Abstract
The selection rules for the indirect optical transition in ε- and γ-GaSe are investigated group-theoretically by using the band structure of β-GaSe calculated by Schlüter. Without taking into account the spin-orbit interaction, the indirect transition is allowed only for the light with polarization vector E parallel to the crystal c-axis (E⁄⁄c) in ε-GaSe as in β-GaSe, but it is allowed both for E⁄⁄c and for E⊥c in γ-GaSe. The irreducible representations of the phonon mode associated with the transitions are M1+(Ag) in β, M1(Ag) in ε and M1(A′) in γ. The M1(A′) mode of γ-GaSe is compatible with M1(Ag) and M3(Bg) of ε-GaSe, and with M1+(Ag), M3+(B2g), M2−(B3u) and M4−(B1u) of β-GaSe. So, the number of phohons associated with the indirect optical transition in GaSe is affected by the mixture of these modifications.