Abstract:The refractive indices of GaAs at room temperature were determined from accurate double-beam reflectance measurements. The uncertainty in the refractive indices obtained by this technique is ±0.005. Measurements were made on high-purity n -type samples, n -type samples with free-electron concentrations from 5×1016 to 6.7×1018 cm−3, p -type samples with free-hole concentrations from 1.5×1016 to 1.6×1019 cm−3, and p -type samples heavily doped with the amphoteric impurity Si. These data agree with Marple's prism… Show more
“…2(b) show the results of fitting our model to available GaAs data for absorption [7] and refractive index [8].The discrete exciton [2] is fitted by using the double-Lorentzian LSF. In GaAs, the light-hole band becomes quite nonparabolic after about 0.06 eV away from the valence-band maximum [15].…”
Section: Resultsmentioning
confidence: 99%
“…2 (a) The best fit of our absorption model to the experimental data for high-purity GaAs [7] in the 2 nd zone which yields a broadening parameter of 9.8 meV. (b) Comparison of the refractive-index spectrum obtained by our procedure and the experimental data [8].…”
New improved formulas of refractive indices of III-V materials to energies somewhat above the band gap have been developed from an absorption model with Coulomb interaction and a double-Lorentzian model for broadening.
“…2(b) show the results of fitting our model to available GaAs data for absorption [7] and refractive index [8].The discrete exciton [2] is fitted by using the double-Lorentzian LSF. In GaAs, the light-hole band becomes quite nonparabolic after about 0.06 eV away from the valence-band maximum [15].…”
Section: Resultsmentioning
confidence: 99%
“…2 (a) The best fit of our absorption model to the experimental data for high-purity GaAs [7] in the 2 nd zone which yields a broadening parameter of 9.8 meV. (b) Comparison of the refractive-index spectrum obtained by our procedure and the experimental data [8].…”
New improved formulas of refractive indices of III-V materials to energies somewhat above the band gap have been developed from an absorption model with Coulomb interaction and a double-Lorentzian model for broadening.
“…1. The data are corrected for reflectivity using the refractive index values reported in [17]. The absorption coefficient is well described by Urbach's rule, as staked in expression (I), with KO = 8 x 10l6 cm-l and hw, = 1.634 eV.…”
The optical absorption a t the edge of the fundamental absorption band is investigated in highpurity and high-perfection GaAs crystah. The experimental curves show an exponential decay of the absorption coefficient as a function of the photon energy (Urbach's rule) with temperature dependent slope. Since the impurity contribution can be neglected, the data are analyzed within the framework of the polaron model of phonon-assisted transitions. The good agreement obtained between experimental and calculated curves makes it possible to conclude that the interaction of electrons with LO phonons plays a dominant role in shaping the intrinsic Urbach tail in GaAs. The same theoretical model is also applied successfully to I n P and InAs using previously published experimental data.Es wird die optische Absorption an der Kante der Grundgitterabsorptionsbande in hochreinen und hochperfekten GaAs-Kristallen untersucht. Die experimentellen Kurven zeigen einen exponentiellen Abfall des Absorptionskoeffizienten in Abhangigkeit von der Photonenenergie (Urbach'sche Regel) mit temperaturabhangigem Anstieg. Da die Storstellenbeitrage vernachlassigt werden konnen, werden die Daten im Rahmen des Polaronenmodells von phononenassistierten ubergangen analysiert. Die gute Ubereinstimmung zwischen experimentellen und berechneten Kurven macht den SchluB moglich, da13 die Wechselwirkung der Elektronen mit LO-Phononen eine dominierende Rolle fur die Form des Urbachausliufers in GaAs spielt. Dasselbe theoretische Model1 wird erfolgreich auch auf I n P und InAs unter Benutzung fruherer experimenteller Daten angewendet.
“…The free space wavelength of transmitted light ho was taken to be 0.84 pm. These values of ea and E , correspond to Alo~,,Ga,~,,As and Alo.,,Gao.65As as a material for an active layer and confinement layer [9] , [IO] .…”
Section: Framework Of Analysismentioning
confidence: 99%
“…[7] - [9] wasused [ 131. These lasers show impressive mode selectivity (high ratio of lasing to nonlasing mode intensities).…”
Section: Charles H Henry and R F Kazarinovmentioning
Abstract-Numerical analysis has been carried out for a waveguide with graded index and gain. I t is shown that the radiation peak of the fundamental mode is deflected as the gradient of either the index or gain increases. The high-order modes also change their peak intensity ratio as the gradient of index or gain increases. The behavior of the fundamental mode is suitable for use in a beam scanner while that of higher-order modes is suitable for use in a deflection switching of laser beams. The analysis also shows that the modal gain of higher-order modes becomes larger than that of the fundamental mode as the gradient of the index and gain increases, which provides some explanation for the wide laser beam scanning observed by Scifres et al.
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