Suppr超能文献

用于扫描电子显微镜时间分辨测量的、采用负电子亲和势光电阴极的脉冲电子枪的亮度评估。

Brightness evaluation of pulsed electron gun using negative electron affinity photocathode developed for time-resolved measurement using scanning electron microscope.

作者信息

Morishita Hideo, Ohshima Takashi, Otsuga Kazuo, Kuwahara Makoto, Agemura Toshihide, Ose Yoichi

机构信息

Research & Development Group, Hitachi, Ltd., 1-280, Higashi-koigakubo Kokubunji-shi, Tokyo 185-8601, Japan; Graduate School of Engineering, Nagoya University, Furo-cho, Chikusa-ku, Nagoya-shi, Aichi 464-8603, Japan.

Research & Development Group, Hitachi, Ltd., 1-280, Higashi-koigakubo Kokubunji-shi, Tokyo 185-8601, Japan.

出版信息

Ultramicroscopy. 2021 Nov;230:113386. doi: 10.1016/j.ultramic.2021.113386. Epub 2021 Sep 4.

Abstract

Temporal changes in carrier relaxations, magnetic switching, and biological structures are known to be in the order of ns. These phenomena can be typically measured by means of an optical-pump & electron-probe method using an electron microscope combined with a pulsed electron source. A photoemission-type pulsed electron gun makes it possible to obtain a short-pulsed electron beam required for high temporal resolution. On the other hand, spatial resolution is restricted by the brightness of the pulsed electron gun used in electron microscopes when a low brightness electron source is used and an irradiation current larger than a certain value is required. Thus, we constructed a prototype pulsed electron gun using a negative electron affinity (NEA) photocathode for time-resolved measurement using a scanning electron microscope (SEM) with high spatiotemporal resolution. In this study, a high-speed detector containing an avalanche photodiode (APD) was used to directly measure waveforms of the pulsed electron beam excited by a rectangular-shape pulsed light with a variable pulse duration in the range of several ns to several μs. The measured waveforms were the same rectangular shape as incident pulsed excitation light. The maximum peak brightness of the pulsed electron beam was 4.2×10 A/m/sr/V with a pulse duration of 3 ns. This value was larger than that of the continuous electron beam (1.6 × 10 A/m/sr/V). Furthermore, an SEM image with image sharpness of 6.2 nm was obtained using an SEM equipped with a prototype pulsed electron gun at an acceleration voltage of 3 kV.

摘要

已知载流子弛豫、磁开关和生物结构的时间变化在纳秒量级。这些现象通常可以通过使用与脉冲电子源相结合的电子显微镜的光泵浦和电子探针方法来测量。光发射型脉冲电子枪使得获得高时间分辨率所需的短脉冲电子束成为可能。另一方面,当使用低亮度电子源且需要大于一定值的辐照电流时,空间分辨率受到电子显微镜中使用的脉冲电子枪亮度的限制。因此,我们构建了一种使用负电子亲和势(NEA)光电阴极的脉冲电子枪原型,用于使用具有高时空分辨率的扫描电子显微镜(SEM)进行时间分辨测量。在本研究中,使用包含雪崩光电二极管(APD)的高速探测器直接测量由脉冲持续时间在几纳秒到几微秒范围内可变的矩形脉冲光激发的脉冲电子束的波形。测量的波形与入射脉冲激发光的形状相同,均为矩形。脉冲电子束的最大峰值亮度在脉冲持续时间为3纳秒时为4.2×10 A/m/sr/V。该值大于连续电子束的亮度(1.6×10 A/m/sr/V)。此外,在3 kV的加速电压下,使用配备脉冲电子枪原型的SEM获得了图像清晰度为6.2纳米的SEM图像。

文献检索

告别复杂PubMed语法,用中文像聊天一样搜索,搜遍4000万医学文献。AI智能推荐,让科研检索更轻松。

立即免费搜索

文件翻译

保留排版,准确专业,支持PDF/Word/PPT等文件格式,支持 12+语言互译。

免费翻译文档

深度研究

AI帮你快速写综述,25分钟生成高质量综述,智能提取关键信息,辅助科研写作。

立即免费体验