场发射枪
加速电压
阴极射线
扫描电子显微镜
电子枪
材料科学
梁(结构)
电子
电子束诱导沉积
电压
能量色散X射线光谱学
场电子发射
光学
热离子发射
法拉第杯
静电透镜
高压
显微镜
物理
扫描透射电子显微镜
离子束
核物理学
量子力学
作者
D. Phifer,L. Tuma,T. Vystavěl,Petr Wandrol,R.J. Young
出处
期刊:Microscopy Today
[Cambridge University Press]
日期:2009-06-26
卷期号:17 (4): 40-49
被引量:37
标识
DOI:10.1017/s1551929509000170
摘要
Abstract Beam Deceleration is a relatively simple method to reduce electron beam energy and improve imaging parameters such as resolution and contrast. The scanning electron microscope (SEM) uses a sharply focused electron beam to probe the specimen surface. The energy of the electrons forming such a probe is determined by the electrical potential of the electron source, referred to as accelerating voltage or high voltage (HV). No matter how many times the electrons are accelerated or decelerated inside the column, they leave the column with an energy corresponding to the high voltage. The high voltage is usually controllable within a range of 200 V to 30 kV for most commercially available SEMs, allowing the operator to select the electron beam energy suitable for the application. Imaging with very low electron beam energy has great importance, which is illustrated by SEM instrumentation development over the last few decades [1–2]. Low voltage microscopy is a topic discussed at most microscopy-related conferences these days, but generally, it is approached with an immersion lens and field emission gun (FEG) SEM system because of the better beam current densities. However, beam deceleration is also a means to bring low kV improvement to SEMs with thermionic electron sources.
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