利用半导体光电阴极的光电子束进行选择性电子光束扫描电镜成像

T. Nishitani, Y. Arakawa, S. Noda, A. Koizumi, D. Sato, H. Shikano, H. Iijima, Y. Honda, H. Amano
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引用次数: 2

摘要

使用InGaN半导体的光电阴极的脉冲电子束为扫描电子显微镜带来了选择性扫描技术,在扫描电子显微镜中,电子束的照射强度和面积可以在扫描电子显微镜图像的视场内任意选择。利用金属有机化学气相沉积设备中生长的p型InGaN半导体晶体,在超高真空条件下,将其表面在电子枪中激活至负电子亲和态,作为电子束源的光电阴极材料。InGaN半导体光电阴极产生的脉冲电子束上升和下降时间为3ns,与用于光激发电子的辐照脉冲激光器的时间结构一致。在15 μA束流下,经过23次表面活化和连续束流操作,InGaN光电阴极电子枪的总束流运行时间为1300 h,停机率为4%,电流稳定性为0.033%。将InGaN光电阴极电子枪取代原场发射电子枪安装在传统扫描电镜中。扫描电镜成像采用选择性电子光束,将扫描电镜系统的扫描信号与激光同步,以任意强度照射扫描电镜图像中的任意区域。在扫描电镜的电视扫描速度(80 ns/像素,25帧/秒)下,选择电子束对扫描电镜图像区域的选择精度是逐像素的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Scanning electron microscope imaging by selective e-beaming using photoelectron beams from semiconductor photocathodes
Pulsed electron beams from a photocathode using an InGaN semiconductor have brought selectively scanning technology to scanning electron microscopes, where the electron beam irradiation intensity and area can be arbitrarily selected within the field of view in SEM images. The p-type InGaN semiconductor crystals grown in the metalorganic chemical vapor deposition equipment were used as the photocathode material for the electron beam source after the surface was activated to a negative electron affinity state in the electron gun under ultrahigh vacuum. The InGaN semiconductor photocathode produced a pulsed electron beam with a rise and fall time of 3 ns, consistent with the time structure of the irradiated pulsed laser used for the optical excitation of electrons. The InGaN photocathode-based electron gun achieved a total beam operation time of 1300 h at 15  μA beam current with a downtime rate of 4% and a current stability of 0.033% after 23 cycles of surface activation and continuous beam operation. The InGaN photocathode-based electron gun has been installed in the conventional scanning electron microscope by replacing the original field emission gun. SEM imaging was performed by selective electron beaming, in which the scanning signal of the SEM system was synchronized with the laser for photocathode excitation to irradiate arbitrary regions in the SEM image at arbitrary intensity. The accuracy of the selection of regions in the SEM image by the selective electron beam was pixel by pixel at the TV scan speed (80 ns/pix, 25 frame/s) of the SEM.
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