“…For reason of clarity we concentrate on the lowest three energy electronic states p e1 = {1, 0, +1}, p e2 = {2, 0, +1}, p e3 = {3, 0, +1}, the highest heavy hole state p h1 = {1, 0, +1}, and inter-band optical transitions between them satisfying the selection rule: l h -l e = 0 (see Ref. [5][6][7]14]). The corresponding allowed transition energies are shown Fig.…”