Abstract:Articles you may be interested inThe optical gain and radiative current density of GaInNAs/GaAs/AlGaAs separate confinement heterostructure quantum well lasers
“…11 Recently, much effort has been focused on exploring the GaInAsN/GaAs QW where adding small amounts of nitrogen(N) leads to favorable changes in band alignment and pushes the emission wavelength towards 1310 nm. [12][13][14] An impact of N incorporation is the deterioration of the optical properties as defect induced nonradiative recombination (NRR) increases with increasing N concentration, 15 although recent work has shown that the addition of minimal amount of N ( 0:5%) together with a post-growth annealing treatment (680 C, 10 min) in GaInAsN QW hinder from formation of N-N pairs and clusters and thus do not lead to reduction in the intrinsic gain of the active region. 16 While the NRR could be advantageous for fast saturable aborbers (SAs) and electroabsorption modulators (EAMs) as an additional carrier recombination process, 17,18 it is largely detrimental for the gain properties, with lasing threshold densities remaining relatively high.…”
The electro-optic properties of strained GaInAsSb/GaAs quantum wells (QWs) are investigated. A single QW p-i-n sample was grown by molecular beam epitaxy with antimony (Sb) pre-deposition technique. We numerically predict and experimentally verify a strong quantum confined Stark shift of 40 nm. We also predict a fast absorption recovery times crucial of high-speed optoelectronic devices mainly due to strong electron tunneling and thermionic emission. Predicted recovery times are corroborated by bias and temperature dependent time-resolved photoluminescence measurements indicating (<= 30 ps) recovery times. This makes GaInAsSb QW an attractive material particularly for electroabsorption modulators and saturable absorbers. (C) 2013 American Institute of Physics. (http://dx.doi.org/10.1063/1.4775371
“…11 Recently, much effort has been focused on exploring the GaInAsN/GaAs QW where adding small amounts of nitrogen(N) leads to favorable changes in band alignment and pushes the emission wavelength towards 1310 nm. [12][13][14] An impact of N incorporation is the deterioration of the optical properties as defect induced nonradiative recombination (NRR) increases with increasing N concentration, 15 although recent work has shown that the addition of minimal amount of N ( 0:5%) together with a post-growth annealing treatment (680 C, 10 min) in GaInAsN QW hinder from formation of N-N pairs and clusters and thus do not lead to reduction in the intrinsic gain of the active region. 16 While the NRR could be advantageous for fast saturable aborbers (SAs) and electroabsorption modulators (EAMs) as an additional carrier recombination process, 17,18 it is largely detrimental for the gain properties, with lasing threshold densities remaining relatively high.…”
The electro-optic properties of strained GaInAsSb/GaAs quantum wells (QWs) are investigated. A single QW p-i-n sample was grown by molecular beam epitaxy with antimony (Sb) pre-deposition technique. We numerically predict and experimentally verify a strong quantum confined Stark shift of 40 nm. We also predict a fast absorption recovery times crucial of high-speed optoelectronic devices mainly due to strong electron tunneling and thermionic emission. Predicted recovery times are corroborated by bias and temperature dependent time-resolved photoluminescence measurements indicating (<= 30 ps) recovery times. This makes GaInAsSb QW an attractive material particularly for electroabsorption modulators and saturable absorbers. (C) 2013 American Institute of Physics. (http://dx.doi.org/10.1063/1.4775371
“…The unusually strong bowing in the fundamental band gap as a function of nitrogen (N) composition has been well studied in GaN 1−x As x alloys with low N contents in accordance with the conduction band anticrossing (BAC) model, [1][2][3][4] which are potential materials for high-efficiency hybrid solar cells, 5) long-wavelength optoelectronic devices, 6) and photoanode applications in hydrogen production. 7) On the other hand, for N-rich GaNAs, [8][9][10] the structure of the valence band (VB) is explained by the hybridization of the localized arsenic (As) states with the extended VB states of the GaN matrix.…”
GaN1−xAsx alloys have been successfully grown on (100) GaAs substrates over a wide composition range (0.15 < x < 0.98) by plasma-assisted molecular beam epitaxy. In the middle composition range, the weak and broad (111) diffraction peaks are observed in the X-ray diffraction patterns. These diffraction peaks most likely come from small crystalline grains within the amorphous matrix and are unlike the entirely amorphous GaNAs alloys grown on sapphire and Pyrex glass. A transmission electron microscopy micrograph of the GaN0.50As0.50 alloy also shows a weak periodic structure consisting of small polycrystalline grains. To study the band gap and the As-affected spin–orbit band to conduction-band minimum transition, photomodulated reflectance is utilized. The band gap energies range from 0.78 to 2.15 eV (3.4 eV for end-point compounds GaN). Finally, the original and modified band anticrossing (BAC) models for GaNAs alloys were thoroughly verified over the entire composition range. Remarkably, the band gap energies of the partially polycrystalline GaNAs alloys agree well with those obtained using the original BAC model in the middle composition range because the model has been developed for crystalline materials. These results improve the growth of highly mismatched GaNAs alloys with different substrates and should expedite studies of high-efficiency multijunction solar cells fabricated using such a single ternary alloy system.
“…Undoubtedly, during the last decade, semiconductor waveguides with strong nonlinear effects, such as the silicon and chalcogenide waveguide, have attracted tremendous attention [1,2], and have been considerably investigated and demonstrated to realize compactly optoelectronic devices for wavelength conversion [3,4], optical switching [5,6], modulation [7,8], and light propagation [9,10]. Compared to the significant previous reports, the passive GaAs semiconductor waveguide has stronger third order nonlinearity and 2-photon absorption coefficients [11,12] and so it can be considered another highly nonlinear medium, and has already been investigated in wavelength conversion, optical switching, and other potential applications [13][14][15][16]. In general, it is thought that the GaAs based waveguide is strictly limited in signal processing due to its enhanced free carrier related effects.…”
This paper presents a simulation and investigation about the nonlinear interplay between an optical pulse and GaAs waveguide. The results obtained show that the nonlinear processes including self-phase modulation, 2-photon absorption, and free carrier related effects will have significant influences on the temporal shape and frequency spectrum of a propagating pulse in the GaAs waveguide with the result that 2-photon absorption can extend the pulse duration that can be again compressed by the free carrier absorption. The outcome spectrum is also asymmetrical due to the free carrier related effects, which takes on a complicated oscillation structure resulting from the interference. In addition, an interesting phenomenon is that the input pulse will eventually evolve into a double pulse along the GaAs waveguide by means of judiciously adjusting the intensity, waveform, and time duration of the input pulse, i.e. when the time duration of the input pulse is larger than the carrier lifetime, the input pulse with high enough intensity can develop into a double pulse at the end of the waveguide.
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