The dielectric constant of TCNQ single crystals as deduced by reflection electron energy loss spectroscopy

1993 ◽  
Vol 8 (10) ◽  
pp. 2627-2633 ◽  
Author(s):  
G. Mondio ◽  
F. Neri ◽  
G. Curró ◽  
S. Patané ◽  
G. Compagnini

The dielectric constant of tetracyanoquinodimethane (TCNQ) single crystals has been obtained by reflection electron energy loss spectroscopy (REELS) over the 0–60 eV energy range, using primary electron energies ranging from 0.5 to 1.5 keV at an incidence angle of about 40°. A self-consistent method is discussed concerning the evaluation of the surface and bulk contributions to the loss spectra. As a result, for the first time, the Im(−1/∊) function and the dielectric constant of TCNQ have been deduced in such a wide energy range. According to the results obtained by other authors, the low-energy loss spectral profile is characterized by two main structures ascribed to the π → π∗ dipole-allowed transitions located at about 3.5 and 6.5 eV while, at higher energy loss, the π + σ plasmon, centered at about 21.5 eV, dominates the spectrum. The differences among the spectra taken at different primary energies are interpreted as due only to surface effects, more evident in the low-energy-loss spectral region. The results are in good agreement with those obtained by recent transmission-mode (TEELS) experiments.

2013 ◽  
Vol 124 ◽  
pp. 130-138 ◽  
Author(s):  
Jeffery A. Aguiar ◽  
Bryan W. Reed ◽  
Quentin M. Ramasse ◽  
Rolf Erni ◽  
Nigel D. Browning

2007 ◽  
Vol 126 (2) ◽  
pp. 024303 ◽  
Author(s):  
M. Hoshino ◽  
K. Sunohara ◽  
C. Makochekanwa ◽  
L. Pichl ◽  
H. Cho ◽  
...  

1983 ◽  
Vol 78 (3) ◽  
pp. 1200-1212 ◽  
Author(s):  
M.‐J. Hubin‐Franskin ◽  
J. Delwiche ◽  
A. Poulin ◽  
B. Leclerc ◽  
P. Roy ◽  
...  

1998 ◽  
Vol 05 (01) ◽  
pp. 427-431 ◽  
Author(s):  
Susanne Siebentritt ◽  
Roland Pues ◽  
Karl-Heinz Rieder ◽  
Alexander M. Shikin

Using high resolution electron energy loss spectroscopy (HREELS) the surface phonon dispersion of graphite has been determined in the Γ K direction over the whole energy range and the whole Brillouin zone. By depositing lanthanum and annealing we prepared a GIC-like phase which grows on top of an intermediate carbide. The phonon dispersion of this phase shows the same modes as graphite, but the optical ones are softened and the acoustical ones are stiffened. This is described within a Born-von Karman model. The evolution of the phonon dispersion gives a first hint that the GIC-like phase may develop in two stages: first a monolayer graphite on top of the carbide and then the very thin GIC layer.


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