First-principles calculations of band-edge electronic states of silicon quantum wires

1994 ◽  
Vol 50 (19) ◽  
pp. 14223-14227 ◽  
Author(s):  
R. J. Needs ◽  
S. Bhattacharjee ◽  
K. J. Nash ◽  
A. Qteish ◽  
A. J. Read ◽  
...  
1993 ◽  
Vol 70 (13) ◽  
pp. 2050-2050 ◽  
Author(s):  
A. J. Read ◽  
R. J. Needs ◽  
K. J. Nash ◽  
L. T. Canham ◽  
P. D. J. Calcott ◽  
...  

1992 ◽  
Vol 69 (8) ◽  
pp. 1232-1235 ◽  
Author(s):  
A. J. Read ◽  
R. J. Needs ◽  
K. J. Nash ◽  
L. T. Canham ◽  
P. D. J. Calcott ◽  
...  

MRS Bulletin ◽  
2001 ◽  
Vol 26 (12) ◽  
pp. 998-1004 ◽  
Author(s):  
Victor I. Klimov ◽  
Moungi G. Bawendi

Semiconductor materials are widely used in both optically and electrically pumped lasers. The use of semiconductor quantum wells (QWs) as optical-gain media has resulted in important advances in laser technology. QWs have a two-dimensional, step-like density of electronic states that is nonzero at the band edge, enabling a higher concentration of carriers to contribute to the band-edge emission and leading to a reduced lasing threshold, improved temperature stability, and a narrower emission line. A further enhancement in the density of the band-edge states and an associated reduction in the lasing threshold are in principle possible using quantum wires and quantum dots (QDs), in which the confinement is in two and three dimensions, respectively. In very small dots, the spacing of the electronic states is much greater than the available thermal energy (strong confinement), inhibiting thermal depopulation of the lowest electronic states. This effect should result in a lasing threshold that is temperatureinsensitive at an excitation level of only 1 electron-hole (e-h) pair per dot on average. Additionally, QDs in the strongconfinement regime have an emission wavelength that is a pronounced function of size, adding the advantage of continuous spectral tunability over a wide energy range simply by changing the size of the dots.


2009 ◽  
Vol 20 (9) ◽  
pp. 095201 ◽  
Author(s):  
Y Min ◽  
K L Yao ◽  
Z L Liu ◽  
G Y Gao ◽  
H G Cheng ◽  
...  

2022 ◽  
Vol 12 (1) ◽  
Author(s):  
Masayuki Morimoto ◽  
Shoya Kawano ◽  
Shotaro Miyamoto ◽  
Koji Miyazaki ◽  
Shuzi Hayase ◽  
...  

AbstractTo develop high-performance thermoelectric devices that can be created using printing technology, the interface of a composite material composed of MASnI3 and Bi2Te3, which individually show excellent thermoelectric performance, was studied based on first-principles calculations. The structural stability, electronic state, and interfacial thermal conductance of the interface between Bi2Te3 and MASnI3 were evaluated. Among the interface structure models, we found stable interface structures and revealed their specific electronic states. Around the Fermi energy, the interface structures with TeII and Bi terminations exhibited interface levels attributed to the overlapping electron densities for Bi2Te3 and MASnI3 at the interface. Calculation of the interfacial thermal conductance using the diffuse mismatch model suggested that construction of the interface between Bi2Te3 and MASnI3 could reduce the thermal conductivity. The obtained value was similar to the experimental value for the inorganic/organic interface.


2005 ◽  
Vol 483-485 ◽  
pp. 573-576 ◽  
Author(s):  
Toshiharu Ohnuma ◽  
Hidekazu Tsuchida ◽  
Tamotsu Jikimoto ◽  
Atsumi Miyashita ◽  
Masahito Yoshikawa

First-principles calculations for the abrupt SiO2/4H-SiC interfaces accounting for Si-Si bonding and Nitrogen atom termination have been performed. Interface states due to Si-Si bonds appear at the valence band edge. Interface states at the midgap vanish when N atom terminates the Si dangling bond, but the interface states arising from the Si-N bonds appear at the valence band edge at the same time.


2004 ◽  
Vol 45 (7) ◽  
pp. 1987-1990 ◽  
Author(s):  
Tomoyuki Yamamoto ◽  
Fumie Yamashita ◽  
Isao Tanaka ◽  
Eiichiro Matsubara ◽  
Atsushi Muramatsu

2017 ◽  
Vol 31 (18) ◽  
pp. 1750199 ◽  
Author(s):  
F. J. Si ◽  
W. Hu ◽  
F. L. Tang ◽  
Y. W. Cheng ◽  
H. T. Xue

The lattice structure, interface binding energy, density of states, charge density difference and Bader charges of Au (100)/CH3NH3PbI3 (MAPbI3) (100) interface were studied with the first-principles calculations. The lattice mismatch of the Au (100)/MAPbI3 (100) interface is 3.48%. The interface binding energy is −0.124 J/m2. There is a small amount of electronic states nearby the interface through analyzing the density of states of the interface. In addition, the atom orbital has hybridizations nearby the interface. Through analyzing charge density difference and Bader charges, it is found that there is obvious charge transfer at the interface.


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