domains. 相似文献
43.
44.
45.
46.
Energy loss of a fast-electron beam due to the excitation of collective oscillation in hot plasma 下载免费PDF全文
Energy loss due to a fast-electron beam interacting with the hot plasma at a high density is analysed theoretically. By splitting the particle density fluctuations into the individual part due to the random thermal motion of the individual electrons and the collective part due to plasma-wave excitation, we are concerned with the collective interaction of the relativistic plasma electrons resulting from the Coulomb interactions. Consequently, we derive the frequency of the hot plasma and the "Debye length" with the modification of the relativistic effect. And finally we calculate the energy loss of a fast-electron beam due to the excitation of collective oscillation in the hot plasma. 相似文献
47.
48.
49.
50.
为了模拟钍基熔盐堆(TMSR)材料的中子辐照损伤,基于中国科学院上海应用物理研究所(SINAP)的4 MV静电加速器,研制了一台专用的离子束辐照装置。装置主要由束流传输线和高温、高真空靶室组成。束流传输线装有用于束流磁场扫描和束流监测的设备。装置可提供H^+,He^+,Ar^+等束流用于离子束辐照,束流最高能量4 Me V,最大流强2μA。辐照温度范围为液氮温度至950℃。辐照面积最大为30 mm×30mm。装在靶室的由旋转铝片构成的变能器对束流能量进行调制,可以在样品中得到均匀的辐照损伤。初步的实验结果表明,装置适用于高温合金及其他熔盐堆材料的辐照损伤研究。 相似文献