2002
DOI: 10.1063/1.1462849
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Temperature dependence of the Raman shift in GaAs conformal layers grown by hydride vapor phase epitaxy

Abstract: Raman spectra between room temperature and 350 °C were measured in GaAs layers grown by hydride vapor phase epitaxy on Si substrates using the selective conformal growth method. The contributions of the thermal expansion, anharmonic phonon decay, and strain are considered in order to analyze the Raman data. The tensile strain in the conventional GaAs/Si seed and in the conformal GaAs layers was determined from the Raman spectra. It is shown that the thin SiO2 layer between the GaAs and the Si substrate is a co… Show more

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Cited by 17 publications
(10 citation statements)
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“…S2 in the supplementary material) allows to estimate the temperature of the nanowires. 31 For power density of 1.4 MW/cm 2 , the nanowire temperature reaches ~ 700 K, that is enough to evaporate the arsenic layer from the nanowire surface.…”
Section: (B) Figures 5(a) and 5(b) Showmentioning
confidence: 99%
“…S2 in the supplementary material) allows to estimate the temperature of the nanowires. 31 For power density of 1.4 MW/cm 2 , the nanowire temperature reaches ~ 700 K, that is enough to evaporate the arsenic layer from the nanowire surface.…”
Section: (B) Figures 5(a) and 5(b) Showmentioning
confidence: 99%
“…2 has a bandwidth of 135 THz, from 2 to 20 μm, and is limited by the transmission of the material [14]. The spectrum contains a feature related to the 8.55 THz Raman shift in GaAs [15], which results in a Stokes peak near 16 μm. Harmonic generation results in features at 5.3 and 3.5 μm.…”
mentioning
confidence: 98%
“…The LO modes are shifted about 4 cm -1 , while the TO modes are 1.7 cm -1 . As it is known the Raman peak shifts are linear with the stress σ, [30][31][32] i.e. Δω=aσ and Δω=bσ for the LO-and TO-mode, respectively.…”
Section: Resultsmentioning
confidence: 99%