Uniformly excited electron-hole plasma under three-dimensional confinement has been studied in Ga1-xAlx As by photoluminescence at 2 K. With this approach, a satisfactory fitting of the experimental data has been obtained over a wide range of densities and Al concentrations using a single value of density and temperature throughout the excited region. The theoretical model used is based on the preservation of k-selection rules with a built-in broadening in the single-particle density of states. The fitting renormalized gap closely agrees with existing many-body theories, contrary to recent claims. The possibilities of plasmon-replica contributions and of thermalization processes by recent claims. The possibilities of plasmon-replica contributions and of thermalization processes by impurity or disorder-activated scattering are discussed. A new estimate of the radiative-recombination coefficient is reported.
Electron-hole plasma in direct-gap Ga_{1-x}Al_{x} As and k-selection rule / M., Capizzi; Modesti, Silvio; A., Frova; J., Staehli; M., Guzzi; R., Logan. - In: PHYSICAL REVIEW. B, CONDENSED MATTER. - ISSN 0163-1829. - STAMPA. - 29:(1984), pp. 2028-2035. [10.1103/PhysRevB.29.2028]
Electron-hole plasma in direct-gap Ga_{1-x}Al_{x} As and k-selection rule
MODESTI, SILVIO;
1984-01-01
Abstract
Uniformly excited electron-hole plasma under three-dimensional confinement has been studied in Ga1-xAlx As by photoluminescence at 2 K. With this approach, a satisfactory fitting of the experimental data has been obtained over a wide range of densities and Al concentrations using a single value of density and temperature throughout the excited region. The theoretical model used is based on the preservation of k-selection rules with a built-in broadening in the single-particle density of states. The fitting renormalized gap closely agrees with existing many-body theories, contrary to recent claims. The possibilities of plasmon-replica contributions and of thermalization processes by recent claims. The possibilities of plasmon-replica contributions and of thermalization processes by impurity or disorder-activated scattering are discussed. A new estimate of the radiative-recombination coefficient is reported.Pubblicazioni consigliate
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