The electronic band structures of III nitride semiconductors calculated within
the adiabatic approximation give essential information about the optical
properties of materials. However, atoms of the lattice are not at rest; their
displacement away from the equilibrium positions perturbs the periodic
potential acting on the electrons in the crystal, leading to an
electron-phonon interaction energy. Due to different ways that the lattice
vibration perturbs the motions of electrons, there are various types of
interaction, such as Fröhlich interaction with longitudinal optical phonons,
deformation-potential interactions with optical and acoustic phonons and
piezoelectric interaction with acoustic phonons. These interactions,
especially the Fröhlich interaction, which is very strong due to the ionic
nature of III nitrides, have a great influence on the optical properties of
the III nitride semiconductors. As a result of electron-phonon interaction,
several phenomena, such as phonon replicas in the emission spectra,
homogeneous broadening of the excitonic line width and the relaxation of
hot carriers to the fundamental band edge, which have been observed in GaN and
its low dimensional heterostructures, are reviewed.
Time-resolved photoluminescence (PL), at T=8 K, is used to study a graded-width InGaN/GaN quantum well. Across the sample, the well width continuously varies from ∼5.5 to 2.0 nm corresponding to PL peak energies varying between 2.0 and 2.9 eV and to PL decay rates covering four orders of magnitude. The plot of decay times versus PL energies is very well fitted by a calculation of the electron–hole recombination probability versus well width. The only fitting parameter is the electric field in the well, which we find equal to 2.45±0.25 MV/cm, in excellent agreement with experimental Stokes shifts for this type of samples.
We report a cross-correlated investigation, performed by means of Raman scattering and infrared spectroscopy, of coupled LO phonon-plasmon modes in bulk GaN. Using different samples with different (high) residual concentrations of free carriers, we find that the high-energy Raman mode follows closely the plasma frequency resolved from the infrared data. On the opposite, the low-frequency modes appears down shifted, with respect to the standard TO phonon frequency, by about 11 cm−1. Both findings agree satisfactorily with predictions of the linear response theory for undamped phonon-plasmon modes and establish Raman scattering as a powerful and nondestructive tool to investigate the residual doping level of GaN up to about 1020 cm−3 .
We report micro-photoluminescence studies of single GaN/AlN quantum dots grown along the (0001) crystal axis by molecular beam epitaxy on Si(111) substrates. The emission lines exhibit a linear polarization along the growth plane, but with varying magnitudes of the polarization degree and with principal polarization axes that do not necessarily correspond to crystallographic directions. Moreover, we could not observe any splitting of polarized emission lines, at least within the spectral resolution of our setup (1 meV). We propose a model based on the joint effects of electron-hole exchange interaction and in-plane anisotropy of strain and/or quantum dot shape, in order to explain the quantitative differences between our observations and those previously reported on, e.g. CdTe-or InAs-based quantum dots.
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