2004
DOI: 10.1016/j.jcrysgro.2004.08.055
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Pendeoepitaxy of GaAs and In0.15Ga0.85As using laterally oxidized GaAs/Al0.96Ga0.04As templates

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Cited by 2 publications
(2 citation statements)
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“…[18] The ACF of the In 0.83 Ga 0.17 As detector displayed random periodic oscillations with a relatively larger amplitude and peak-to-peak period, as shown in Figure 3f, owing to a shorter diffusion length of Ga ad-atoms with a larger activation energy for surface diffusion than that of In ad-atoms, resulting in a higher density of surface ledge steps and a rougher surface. [20,21] Figure 4a shows the temperature-dependent photoluminescence (PL) spectra of the InGaAs and InAsP detectors measured in the temperature range of 60-300 K. The energy bandgaps were plotted as a function of temperature, as shown in Figure 4b, to indicate bandgap narrowing with an increase in temperature due to electron-phonon interactions and lattice thermal expansion. [22] The temperature dependence of the fundamental bandgaps (E g ) was well fitted using the O'Donnell and Chen equation to account for the temperature-dependent electron-phonon coupling.…”
Section: Resultsmentioning
confidence: 99%
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“…[18] The ACF of the In 0.83 Ga 0.17 As detector displayed random periodic oscillations with a relatively larger amplitude and peak-to-peak period, as shown in Figure 3f, owing to a shorter diffusion length of Ga ad-atoms with a larger activation energy for surface diffusion than that of In ad-atoms, resulting in a higher density of surface ledge steps and a rougher surface. [20,21] Figure 4a shows the temperature-dependent photoluminescence (PL) spectra of the InGaAs and InAsP detectors measured in the temperature range of 60-300 K. The energy bandgaps were plotted as a function of temperature, as shown in Figure 4b, to indicate bandgap narrowing with an increase in temperature due to electron-phonon interactions and lattice thermal expansion. [22] The temperature dependence of the fundamental bandgaps (E g ) was well fitted using the O'Donnell and Chen equation to account for the temperature-dependent electron-phonon coupling.…”
Section: Resultsmentioning
confidence: 99%
“…[ 18 ] The ACF of the In 0.83 Ga 0.17 As detector displayed random periodic oscillations with a relatively larger amplitude and peak‐to‐peak period, as shown in Figure 3f, owing to a shorter diffusion length of Ga ad‐atoms with a larger activation energy for surface diffusion than that of In ad‐atoms, resulting in a higher density of surface ledge steps and a rougher surface. [ 20,21 ]…”
Section: Resultsmentioning
confidence: 99%