High-Brightness Spin-Polarized Electron Source Using Semiconductor Photocathodes

2009 ◽  
Vol 48 (6) ◽  
pp. 06FF02 ◽  
Author(s):  
Tomohiro Nishitani ◽  
Masao Tabuchi ◽  
Yoshikazu Takeda ◽  
Yuji Suzuki ◽  
Kazuya Motoki ◽  
...  
Author(s):  
A. Strojnik ◽  
J.W. Scholl ◽  
V. Bevc

The electron accelerator, as inserted between the electron source (injector) and the imaging column of the HVEM, is usually a strong lens and should be optimized in order to ensure high brightness over a wide range of accelerating voltages and illuminating conditions. This is especially true in the case of the STEM where the brightness directly determines the highest resolution attainable. In the past, the optical behavior of accelerators was usually determined for a particular configuration. During the development of the accelerator for the Arizona 1 MEV STEM, systematic investigation was made of the major optical properties for a variety of electrode configurations, number of stages N, accelerating voltages, 1 and 10 MEV, and a range of injection voltages ϕ0 = 1, 3, 10, 30, 100, 300 kV).


Author(s):  
M. Iwatsuki ◽  
Y. Kokubo ◽  
Y. Harada

On accout of its high brightness, small optical source size, and minimal energy spread, the field emission gun (FEG) has the advantage that it provides the conventional transmission electron microscope (TEM) with a highly coherent illumination system and directly improves the resolving power and signal-to-noise ratio of the scanning electron microscope (SEM). The FEG is generally classified into two types; the cold field emission (C-FEG) and thermal field emission gun (T-FEG). The former, in which a field emitter is used at the room temperature, was successfully developed as an electron source for the SEM. The latter, in which the emitter is heated to the temperature range of 1000-1800°K, was also proved to be very suited as an electron source for the TEM, as well as for the SEM. Some characteristics of the two types of the FEG have been studied and reported by many authors. However, the results of the respective types have been obtained separately under different experimental conditions.


2004 ◽  
Vol 43 (6A) ◽  
pp. 3371-3375 ◽  
Author(s):  
Tetsuya Matsuyama ◽  
Hisaya Takikita ◽  
Hiromichi Horinaka ◽  
Kenji Wada ◽  
Tsutomu Nakanishi ◽  
...  

Vacuum ◽  
2021 ◽  
pp. 110660
Author(s):  
Zufang Lin ◽  
Huanjun Chen ◽  
Juncong She ◽  
Shaozhi Deng ◽  
Jun Chen

2007 ◽  
Author(s):  
A. Mano ◽  
N. Yamamoto ◽  
K. Tamagaki ◽  
S. Okumi ◽  
M. Yamamoto ◽  
...  

2001 ◽  
Vol 40 (Part 1, No. 11) ◽  
pp. 6468-6472
Author(s):  
Tetsuya Matsuyama ◽  
Masayasu Mukai ◽  
Hiromichi Horinaka ◽  
Kenji Wada ◽  
Tsutomu Nakanishi ◽  
...  

Materia Japan ◽  
1998 ◽  
Vol 37 (8) ◽  
pp. 694-696
Author(s):  
Takashi Saka ◽  
Toshihiro Kato ◽  
Tsutomu Nakanishi ◽  
Shoji Okumi ◽  
Hiromichi Horinaka

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