ISOTOPIC CONSTITUTION OF SEMICONDUCTORS - MANIFESTATIONS IN THEIR ELECTRONIC AND VIBRATIONAL-SPECTRA

Semiconductors are prime examples of crystals which can be grown with unprecedented purity, imperfections being introduced deliberately in a controlled manner. However; even the chemically purest semiconductor is isotopically disordered as dictated by the natural abundance of ele ments. Diamonds have 98.9% C-12 and 1.1% C-13; silicon consists of 92. 23% Si-28, 4.67% Si-29 and 3.1% Si-30 whereas germanium exhibits a lar ge isotopic disorder originating in 21.23% Ge-70, 27.66% Ge-72, 7.73% Ge-73, 35.94% Ge-74 and 7.44% Ge-78! The isotopic composition of singl e crystal diamonds, controlled by the starting material used for growt h by chemical vapor deposition followed by high temperature growth, pr ovides a splendid opportunity to address the subtle manifestations of zero-point motion in their Brillouin and Raman spectra. Isotopically p ure Ge shows mass dependent small shifts in its electronic band struct ure which can however be detected in the signatures observed in its mo dulated reflection and transmission spectra. The local modes of oxygen in isotopically pure Ge are observed by infrared spectroscopy as exce ptionally sharp lines with striking fine structure. Substitutional inc orporation of the lighter elements (e.g., Mg, Mn, Ca,...) in the II-VI semiconductors leads to sharp local modes (including isotopic shifts) in their infrared spectra.