Implantation and Detection of Low Energy Argon Ions in Silicon Single Crystals

1968 ◽  
Vol 115 (9) ◽  
pp. 974 ◽  
Author(s):  
James Comas ◽  
Carmine A. Carosella
RSC Advances ◽  
2021 ◽  
Vol 11 (22) ◽  
pp. 13183-13192
Author(s):  
Jacqueline M. Cole ◽  
David J. Gosztola ◽  
Sven O. Sylvester

Single crystals that behave as optical switches are desirable for a wide range of applications, from optical sensors to read–write memory media.


2017 ◽  
Vol 496 ◽  
pp. 18-23 ◽  
Author(s):  
E. Marenkov ◽  
K. Nordlund ◽  
I. Sorokin ◽  
A. Eksaeva ◽  
K. Gutorov ◽  
...  
Keyword(s):  

2000 ◽  
Author(s):  
De-Quan Yang ◽  
Yuqing Xiong ◽  
Weigang Lu ◽  
Yun Guo ◽  
Dao-an Da
Keyword(s):  

2020 ◽  
Vol 124 (45) ◽  
pp. 24795-24808
Author(s):  
Elif Bilgilisoy ◽  
Rachel M. Thorman ◽  
Jo-Chi Yu ◽  
Timothy B. Dunn ◽  
Hubertus Marbach ◽  
...  

2019 ◽  
Vol 12 (5) ◽  
pp. 051009 ◽  
Author(s):  
Soichiro Yamanaka ◽  
Ko Tonami ◽  
Masaki Iwashita ◽  
Koki Yoshida ◽  
Riku Takeuchi ◽  
...  

2011 ◽  
Vol 131 (10) ◽  
pp. 2093-2099 ◽  
Author(s):  
A. Choubey ◽  
S.K. Sharma ◽  
S.P. Lochab ◽  
D. Kanjilal
Keyword(s):  

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.


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