Double-Band Anticrossing in GaAsSbN Induced by Nitrogen and Antimony Incorporation
Photoreflectance spectroscopy is utilized to study the effect of dilute nitrogen and antimony on the electronic band structure of as-grown GaAs 1-x-y Sb x N y alloys, which are potential materials for 1 eV solar cells and long-wavelength optoelectronic devices. The band gap, spin--orbit splitting, a...
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Published in | Applied physics express Vol. 6; no. 12; pp. 121202 - 121202-4 |
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Main Authors | , , , , |
Format | Journal Article |
Language | English |
Published |
The Japan Society of Applied Physics
01.12.2013
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Online Access | Get full text |
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Summary: | Photoreflectance spectroscopy is utilized to study the effect of dilute nitrogen and antimony on the electronic band structure of as-grown GaAs 1-x-y Sb x N y alloys, which are potential materials for 1 eV solar cells and long-wavelength optoelectronic devices. The band gap, spin--orbit splitting, and valence-band maximum to the N-induced upward conduction-band transition, for the first time, are obtained and analyzed using the double-band anticrossing model. The $E_{\text{N}}$ level with respect to the GaAs valence-band maximum and the interaction potential are determined as 1.540 and 2.839 eV, respectively. The results are helpful information for intermediate-band solar cell application. |
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Bibliography: | (a) PR spectra of the GaAs 1-x-y Sb x N y alloys at 298 K pumped with a He--Ne laser operating at 633 nm. The numbers show the index of the $n$th extreme of FKOs. The lowest spectrum is enlarged three times. (b) Schematic diagram showing the relative positions of the energy levels at $\Gamma$ point of GaAsSbN explained using the DBAC model. (c) Plot of FKO extreme, $E'_{n}$ vs $F_{n}$ for the GaAsSbN alloys. The intercepts indicate the band gaps of the alloys. The inset shows the high-resolution X-ray rocking curve of the GaAs 0.932 Sb 0.051 N 0.017 /GaAs heterostructure, whose lattice mismatch of $-9.2\times 10^{-4}$ is larger than those of the other two samples. PR spectra of the GaAs 1-x-y Sb x N y alloys at 298 K pumped with a He--Cd laser operating at 325 nm. The spectra with energy below 1.25 eV are detected using an InGaAs photodiode and that above 1.25 eV are detected using a Si photodiode. The red lines represent theoretical fits using Eq. ( ). The band gap ($E_{0}$), the Sb-affected spin--orbit band to the conduction band minimum ($E_{0}+\Delta_{0}$), and the valence band maximum to the N-induced upward conduction band ($E_{+}$) are observed. Transition energies versus N and Sb composition. The solid symbols depict the transition energies of GaAs 1-x-y Sb x N y alloys obtained from PR spectra. The open symbols represent the calculated transition energies of GaAs 1-x Sb x alloys using the VCA and VBAC model. The colored symbols are projections of the transition energies on the energy--N Composition plane. Projections of the transition energies (symbols) as illustrated in Fig. . The solid lines are the least-squares fits to the CBAC model based on the energy levels of GaAs 1-x Sb x alloys considering the VCA and VBAC model. The dotted lines are produced using the obtained CBAC parameters, i.e., $E_{\text{N}}$ and $C_{\text{N}}$. |
ISSN: | 1882-0778 1882-0786 |
DOI: | 10.7567/APEX.6.121202 |