scholarly journals Engineering Valence Band Dispersion for High Mobility p-Type Semiconductors

2016 ◽  
Vol 29 (6) ◽  
pp. 2402-2413 ◽  
Author(s):  
Benjamin A. D. Williamson ◽  
John Buckeridge ◽  
Jennilee Brown ◽  
Simon Ansbro ◽  
Robert G. Palgrave ◽  
...  
2009 ◽  
Vol 79-82 ◽  
pp. 1253-1256 ◽  
Author(s):  
Li Guan ◽  
Qiang Li ◽  
Xu Li ◽  
Jian Xin Guo ◽  
Bo Geng ◽  
...  

In the present paper, the lattice structure, band structure and density of state of pure and P-doped ZnO are calculated by first-principle method based on density functional theory. By analyzing the Mulliken charge overlap population and bond length, it is found that the bond of P-Zn is longer and stronger than O-Zn bond for PO-ZnO. But for PZn-ZnO, the O-P bond becomes shorter and more powerful than O-Zn bond. Also, weak O-O bonds are formed in this case. Our results show that the final total energy of PO-ZnO is lower than PZn-ZnO. The lattice structure of PO-ZnO is more stability than PZn-ZnO. For PO-ZnO, The Fermi level moves into the valence band, which expresses that the holes appear on the top of valence band and thus the PO-ZnO exhibits p-type conductivity. For PZn-ZnO, the Fermi level moves up to the conductor band and the total density of states shifts to the lower energy region, thus PZn-ZnO shows the n-type conductivity.


2021 ◽  
Vol 90 (12) ◽  
Author(s):  
Fumihiko Matsui ◽  
Seiji Makita ◽  
Hiroyuki Matsuda ◽  
Eiken Nakamura ◽  
Yasuaki Okano ◽  
...  

Author(s):  
Tien Dat Ngo ◽  
Min Sup Choi ◽  
Myeongjin Lee ◽  
Fida Ali ◽  
Won Jong Yoo

A technique to form the edge contact in two-dimensional (2D) based field-effect transistors (FETs) has been intensively studied for the purpose of achieving high mobility and also recently overcoming the...


2017 ◽  
Vol 4 (9) ◽  
pp. 1458-1464 ◽  
Author(s):  
M.-Y. Lee ◽  
D. I. Bilc ◽  
E. Symeou ◽  
Y.-C. Lin ◽  
I.-C. Liang ◽  
...  

A new p-type semiconductor Ba3Ag3InTe6 with transport properties dominated by the layer [Ag3Te4]5− distributed in the valence band.


1982 ◽  
Vol 25 (4) ◽  
pp. 351-354
Author(s):  
V. V. Konev ◽  
V. A. Chaldyshev

2001 ◽  
Vol 64 (8) ◽  
Author(s):  
P. A. Shields ◽  
R. J. Nicholas ◽  
F. M. Peeters ◽  
B. Beaumont ◽  
P. Gibart

Author(s):  
Ming-Wei Chen ◽  
HoKwon Kim ◽  
Dmitry Ovchinnikov ◽  
Agnieszka Kuc ◽  
Thomas Heine ◽  
...  

2012 ◽  
Vol 717-720 ◽  
pp. 1195-1198
Author(s):  
Geunsik Lim ◽  
Tariq Manzur ◽  
Aravinda Kar

An uncooled SiC-based electro-optic device is developed for gas sensing applications. P-type dopants Ga, Sc, P and Al are incorporated into an n-type crystalline 6H-SiC substrate by a laser doping technique for sensing CO2, CO, NO2 and NO gases, respectively. Each dopant creates an acceptor energy level within the bandgap of the substrate so that the energy gap between this acceptor level and the valence band matches the quantum of energy emitted by the gas of interest. The photons of the gas excite electrons from the valence band to the acceptor level, which alters the electron density in these two states. Consequently, the refractive index of the substrate changes, which, in turn, modifies the reflectivity of the substrate. This change in reflectivity represents the optical signal of the sensor, which is probed remotely with a laser such as a helium-neon laser. Although the midwave infrared (3-5 mm) band is studied in this paper, the approach is applicable to other spectral bands.


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