scholarly journals Determination of the impact of Bi content on the valence band energy of GaAsBi using x-ray photoelectron spectroscopy

AIP Advances ◽  
2017 ◽  
Vol 7 (7) ◽  
pp. 075016 ◽  
Author(s):  
K. Collar ◽  
J. Li ◽  
W. Jiao ◽  
Y. Guan ◽  
M. Losurdo ◽  
...  
1989 ◽  
Vol 53 (370) ◽  
pp. 153-164 ◽  
Author(s):  
David S. Urch

AbstractX-ray photoelectron spectroscopy can be used to measure the ionization energies of electrons in both valence band and core orbitals. As core vacancies are the initial states for X-ray emission, a knowledge of their energies for all atoms in a mineral enables all the X-ray spectra to be placed on a common energy scale. X-ray spectra are atom specific and are governed by the dipole selection rule. Thus the individual bonding roles of the different atoms are revealed by the fine structure of valence X-ray peaks (i.e. peaks which result from electron transitions between valence band orbitals and core vacancies). The juxtaposition of such spectra enables the composition of the molecular orbitals that make up the chemical bonds of a mineral to be determined.Examples of this approach to the direct determination of electronic structure are given for silica, forsterite, brucite, and pyrite. Multi-electron effects and developments involving anisotropic X-ray emission from single crystals are also discussed.


1975 ◽  
Vol 35 (26) ◽  
pp. 1803-1806 ◽  
Author(s):  
P. Mengel ◽  
P. M. Grant ◽  
W. E. Rudge ◽  
B. H. Schechtman ◽  
D. W. Rice

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

2008 ◽  
Vol 93 (20) ◽  
pp. 202101 ◽  
Author(s):  
Jianxiao Si ◽  
Shuqiang Jin ◽  
Hanjie Zhang ◽  
Ping Zhu ◽  
Dongjiang Qiu ◽  
...  

1995 ◽  
Vol 34 (Part 2, No. 6A) ◽  
pp. L653-L656 ◽  
Author(s):  
Josep L. Alay ◽  
Masatoshi Fukuda ◽  
ClaesH.Bjorkman ◽  
Kazuyuki Nakagawa ◽  
ShinYokoyama ◽  
...  

2007 ◽  
Vol 91 (16) ◽  
pp. 162104 ◽  
Author(s):  
Riqing Zhang ◽  
Panfeng Zhang ◽  
Tingting Kang ◽  
Haibo Fan ◽  
Xianglin Liu ◽  
...  

Nanomaterials ◽  
2021 ◽  
Vol 11 (8) ◽  
pp. 1969
Author(s):  
Riccardo Scarfiello ◽  
Elisabetta Mazzotta ◽  
Davide Altamura ◽  
Concetta Nobile ◽  
Rosanna Mastria ◽  
...  

The surface and structural characterization techniques of three atom-thick bi-dimensional 2D-WS2 colloidal nanocrystals cross the limit of bulk investigation, offering the possibility of simultaneous phase identification, structural-to-morphological evaluation, and surface chemical description. In the present study, we report a rational understanding based on X-ray photoelectron spectroscopy (XPS) and structural inspection of two kinds of dimensionally controllable 2D-WS2 colloidal nanoflakes (NFLs) generated with a surfactant assisted non-hydrolytic route. The qualitative and quantitative determination of 1T’ and 2H phases based on W 4f XPS signal components, together with the presence of two kinds of sulfur ions, S22− and S2−, based on S 2p signal and related to the formation of WS2 and WOxSy in a mixed oxygen-sulfur environment, are carefully reported and discussed for both nanocrystals breeds. The XPS results are used as an input for detailed X-ray Diffraction (XRD) analysis allowing for a clear discrimination of NFLs crystal habit, and an estimation of the exact number of atomic monolayers composing the 2D-WS2 nanocrystalline samples.


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.


Sign in / Sign up

Export Citation Format

Share Document