Valence band offsets in strained GaAs1−xPx/GaAs heterojunctions

1995 ◽  
Vol 24 (6) ◽  
pp. 713-717 ◽  
Author(s):  
Neal G. Anderson ◽  
Farid Agahi ◽  
Arvind Baliga ◽  
Kei May Lau
Keyword(s):  
2019 ◽  
Vol 14 (1) ◽  
Author(s):  
Ya-Wei Huan ◽  
Ke Xu ◽  
Wen-Jun Liu ◽  
Hao Zhang ◽  
Dmitriy Anatolyevich Golosov ◽  
...  

AbstractHybrid heterojunctions based on two-dimensional (2D) and conventional three-dimensional (3D) materials provide a promising way toward nanoelectronic devices with engineered features. In this work, we investigated the band alignment of a mixed-dimensional heterojunction composed of transferred MoS2 on β-Ga2O3($$ 2- $$2-01) with and without nitridation. The conduction and valence band offsets for unnitrided 2D-MoS2/3D-β-Ga2O3 heterojunction were determined to be respectively 0.43 ± 0.1 and 2.87 ± 0.1 eV. For the nitrided heterojunction, the conduction and valence band offsets were deduced to 0.68 ± 0.1 and 2.62 ± 0.1 eV, respectively. The modified band alignment could result from the dipole formed by charge transfer across the heterojunction interface. The effect of nitridation on the band alignments between group III oxides and transition metal dichalcogenides will supply feasible technical routes for designing their heterojunction-based electronic and optoelectronic devices.


1991 ◽  
Vol 240 ◽  
Author(s):  
Emil S. Koteies

ABSTRACTWe have developed a novel experimental technique for accurately determining band offsets in semiconductor quantum wells (QW). It is based on the fact that the ground state heavy- hole (HH) band energy is more sensitive to the depth of the valence band well than the light-hole (LH) band energy. Further, it is well known that as a function of the well width, Lz, the energy difference between the LH and HH excitons in a lattice matched, unstrained QW system experiences a maximum. Calculations show that the position, and more importantly, the magnitude of this maximum is a sensitive function of the valence band offset, Qy, which determines the depth of the valence band well. By fitting experimentally measured LH-HH splittings as a function of Lz, an accurate determination of band offsets can be derived. We further reduce the experimental uncertainty by plotting LH-HH as a function of HH energy (which is a function of Lz ) rather than Lz itself, since then all of the relevant parameters can be precisely determined from absorption spectroscopy alone. Using this technique, we have derived the conduction band offsets for several material systems and, where a consensus has developed, have obtained values in good agreement with other determinations.


2018 ◽  
Vol 8 (7) ◽  
pp. Q3001-Q3006 ◽  
Author(s):  
Chaker Fares ◽  
F. Ren ◽  
David C. Hays ◽  
B. P. Gila ◽  
S. J. Pearton

2013 ◽  
Vol 114 (4) ◽  
pp. 043718 ◽  
Author(s):  
Yoyo Hinuma ◽  
Fumiyasu Oba ◽  
Yoshitaro Nose ◽  
Isao Tanaka

2000 ◽  
Vol 77 (9) ◽  
pp. 723-729
Author(s):  
A Ennaoui

The highest efficiency for Cu(Ga,In)Se2 (CIGS) thin-film-based solar cells has been achieved with CdS buffer layers prepared by a solution growth method known as the chemical bath deposition (CBD). With the aim of developing Cd-free chalcopyrite-based thin-film solar cells, we describe the basic concepts involved in the CBD technique. The recipes developed in our laboratory for the heterogeneous deposition of good-quality thin films of ZnO, ZnSe, and MnS are presented. In view of device optimization, the initial formation of chemical-bath-deposited ZnSe thin films on Cu(Ga,In)(S,Se)2 (CIGSS) and the subsequent development of the ZnSe/CIGSS heterojunctions were investigated by X-ray photoelectron spectroscopy (XPS). The good surface coverage was controlled by measuring changes in the valence-band electronic structure as well as changes in the In4d, Zn3d core lines. From these measurements, the growth rate was found to be around 3.6 nm/min. The valence band and the conduction band-offsets ΔEV and ΔEC between the layers were determined to be 0.60 and 1.27 eV, respectively for the CIGSS/ZnSe interface. The energy-band diagram is discussed in connection with the band-offsets detemined from XPS data. A ZnSe thickness below 10 nm has been found to be optimum for achieving a homogeneous and compact buffer layer on CIGSS with a total area efficiency of 13.7%.PACS No.: 42.70


1993 ◽  
Vol 326 ◽  
Author(s):  
K. Schmalz ◽  
H. RüCker ◽  
I. N. Yassievich ◽  
H. G. Grimmeiss ◽  
W. Mehr ◽  
...  

1996 ◽  
Vol 69 (18) ◽  
pp. 2719-2721 ◽  
Author(s):  
Su‐Huai Wei ◽  
Alex Zunger
Keyword(s):  

2010 ◽  
Vol 207 (6) ◽  
pp. 1335-1337 ◽  
Author(s):  
Anja Eisenhardt ◽  
Andreas Knübel ◽  
Ralf Schmidt ◽  
Marcel Himmerlich ◽  
Joachim Wagner ◽  
...  

1996 ◽  
Vol 80 (5) ◽  
pp. 2918-2921 ◽  
Author(s):  
San‐huang Ke ◽  
Kai‐ming Zhang ◽  
Xi‐de Xie
Keyword(s):  
Band Gap ◽  

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