Raman scattering and infrared studies are reported for the layer compound GaSe under hydrostatic pressures up to 4 GPa. The rigid-layer mode shifts towards higher frequencies with an initial pressure coefficient of 0.234 GPa^-1. The overall behavior is explained in terms of the volume anharmonicity characteristic of the van der Waals bonding. The internal bond-bending mode softens and the Born effective charge decreases linearly. By adopting the single-layer compressibility κₗ{}0.015 GPa^-1 we obtain a Gr\"uneisen parameter of -1.9 for the bond-bending mode and -0.55±{}0.05 for the effective charge, comparable to those of a tetrahedral semiconductor. Coexistence of such molecular and covalent characters leads to a nonlinear shift of the energy, Eg, of the Penn-Phillips oscillator. This behavior is shown to be described well by {Δ}Eg=Dₐ({Δ}a/a₀) +Dc({Δ}c/c₀) with the deformation potentials Dₐ=-7.6±{}1.0 eV for the a axis and Dc=1.06±{}0.16 eV for the c axis. These deformation potentials reflect the dimensionality of bonding network as well as the nature of the electronic structure.
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Kuroda et al. (1987) studied this question.
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