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Pressure dependence of the band gap energy for dilute nitride and antimony GaNxSbyAs1−x−y

Zhao Chuan-Zhen, Ren He-Yu, Sun Xiao-Dong, Wang Sha-Sha, Lu Ke-Qing

Materials Science Poland

2020

Vol. 38, No. 2

248--252

Dilute nitride and antimony GaNAsSb alloy can be considered as an alloy formed by adding N and Sb atoms into the host material GaAs. Under this condition, its band gap energy depending on pressure can be divided into two regions. In the low pressure range, the band gap energy is due to two factors. One is the coupling interaction between the N level and the Γ conduction band minimum (CBM) of GaAs. The other one is the coupling interaction between the Sb level and the Γ valence band maximum (VBM) of GaAs. In the high pressure range, the band gap energy depends also on two factors. One is the coupling interaction between the N level and the X CBM of GaAs. The other one is the coupling interaction between the Sb level and the Γ VBM of GaAs. In addition, it has been found that the energy difference between the Γ CBM and the X CBM in GaNAsSb is larger than that in GaAs. It is due to two factors. One is the coupling interaction between the N level and the Γ CBM of GaAs. The other is the coupling interaction between the N level and the X CBM of GaAs.

Pressure dependence of the band gap energy for the dilute nitride GaNxAs1−x

Zhao C.-Z., Wei T., Sun X.-D., Wang S.-S., Lu K.-Q.

Materials Science Poland

2016

Vol. 34, No. 4

881--885

A model is developed to describe the pressure dependence of the band gap energy for the dilute nitride GaNxAs1-x. It is found that the sublinear pressure dependence of E- is due to the coupling interaction between E+ and E-. We have also found that GaNxAs1-xneeds much larger pressure than GaAs to realize the transition from direct to indirect band gap. It is due to two factors. One is the coupling interaction between the E+ and E-. The other is that the energy difference between the X conduction band minimum (CBM) and the G CBM in GaNxAs1-x is larger than that in GaAs. In addition, we explain the phenomenon that the energy difference between the X CBM and the G CBM in GaNxAs1-xis larger than that in GaAs. It is due to the impurity-host interaction.

Oscillator strength of optical transitions in InGaAsN/GaAsN/GaAs quantum wells

Mika A, Sek G, Ryczko K, Kozub M, Musial A, Marynski A, Misiewicz J, Langer F, Höfling S, Appel T, Kamp M, Forchel A

Optica Applicata

2013

Vol. 43, nr 1

53--60

Experimental and theoretical considerations and results on the effect of nitrogen incorporation on the oscillator strength of optical transitions in InGaNAs/GaAs quantum wells (QWs) are presented. Therefore, a set of dilute nitride quantum well structures was grown by molecular beam epitaxy. Optical investigation via spectroscopic methods have been performed at various temperatures for both the as-grown samples, and after rapid thermal annealing. The fundamental transition energy and its oscillator strength vs. the QW composition have been systematically investigated. Additionally, the effect of the bandgap discontinuities on the transitions intensity has also been considered. The experimental data have been confronted with the band structure calculations within the effective mass approximation employing a two level repulsion model for the nitrogen-containing structures. The obtained results are crucial for possible future applications employing the quantum well in cavity structures and bringing the practical exploitation of quantum electrodynamics phenomena to the telecommunication spectral range.