scholarly journals Local versus Global Optimization of Electron Lens System Design

Author(s):  
Neda Hesam Mahmoudi Nezhad ◽  
Mohamad Ghaffarian Niasar ◽  
Cornelis Wouter Hagen ◽  
Pieter Kruit
2017 ◽  
Vol 46 (4) ◽  
pp. 422001
Author(s):  
刘鹏 LIU Peng ◽  
刘钦晓 LIU Qin-xiao ◽  
周海洋 ZHOU Hai-yang ◽  
江城 JIANG Cheng ◽  
余飞鸿 YU Fei-hong

2007 ◽  
Author(s):  
Tao Ren ◽  
Jun Chang ◽  
Zhi-cheng Weng ◽  
Huilin Jiang ◽  
Xiaojie Cong

2010 ◽  
Vol 18 (12) ◽  
pp. 13285 ◽  
Author(s):  
Lei Li ◽  
Qiong-Hua Wang ◽  
Xiao-Qing Xu ◽  
Da-Hai Li

2014 ◽  
Vol 53 (29) ◽  
pp. H146
Author(s):  
Chen-Hung Lin ◽  
Li-Jen Hsiao ◽  
Jing-Ting Hsaio ◽  
Hoang Yan Lin

2008 ◽  
Vol 8 (4) ◽  
pp. 1439-1452 ◽  
Author(s):  
Christian Gagné ◽  
Julie Beaulieu ◽  
Marc Parizeau ◽  
Simon Thibault

2008 ◽  
Vol 23 (3) ◽  
pp. 193-204 ◽  
Author(s):  
Masaharu Tanaka ◽  
Yohei Akimoto ◽  
Jun Sakuma ◽  
Isao Ono ◽  
Shigenobu Kobayashi

Author(s):  
G. F. Rempfer

In photoelectron microscopy (PEM), also called photoemission electron microscopy (PEEM), the image is formed by electrons which have been liberated from the specimen by ultraviolet light. The electrons are accelerated by an electric field before being imaged by an electron lens system. The specimen is supported on a planar electrode (or the electrode itself may be the specimen), and the accelerating field is applied between the specimen, which serves as the cathode, and an anode. The accelerating field is essentially uniform except for microfields near the surface of the specimen and a diverging field near the anode aperture. The uniform field forms a virtual image of the specimen (virtual specimen) at unit lateral magnification, approximately twice as far from the anode as is the specimen. The diverging field at the anode aperture in turn forms a virtual image of the virtual specimen at magnification 2/3, at a distance from the anode of 4/3 the specimen distance. This demagnified virtual image is the object for the objective stage of the lens system.


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