Valence and conduction band offsets at low-k a-SiOxCy:H/a-SiCxNy:H interfaces

2014 ◽  
Vol 116 (11) ◽  
pp. 113703 ◽  
Author(s):  
Sean W. King ◽  
Justin Brockman ◽  
Marc French ◽  
Milt Jaehnig ◽  
Markus Kuhn ◽  
...  
Keyword(s):  
2004 ◽  
Vol 241 (10) ◽  
pp. 2246-2252 ◽  
Author(s):  
S. Sayan ◽  
R. A. Bartynski ◽  
X. Zhao ◽  
E. P. Gusev ◽  
D. Vanderbilt ◽  
...  

2020 ◽  
Vol 529 ◽  
pp. 147119 ◽  
Author(s):  
Xiaobing Cao ◽  
Guoshuai Zhang ◽  
Yifan Cai ◽  
Long Jiang ◽  
Yan Chen ◽  
...  

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

1996 ◽  
Vol 39 (2) ◽  
pp. 79-81 ◽  
Author(s):  
A.Y. Polyakov ◽  
N.B. Smirnov ◽  
A.V. Govorkov ◽  
A.A. Chelniy ◽  
A.G. Milnes ◽  
...  
Keyword(s):  

1997 ◽  
Vol 482 ◽  
Author(s):  
J. A. Majewski ◽  
M. Städele

AbstractWe present a first-principles study of heteroepitaxial interfaces between GaN and both cubic as well as wurtzite AlN substrates oriented along main cubic or hexagonal directions and of stacking fault interfaces between cubic and wurtzite GaN. Our calculations show that all studied heterostructures are of type I. Valence band offsets for GaN/AlN are nearly independent of the substrate orientation and of the order of 0.8 eV. The valence and conduction band offsets for a stacking fault interface are predicted to be 40 meV and 175 meV, respectively.


2002 ◽  
Vol 737 ◽  
Author(s):  
V. Ligatchev ◽  
T.K.S. Wong Rusli ◽  
B. Liu ◽  
K. Ostrikov

ABSTRACTResults of experimental investigations on the relationship between nanoscale morphology of carbon doped hydrogenated silicon-oxide (SiOCH) low-k films and their electron spectrum of defect states are presented. The SiOCH films have been deposited using trimethylsilane (3MS) - oxygen mixture in a 13.56 MHz plasma enhanced chemical vapor deposition (PECVD) system at variable RF power densities (from 1.3 to 2.6 W/cm2) and gas pressures of 3, 4, and 5 Torr. The atomic structure of the SiOCH films is a mixture of amorphous-nanocrystalline SiO2-like and SiC-like phases. Results of the FTIR spectroscopy and atomic force microscopy suggest that the volume fraction of the SiC-like phase increases from ∼0.2 to 0.4 with RF power. The average size of the nanoscale surface morphology elements of the SiO2-like matrix can be controlled by the RF power density and source gas flow rates.Electron density of the defect states N(E) of the SiOCH films has been investigated with the DLTS technique in the energy range up to 0.6 eV from the bottom of the conduction band. Distinct N(E) peaks at 0.25 - 0.35 eV and 0.42 - 0.52 eV below the conduction band bottom have been observed. The first N(E) peak is identified as originated from E1-like centers in the SiC-like phase. The volume density of the defects can vary from 1011 - 1017 cm-3 depending on specific conditions of the PECVD process.


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