Hot-electron mean free path of ErAs thin films grown on GaAs determined by metal-base transistor ballistic electron emission spectroscopy

2006 ◽  
Vol 74 (20) ◽  
Author(s):  
K. J. Russell ◽  
V. Narayanamurti ◽  
Ian Appelbaum ◽  
M. P. Hanson ◽  
A. C. Gossard
Keyword(s):  
Thin Films ◽  
Free Path ◽  
Electron Emission ◽  
Emission Spectroscopy ◽  
Mean Free Path ◽  
Hot Electron ◽  
Metal Base ◽  
Ballistic Electron ◽  
Electron Mean Free Path

scholarly journals Study of the Electron Mean Free Path by Ballistic Electron Emission Microscopy

1996 ◽  
Vol 6 (5) ◽  
pp. 661-669 ◽  
Author(s):  
C. Girardin ◽  
R. Coratger ◽  
R. Pechou ◽  
F. Ajustron ◽  
J. Beauvillain
Keyword(s):  
Free Path ◽  
Electron Emission ◽  
Mean Free Path ◽  
Ballistic Electron Emission Microscopy ◽  
Ballistic Electron ◽  
Emission Microscopy ◽  
Electron Mean Free Path

Imaging of Metal/Semiconductor Interface by Ballistic-Electron-Emission Microscopy (Beem)

1992 ◽  
Vol 295 ◽  
Author(s):  
E. Y. Lee ◽  
B. R. Turnew ◽  
J. R. Jimenez ◽  
L. J. Schowalter
Keyword(s):  
Free Path ◽  
Spatial Resolution ◽  
Electron Emission ◽  
Path Length ◽  
Free Path Length ◽  
Mean Free Path ◽  
Ballistic Electron Emission Microscopy ◽  
Semiconductor Interface ◽  
Ballistic Electron ◽  
Emission Microscopy

AbstractStudies in ballistic-electron-emission spectroscopy (BEES) have enabled precise energy measurements of Schottky barrier heights with excellent spatial resolution and, more recently, it was shown that even scattering at the metal/semiconductor interface affects the BEES spectrum [1]. Monte Carlo simulations have been done to predict the spatial resolution of ballistic-electron-emission microscopy (BEEM) [2]. In this paper, we will discuss the experimental spatial resolution of BEEM, and we will also give some of our BEES results for Au/Si and for Au/PtSi/Si. Our experimental BEEM studies indicate that, for Au/Si, hot electron transport is diffusive rather than ballistic, because the inelastic mean free path length (∼100 nm) is much larger than the elastic mean free path length (∼10 nm). This is in agreement with existing theories and with the literature on the internal photoemission method of studying the transport. Even in this diffusive regime, the spatial resolution of BEEM is still expected to be very good, being on the order of 10 nm [2]. Our preliminary work on PtSi shows that it has an attenuation length of 4 nm, which differs significantly from that of Au.

Ballistic electron mean free path of titanylphthalocyanine films grown on GaAs

2008 ◽  
Vol 5 (1) ◽  
pp. 386-389
Author(s):  
S. Özcan ◽  
J. Smoliner ◽  
M. Andrews ◽  
G. Strasser ◽  
T. Dienel ◽  
...  
Keyword(s):  
Free Path ◽  
Mean Free Path ◽  
Ballistic Electron ◽  
Electron Mean Free Path
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