scholarly journals Electron transverse energy distribution in GaAs negative electron affinity cathodes: Calculations compared to experiments

1996 ◽  
Vol 80 (3) ◽  
pp. 1809-1815 ◽  
Author(s):  
G. Vergara ◽  
A. Herrera‐Gómez ◽  
W. E. Spicer
2005 ◽  
Vol 251 (1-4) ◽  
pp. 182-190 ◽  
Author(s):  
Xiaobing Zhang ◽  
Wei Lei ◽  
Min Liu ◽  
Laibin Zhang ◽  
Daniel den Engelsen ◽  
...  

2012 ◽  
Vol 51 ◽  
pp. 046402 ◽  
Author(s):  
Shunya Matsuba ◽  
Yosuke Honda ◽  
Xiuguang Jin ◽  
Tsukasa Miyajima ◽  
Masahiro Yamamoto ◽  
...  

2001 ◽  
Vol 79 (4) ◽  
pp. 739-748
Author(s):  
F -H Liu

Based on the model of nuclear-collision geometry, the independent N–N collision picture and participant contribution picture are used to describe the transverse-energy distribution in p–A collisions at high energy. In the independent N–N collision picture, the energy loss of leading proton in each p–N collision is considered. The calculated results are in agreement with the experimental data of p–Al, p–Cu, and p–U collisions at 200 GeV/c. PACS Nos.: 13.85-t, 13.85Hd, 25.75-q


1986 ◽  
Vol 447 ◽  
pp. 475-478 ◽  
Author(s):  
T. Akesson ◽  
Y. Choi ◽  
P. Dam ◽  
G. DiTorre ◽  
C. Fabjan ◽  
...  

1998 ◽  
Vol 509 ◽  
Author(s):  
J.E. Yater ◽  
A. Shih

AbstractSecondary electron emission spectroscopy is used to examine the emission characteristics of diamond films as a function of the bulk and surface properties. We find significant variation in the secondary electron yields measured from diamond surfaces even when energy distribution measurements indicate that a low or negative electron affinity is present. In particular, we observe that the material properties, such as bulk and surface uniformity, surface composition, and impurity and defect concentrations, have a strong affect on the secondary electron yield measurements. Furthermore, the energy distribution of the emitted electrons is found to vary with adsorbate species. In certain cases, the energy distribution changes with adsorbate coverage even though the measured electron intensity remains unchanged. From an analysis of the data, we identify bulk and surface properties needed to optimize the emission characteristics.


1988 ◽  
Vol 38 (3) ◽  
pp. 397-402 ◽  
Author(s):  
T. Åkesson ◽  
Y. Choi ◽  
P. Dam ◽  
G. DiTorre ◽  
C. W. Fabjan ◽  
...  

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