Electric Field Ionization of Lithium Atom

2015 ◽  
Vol 35 (6) ◽  
pp. 0602004 ◽  
Author(s):  
马学伟 Ma Xuewei ◽  
马小东 Ma Xiaodong ◽  
戴长建 Dai Changjian
Author(s):  
Patrick P. Camus

The theory of field ion emission is the study of electron tunneling probability enhanced by the application of a high electric field. At subnanometer distances and kilovolt potentials, the probability of tunneling of electrons increases markedly. Field ionization of gas atoms produce atomic resolution images of the surface of the specimen, while field evaporation of surface atoms sections the specimen. Details of emission theory may be found in monographs.Field ionization (FI) is the phenomena whereby an electric field assists in the ionization of gas atoms via tunneling. The tunneling probability is a maximum at a critical distance above the surface,xc, Fig. 1. Energy is required to ionize the gas atom at xc, I, but at a value reduced by the appliedelectric field, xcFe, while energy is recovered by placing the electron in the specimen, φ. The highest ionization probability occurs for those regions on the specimen that have the highest local electric field. Those atoms which protrude from the average surfacehave the smallest radius of curvature, the highest field and therefore produce the highest ionizationprobability and brightest spots on the imaging screen, Fig. 2. This technique is called field ion microscopy (FIM).


2018 ◽  
Vol 98 (5) ◽  
Author(s):  
A. M. Alonso ◽  
L. Gurung ◽  
B. A. D. Sukra ◽  
S. D. Hogan ◽  
D. B. Cassidy

2012 ◽  
Vol 32 (2) ◽  
pp. 0230001
Author(s):  
野仕伟 Ye Shiwei ◽  
戴长建 Dai Changjian ◽  
赵艳红 Zhao Yanhong

2005 ◽  
Vol 72 (3) ◽  
Author(s):  
S. Yamada ◽  
H. Funahashi ◽  
M. Shibata ◽  
K. Kominato ◽  
Y. Kishimoto ◽  
...  

1987 ◽  
Vol 5 (4) ◽  
pp. 287-292 ◽  
Author(s):  
E. P. Vidolova-Angelova ◽  
D. A. Angelov ◽  
S. T. Mincheva ◽  
V. N. Fedoseev ◽  
V. I. Mishin ◽  
...  

1996 ◽  
Vol 76 (19) ◽  
pp. 3530-3533 ◽  
Author(s):  
Hans-Jörg Dietrich ◽  
Klaus Müller-Dethlefs ◽  
Leonid Ya. Baranov

1959 ◽  
Vol 37 (12) ◽  
pp. 1374-1379 ◽  
Author(s):  
Rudolph R. Haering

When a photoconductor is illuminated at low temperatures, trapping states may be populated by electrons. If the light is then removed and an electric field is applied to the sample, these traps may be emptied by field ionization. For an electric field which increases linearly with time, the conductivity and the luminescent brightness display a sharp maximum at some field strength. It is shown that this maximum may be used to obtain the trap energy. The analysis of such field-ionization-induced maxima is very similar to the analysis of glow curves in thermoluminescence.


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