Tuning Fermi Level and Band Gap in Li 4 Ti 5 O 12 by Doping and Vacancy for Ultrafast Li + Insertion/Extraction

Author(s):  
Zhenya Wang ◽  
Hao Guo ◽  
De Ning ◽  
Xiaobai Ma ◽  
Lirong Zheng ◽  
...  
Keyword(s):  
2003 ◽  
Vol 763 ◽  
Author(s):  
U. Rau ◽  
M. Turcu

AbstractNumerical simulations are used to investigate the role of the Cu-poor surface defect layer on Cu(In, Ga)Se2 thin-films for the photovoltaic performance of ZnO/CdS/Cu(In, Ga)Se2 heterojunction solar cells. We model the surface layer either as a material which is n-type doped, or as a material which is type-inverted due to Fermi-level pinning by donor-like defects at the interface with CdS. We further assume a band gap widening of this layer with respect to the Cu(In, Ga)Se2 bulk. This feature turns out to represent the key quality of the Cu(In, Ga)Se2 surface as it prevents recombination at the absorber/CdS buffer interface. Whether the type inversion results from n-type doping or from Fermi-level pinning is only of minor importance as long as the surface layer does not imply a too large number of excess defects in its bulk or at its interface with the normal absorber. With increasing number of those defects an n-type layer proofs to be less sensitive to material deterioration when compared to the type-inversion by Fermi-level pinning. For wide gap chalcopyrite solar cells the internal valence band offset between the surface layer and the chalcopyrite appears equally vital for the device efficiency. However, the unfavorable band-offsets of the ZnO/CdS/Cu(In, Ga)Se2 heterojunction limit the device efficiency because of the deterioration of the fill factor.


2020 ◽  
Vol 22 (48) ◽  
pp. 27987-27998
Author(s):  
Mehmet Aras ◽  
Sümeyra Güler-Kılıç ◽  
Çetin Kılıç

The segregation tendency of an impurity in a semiconductor nanowire can be tuned by adjusting the Fermi level position.


2001 ◽  
Vol 15 (17n19) ◽  
pp. 696-699 ◽  
Author(s):  
G. Fonthal ◽  
M. de los Rios ◽  
J. Quintero ◽  
N. Piraquive ◽  
H. Ariza-Calderón

We analyzed the free to acceptor (e-A) photoluminescence transition on a GaAs:Ge sample using the hot carrier temperature and the Kane's DOS. This latter temperature was calculated by the spectra largest energy tail. While the lattice temperature was put in the e-A Eagles' shape equation, the fitting was poor but if the modified line was put into the equation, the fitting was better. So, the ionization impurity energy, the band gap, the Fermi level and the band tail can be measured with a better precision than the measurements traditionally made with this method, Additional information about phonons participant can be obtained. In conclusion, the hot carrier temperature and the density of states due to the impurity concentration should be used in the e-A transition photoluminescence analysis.


Author(s):  
M. Mirnezhad ◽  
R. Ansari ◽  
H. Rouhi ◽  
M. Faghihnasiri

The application of graphene as a nanosensor in measuring strain through its band structure around the Fermi level is investigated in this paper. The mechanical properties of graphene as well as its electronic structure are determined by using the density functional theory calculations within the framework of generalized gradient approximation. In the case of electronic properties, the simulations are applied for symmetrical and asymmetrical strain distributions in elastic range; also the tight-binding approach is implemented to verify the results. It is indicated that the energy band gap does not change with the symmetrical strain distribution but depend on the asymmetric strain distribution, increasing strain leads to band gap opening around the Fermi level.


ACS Nano ◽  
2017 ◽  
Vol 11 (11) ◽  
pp. 11661-11668 ◽  
Author(s):  
Néstor Merino-Díez ◽  
Aran Garcia-Lekue ◽  
Eduard Carbonell-Sanromà ◽  
Jingcheng Li ◽  
Martina Corso ◽  
...  

Author(s):  
L. S. Taura ◽  
Isah Abdulmalik ◽  
A. S. Gidado ◽  
Abdullahi Lawal

Stanene is a 2D hexagonal layer of tin with exceptional electronic and optical properties. However, the semiconductor applications of stanene are limited due to its zero band-gap. However, doping stanene could lead to a band gap opening, which could be a promising material for electronic and optical applications. In this work, optimized structure, electronic band structure, real and imaginary parts of the frequency-dependent dielectric function, electron loss function, and refractive index of stanene substitutionally doped with alkaline earth metal (beryllium) were analyzed using density functional theory (DFT) calculations as implemented in the quantum espresso and yambo suites. A pure stanene has a zero band gap energy, but with the inclusion of spin-orbit coupling in the electronic calculation of pure stanene, the band-gap is observed to open up by 0.1eV. Doping stanene with beryllium opens the band-gap and shifts the Dirac cone from the Fermi level, the band gap opens by 0.25eV, 0.55eV, and 0.8eV when the concentration of Beryllium is 12.5%, 25%, and 37.5% respectively. The Dirac cone vanished when the concentration of the dopant was increased to 50%.  The Fermi level is shifted towards the valence band edge indicating a p-type material. The material absorption shows that SnBe absorption ranges in the visible to the ultraviolet region, The refractive index in stanene doped beryllium (SnBe) was found to be higher than that of pristine stanene, the highest refractive index was 9.2 at SnBe25%. In a nutshell, the results indicate that stanene can be a good material for electronic and optical applications if doped with beryllium.


Author(s):  
М.С. Аксенов ◽  
Н.А. Валишева ◽  
А.П. Ковчавцев

It is shown that the fluorine-containing anodic layers on the n-In0.53Ga0.47As surface, in contrast to the anodic layers without fluorine, form a SiO2/InGaAs interface with an unpinned Fermi level, the state density on which decreases during annealing at a temperature of 300 °C to values (2-4) 1011 and (4-5) 1012 eV-1cm-2 near conduction band bottom and the band gap middle, respectively. An increase in the annealing temperature leads to a reverse increase in the state density (350 ºС) and pinning of the Fermi level (400 ºС).


2011 ◽  
Vol 98 (6) ◽  
pp. 062103 ◽  
Author(s):  
Ph. Ebert ◽  
S. Schaafhausen ◽  
A. Lenz ◽  
A. Sabitova ◽  
L. Ivanova ◽  
...  

2004 ◽  
Vol 92 (1) ◽  
Author(s):  
F. Baumberger ◽  
M. Hengsberger ◽  
M. Muntwiler ◽  
M. Shi ◽  
J. Krempasky ◽  
...  
Keyword(s):  
Band Gap ◽  

2005 ◽  
Vol 86 (19) ◽  
pp. 192111 ◽  
Author(s):  
J. D. Ye ◽  
S. L. Gu ◽  
S. M. Zhu ◽  
S. M. Liu ◽  
Y. D. Zheng ◽  
...  
Keyword(s):  
Band Gap ◽  

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