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We report the infrared radiative capture of electrons at ionized oxygen donors in gallium phosphide. The radiative transition occurs between a shallow excited state (ionization energy 51.5±{}2 meV) and the deep 1s(A₁) ground state (ionization energy 893±{}2 meV) of the donor. The uniaxial stress dependence of this transition suggests that the excited state is the doublet $1s(E)$. The luminescence is predominantly due to phonon-assisted transitions. Appreciable fine structure has been resolved in the vibronic sideband. Some of this structure involves phonons characteristic of pure gallium phosphide, but strong replicas associated with in-band-resonance modes of the oxygen impurity atom are also seen. The energies of the local modes are appreciably reduced when O¹⁶ is replaced by O¹⁸. In addition, the no-phonon transition energy decreases slightly by an amount anticipated from the no-phonon shift of donor-acceptor pair spectra involving the oxygen donor. The oxygen electron-capture luminescence is quenched in crystals containing {}5×{}10¹⁵ cm^-3 neutral acceptors and does not saturate as rapidly as the donor-acceptor pair luminescence. Two Auger transitions are suggested to account for these properties. Weak absorption lines due to no-phonon and phonon-assisted interbound-state excitations within the oxygen donor have been detected through measurements of the excitation spectrum of the oxygen luminescence in n-type crystals. A tentative assignment of the principal no-phonon absorption lines is given.
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Dean et al. (1968) studied this question.
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