1989
DOI: 10.1002/pssb.2221540216
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Long‐Wavelength Optical Phonons in GaAsAlAs Superlattices

Abstract: Optical phonons in polar semiconductor superlattices near the zone center are studied. The microscopic theory based on a rigid-ion model is simplified by restriction to one elastic force constant per material and spatial average of the long-range electric field. The theory allows much insight into the mode structure, particularly anisotropy and layer thickness dependence of frequencies, atomic displacements, and accompanying electric fields. Explicit results are given for short-period GaAs-A1As superlattices. … Show more

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Cited by 31 publications
(5 citation statements)
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References 30 publications
(7 reference statements)
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“…3). The reasons for such drastic changes going from 8 = 0 to 8 + 0 have been discussed in a previous paper [25]. We note that all other wave vectors are shifted to higher values in the same manner.…”
Section: According To the Conditions (13) The Confinement Wave Vectorsupporting
confidence: 65%
See 1 more Smart Citation
“…3). The reasons for such drastic changes going from 8 = 0 to 8 + 0 have been discussed in a previous paper [25]. We note that all other wave vectors are shifted to higher values in the same manner.…”
Section: According To the Conditions (13) The Confinement Wave Vectorsupporting
confidence: 65%
“…Generally we do this numerically. Thereby we neglect the difference of the ion charges in GaAs and &As, setting el" = and f2 and this ion charge e* are adjusted to fit the experimental values wTol, wLol and wTO2 of the bulk zone-center optical phonons [25]. An analytical solution can be tried to find if the wave-vector dispersion of the bulk branches is omitted.…”
Section: Solutionsmentioning
confidence: 99%
“…Optical phonon modes in quantum wells (QW) and superlattices (SL) have been calculated by several authors [1][2][3][4][5][6][7][8][9][10][11][12][13] on the basis of classical theory of phonon modes for bulk materials and the electrodynamics. The equation of motion is where u , E, and M are the mechanical displacement field, the long-range electric field and the reduced mass of the unit cell, respectively.…”
Section: Introductionmentioning
confidence: 99%
“…Microscopic models of the behaviour of optical phonons in semiconductor heterostructures necessarily involve extensive numerical calculations [1][2][3][4][5][6][7][8]. A simple macroscopic model giving analytical results close to those of microscopic models would be useful in studies of the interaction of phonons with electrons and light.…”
mentioning
confidence: 99%