Title :
Material Gain in Ga0.66In0.34NyAs1–y, GaNyAs0.69–ySb0.31, and GaNyP0.46Sb0.54–y Quantum Wells Grown on GaAs Substrates: Comparative The
Author :
Gladysiewicz, M. ; Kudrawiec, R. ; Wartak, Marek S.
Author_Institution :
Inst. of Phys., Wroclaw Univ. of Technol., Wrocław, Poland
Abstract :
Electronic band structure and material gain are calculated using the 8-band kp Hamiltonian for three quantum well (QW) systems grown on GaAs substrates: 1) Ga0.66In0.34NyAs1-y/GaAs; 2) GaNyAs0.69-ySb0.31/GaAs; and 3) GaNyP0.46Sb0.54-y/GaAs QWs with various nitrogen concentrations. Bandgap and electron effective mass for Ga0.66In0.34NyAs1-y, GaNyAs0.69-ySb0.31, and GaNyP0.46 Sb0.54-y alloys are determined within band anticrossing model using the proper alloying approximations. The intensity and spectral position of gain peak are directly compared for QWs with 2% of nitrogen and 2% compressive strain in the QW layer. The largest shift of gain peak has been observed for GaN0.02P0.46Sb0.52/GaAs QW. In this case, the gain peak (transverse electric (TE) mode) is located at 1.77 μm that is longer by 390 nm than the gain peak (TE mode) for Ga0.66In0.34N0.02As0.98/GaAs QW. In addition, for GaN0.02As0.67Sb0.31/GaAs QW the largest shift of gain peak (TE mode) is observed for Ga0.66In0.34N0.02As0.98/GaAs QW (1.67 versus 1.38~μm. The intensities of TE modes of material gain are comparable for all three systems. The above indicates that GaNyAs0.69-ySb0.31/GaAs and GaNyP0.46Sb0.54-y/GaAs QW systems are promising candidates for GaAs-based lasers dedicated for emission in very long-wavelength telecommunication windows. The required nitrogen concentration for achieving gain peak position (TE mode) at 1.3 and 1.55~μm are 0.5% and 1.5% N for GaNyAs0.69-ySb0.31/GaAs QWs, respectively, while for GaN- sub>yP0.46Sb0.54-y/GaAs QWs are 0.3% and 1.2% N. Those values are significantly less than in Ga0.66In0.34NyAs1-y/GaAs QWs. Considering a possible blue shift of QW emission upon annealing (i.e., the post grown procedure, which is usually used for improving optical quality of these QWs) the required nitrogen concentration can be larger by ~0.5% N than the one calculated for as-grown QWs.
Keywords :
III-V semiconductors; band structure; effective mass; energy gap; gallium arsenide; gallium compounds; indium compounds; nitrogen compounds; optical materials; phosphorus compounds; quantum well lasers; semiconductor growth; semiconductor quantum wells; spectral line shift; 8-band kp Hamiltonian; Ga0.66In0.34NyAs1-y-GaAs; GaAs; GaAs-based lasers; GaNyAs0.69-ySb0.31-GaAs; GaNyP0.46Sb0.54-y-GaAs; QW emission; annealing; band anticrossing model; bandgap; blue shift; compressive strain; electron effective mass; electronic band structure; material gain; nitrogen concentration; optical quality; quantum wells; transverse electric mode; very long-wavelength telecommunication windows; Effective mass; Gallium arsenide; Manganese; Nitrogen; Photonic band gap; Dilute nitrides; band structures; material gain;
Journal_Title :
Quantum Electronics, IEEE Journal of
DOI :
10.1109/JQE.2014.2363763