Admittance spectroscopy measurements of band offsets in Si/Si1−xGex/Si heterostructures

1992 ◽  
Vol 60 (2) ◽  
pp. 195-197 ◽  
Author(s):  
K. Nauka ◽  
T. I. Kamins ◽  
J. E. Turner ◽  
C. A. King ◽  
J. L. Hoyt ◽  
...  
1987 ◽  
Vol 50 (12) ◽  
pp. 736-738 ◽  
Author(s):  
D. V. Lang ◽  
M. B. Panish ◽  
F. Capasso ◽  
J. Allam ◽  
R. A. Hamm ◽  
...  

1999 ◽  
Vol 85 (2) ◽  
pp. 985-993 ◽  
Author(s):  
D. V. Singh ◽  
K. Rim ◽  
T. O. Mitchell ◽  
J. L. Hoyt ◽  
J. F. Gibbons

1989 ◽  
Vol 54 (8) ◽  
pp. 739-741 ◽  
Author(s):  
R. E. Cavicchi ◽  
D. V. Lang ◽  
D. Gershoni ◽  
A. M. Sergent ◽  
J. M. Vandenberg ◽  
...  

1997 ◽  
Vol 70 (25) ◽  
pp. 3413-3415 ◽  
Author(s):  
B. L. Stein ◽  
E. T. Yu ◽  
E. T. Croke ◽  
A. T. Hunter ◽  
T. Laursen ◽  
...  

1986 ◽  
Vol 60 (12) ◽  
pp. 4191-4196 ◽  
Author(s):  
K. Kobayashi ◽  
M. Takata ◽  
Y. Fujimura ◽  
S. Okamoto

2000 ◽  
Vol 87 (4) ◽  
pp. 1947-1950 ◽  
Author(s):  
Feng Lin ◽  
Da-wei Gong ◽  
Chi Sheng ◽  
Fang Lu ◽  
Xun Wang

Nanomaterials ◽  
2021 ◽  
Vol 11 (6) ◽  
pp. 1581
Author(s):  
José C. Conesa

Two DFT-based methods using hybrid functionals and plane-averaged profiles of the Hartree potential (individual slabs versus vacuum and alternating slabs of both materials), which are frequently used to predict or estimate the offset between bands at interfaces between two semiconductors, are analyzed in the present work. These methods are compared using several very different semiconductor pairs, and the conclusions about the advantages of each method are discussed. Overall, the alternating slabs method is recommended in those cases where epitaxial mismatch does not represent a significant problem.


Optik ◽  
2021 ◽  
Vol 231 ◽  
pp. 166506
Author(s):  
Najla M. Khusayfan ◽  
A.F. Qasrawi ◽  
Seham R. Alharbi ◽  
Hazem K. Khanfar ◽  
T.S. Kayed

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