Characteristics of Field Emission at Very High Current Densities

Nature ◽  
1950 ◽  
Vol 165 (4193) ◽  
pp. 403-404 ◽  
Author(s):  
A. M. AZZAM ◽  
J. O'M. BOCKRIS

1965 ◽  
Vol 3 (8) ◽  
pp. lxx-lxxi
Author(s):  
A.I. Imenkov ◽  
M.M. Koslov ◽  
D.N. Nasledov ◽  
B.V. Tsarenkov

2002 ◽  
Vol 12 (9) ◽  
pp. 127-128
Author(s):  
A. A. Sinchenko ◽  
S. G. Zybtsev ◽  
I. G. Gorlova ◽  
Yu. I. Latyshev ◽  
V. Ya. Pokrovskii ◽  
...  

We report transport measurements under very high current densities j, up to 108 A/cm2, of quasi-one-dimensional charge-density wave (CDW) conductors NbSe3 and TaS3. Above $j_0-10^1$ A/cm2 the point contacts NbSe3-NbSe3 show a sharp singularity, and the TaS3 nanosamples show metallic temperature dependence (positive dR/dn. We interpret both results as an evidence for the suppression of the Peierls gap 2A and development of the metallic state above j0. Possible scenarios of the Peierls state destruction are discussed.


2007 ◽  
Vol 22 (22) ◽  
pp. 3784-3793 ◽  
Author(s):  
C. H. BOULWARE ◽  
J. D. JARVIS ◽  
H. L. ANDREWS ◽  
C. A. BRAU

At the tips of sharp needles, the surface electric field is enhanced by many orders of magnitude. This intensifies thermionic emission and photoemission of electrons through the Schottky effect, and reduces the effect of space charge. The increased current density improves the brightness of electron sources by orders of magnitude. In addition, at very high fields (>109 V/m ), field emission and photo-field emission produce very high current density. Arrays of needles can be used to achieve high total current.


Sign in / Sign up

Export Citation Format

Share Document