Abstract

A theoretical calculation is presented of the so-called ``gap renormalization'' due to free carriers for the quasi-two-dimensional (2D) electrons or holes confined in a semiconductor quantum well. A general theory of the effect is developed assuming parabolic subbands, the Hubbard approximation (random-phase approximation) for the correlation energy, and a model potential containing the well thickness for the effective 2D Coulomb interaction. Results are presented for gap renormalization versus carrier density for GaAs wells of 81 and 217 A\r{} thickness. An experimental measurement of gap renormalization is presented which is based on an analysis of the excitation and luminescence spectra of a p-type modulation-doped Ga(${\mathrm{Ga}}_{1\mathrm{\ensuremath{-}}\mathrm{x}}$${\mathrm{Al}}_{\mathrm{x}}$)As multilayer sample of well width 107 A\r{} and hole density 5.3\ifmmode\times\else\texttimes\fi{}${10}^{10}$ ${\mathrm{cm}}^{\mathrm{\ensuremath{-}}2}$. The calculated value is in excellent agreement with the experimental value (6.3 meV) in this case.

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