Premium
Forbidden luminescence and resonance Raman scattering of bound exciton states in CdS
Author(s) -
Baumert R.,
Broser I.,
Gutowski J.,
Hoffmann A.
Publication year - 1983
Publication title -
physica status solidi (b)
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.51
H-Index - 109
eISSN - 1521-3951
pISSN - 0370-1972
DOI - 10.1002/pssb.2221160130
Subject(s) - exciton , luminescence , raman scattering , excited state , atomic physics , resonance (particle physics) , scattering , raman spectroscopy , biexciton , chemistry , crystal (programming language) , excitation , phonon , molecular physics , physics , condensed matter physics , optics , quantum mechanics , computer science , programming language
A series of six energy levels is found at energy distances 2.5, 3.8, 4.7, 6.1, 7.0, and 8.3 meV on the high energy side of the neutral‐acceptor bound exciton I 1 in CdS. They appear in the emission and absorption spectra of some freshly grown virgin crystals and of some crystals damaged by laser‐irradiation. Resonance Raman scattering (RRS) establishes the new levels as intermediate states in every high quality crystal. These levels are interpreted as excited states of the bound exciton I 1 . The direct radiative recombination is forbidden due to parity selection rules. These selection rules are removed in symmetry disturbed crystals, at high excitation intensities, or by recombination with phonon participation. In consequence they are detected as forbidden luminescence, as LO phonon replica, or as 1‐LO‐ and 2‐LO‐Raman lines. The 2‐LO scattering cross section of the energy region of bound excitons in CdS is determined.
Accelerating Research
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom
Address
John Eccles HouseRobert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom