DEFECT PHYSICS AND INTRINSIC p-TYPE CONDUCTIVITY IN TOPOLOGICAL INSULATOR AuTlS2

2014 ◽  
Vol 28 (02) ◽  
pp. 1450008 ◽  
Author(s):  
JIAN-MIN ZHANG ◽  
WANGXIANG FENG ◽  
PEI YANG ◽  
LIJIE SHI ◽  
YING ZHANG

Using first-principles calculations, we systematically investigate the defect physics in topological insulator AuTlS 2. An optimal growth condition is explicitly proposed to guide for the experimental synthesis. The stabilities of various native point defects under different growth conditions and different carrier environments are studied in detail. We show that the p-type conductivity is strongly preferred in AuTlS 2, and the band gap can be engineered by the control of intrinsic defects. Our results demonstrate that AuTlS 2 is an ideal p-type topological insulator which can be easily integrated with traditional semiconductor.

2014 ◽  
Vol 16 (40) ◽  
pp. 22299-22308 ◽  
Author(s):  
J. Bekaert ◽  
R. Saniz ◽  
B. Partoens ◽  
D. Lamoen

Starting from first-principles calculations, many experimental observations such as photoluminescence spectra, charge carrier densities and freeze-out can be explained.


Author(s):  
Bo Kong ◽  
Tixian Zeng ◽  
Wentao Wang

Abstract: In this work, the n-type and p-type conductivity mechanisms of bulk BiOCl are systematically investigated using first-principles calculations. Under the O-rich growth conditions, BiOCl presents the intrinsic p-type conductivity,...


2020 ◽  
Vol 22 (3) ◽  
pp. 1784-1784
Author(s):  
Weiwei Wang ◽  
Yang Zhong ◽  
Dahuai Zheng ◽  
Hongde Liu ◽  
Yongfa Kong ◽  
...  

Correction for ‘p-Type conductivity mechanism and defect structure of nitrogen-doped LiNbO3 from first-principles calculations’ by Weiwei Wang et al., Phys. Chem. Chem. Phys., 2020, 22, 20–27.


2020 ◽  
Vol 22 (1) ◽  
pp. 20-27 ◽  
Author(s):  
Weiwei Wang ◽  
Yang Zhong ◽  
Dahuai Zheng ◽  
Hongde Liu ◽  
Yongfa Kong ◽  
...  

The charge-state transition level and geometry structure of non-metallic N-doped LiNbO3 are calculated by DFT, which reveal the p-type conductivity mechanism of LiNbO3:N.


2015 ◽  
Vol 17 (26) ◽  
pp. 16705-16708 ◽  
Author(s):  
Wenzhe Niu ◽  
Hongbin Xu ◽  
Yanmin Guo ◽  
Yaguang Li ◽  
Zhizhen Ye ◽  
...  

The S dopants in S–N co-doped ZnO contribute to easier doping and p-type conductivity, as concluded by experiment and calculations.


2015 ◽  
Vol 17 (7) ◽  
pp. 5485-5489 ◽  
Author(s):  
M. N. Amini ◽  
R. Saniz ◽  
D. Lamoen ◽  
B. Partoens

With the help of first-principles calculations, we investigate the VZn–NO–H acceptor complex in ZnO. We find that H plays an important role, because it lowers the formation energy of the complex with respect to VZn–NO, a complex known to exhibit p-type behavior. However, this additional H atom also occupies the hole level of VZn–NO making the VZn–NO–H complex a deep acceptor.


2013 ◽  
Vol 96 (10) ◽  
pp. 3304-3311 ◽  
Author(s):  
Bin Liu ◽  
Jiemin Wang ◽  
Fangzhi Li ◽  
Luchao Sun ◽  
Jingyang Wang ◽  
...  

2010 ◽  
Vol 88 (12) ◽  
pp. 927-932 ◽  
Author(s):  
Dan Huang ◽  
Yuanming Pan

Intrinsic defects, including vacancies at the Cu and Al sites (VCu and VAl), substitutional Cu at the Al site (CuAl), and interstitial O (Oi), have been proposed to be responsible for the p-type conductivity in CuAlO2. We have investigated the formation energies of these and other intrinsic defects in CuAlO2 using GGA+U calculations. Our results support previous studies that the potential alignment and image charge correction are required in the calculation of defect formation energies by using the supercell approach. In CuAlO2, these p-type defects (VCu, VAl, CuAl, and Oi) invariably have lower formation energies than their n-type counterparts. Particularly, VCu and CuAl have the lowest formation energies among intrinsic defects, and therefore are most likely responsible for the p-type conductivity. However, the transition levels of the VCu and CuAl defects are deep, which are responsible for the poor p-type conductivity in CuAlO2.


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