Abstract
Luminescence and Raman spectroscopy using high-density tunable laser sources in the bound exciton region of CdS yield new informations about excitation channels and excited states of the four-particle (A°,X) complex. Excitation spectroscopy of the I1 luminescence due to the recombination of the (A°,X) complex with two A-valence-band holes in its electronic ground state led to the identification of four fine structure levels of the (A°,XB) complex with one hole from the second B valence band. Excitation with light of polarization and of an energy which coincides with one of these four levels, split off by hole-hole and electron-hole exchange interaction, is followed by a B-A hole conversion and subsequent I1 recombination of the complex. The sharp and strong excitation resonances due to the (A°,XB) levels allow measurements in a magnetic field giving detailed informations about the nature of these states and the interaction mechanisms involved. Investigations of a resonant electronic Raman effect due to hole scattering from the B to the A valence band within the (A°,X) complex supported these results. Four Raman lines showing resonance behaviour successively at the four (A°,XB) levels with distinctly different properties from known low-density Raman spectroscopy1 could be observed. Polarization and magnetic field dependent measurements were used to identify the Raman mechanism to be a one-photon resonant electronic scattering process within the (A°,X) levels while gain measurements and the observation of a mode structure in the high-density excitation spectra supported the excistance of stimulated Raman transitions. High-density excitation spectra of the I1 bound exciton with polarization showed resonances due to first order forbidden electronic excited states2 of the (A°,XA) complex. Extremely high excitation intensities led to the observation of vibration like resonances of the I1 luminescence. Intensity, temperature and magnetic field dependent measurements enabled us to develop a theoretical model to explain these resonances to be vibrations of the particles within the (A°,X) complex analogous to the case of a diatomic molecule.
© 1984 Optical Society of America
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