Basic study of abrasive behavior in the new lapping technology using electric field

2016 ◽  
Vol 2016.11 (0) ◽  
pp. C30
Author(s):  
Takayuki KUSUMI ◽  
Hiroshi IKEDA ◽  
Ryuta NAKAMURA ◽  
Yoichi AKAGAMI
1998 ◽  
Vol 118 (11) ◽  
pp. 1291-1297
Author(s):  
Toshinori Tsuji ◽  
Masahisa Otsubo ◽  
Chikahisa Honda ◽  
Michihiro Uchiumi ◽  
Katsunori Muraoka ◽  
...  

2012 ◽  
Vol 2012.9 (0) ◽  
pp. 151-152
Author(s):  
Shogo CHIBA ◽  
Masuhiro TSUCHIDA ◽  
Yasuharu KEMURIYAMA ◽  
Tatsuo TAKAHASHI ◽  
Ryuta NAKAMURA ◽  
...  

2012 ◽  
Vol 2012.9 (0) ◽  
pp. 155-156
Author(s):  
Takayuki KUSUMI ◽  
Ryuta NAKAMURA ◽  
Yasuhiro SATO ◽  
Yoichi AKAGAMI ◽  
Noritsugu UMEHARA

2013 ◽  
Vol 79 (1) ◽  
pp. 87-92 ◽  
Author(s):  
Takayuki KUSUMI ◽  
Yasuhiro SATO ◽  
Hiroshi IKEDA ◽  
Yoichi AKAGAMI ◽  
Noritsugu UMEHARA

1997 ◽  
Vol 117 (7) ◽  
pp. 1069-1070
Author(s):  
Shinji Yasuda ◽  
Yasuo Nishikori ◽  
Minoru Murano ◽  
Teruya Kouno

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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