Schottky-Barrier Electroreflectance: Application to GaAs

Abstract
We describe a Schottky-barrier electroreflectance (ER) technique for making high-resolution optical spectroscopic measurements on semiconducting materials. When combined with recent line-shape theories of low-field ER spectra, the method provides order-of-magnitude improvement in resolution of structure and accuracy in the determination of critical-point energies and broadening parameters as compared to previous spectroscopic work on higher interband transitions. The Schottky-barrier technique is applied to GaAs, where separate critical-point contributions of Γ and Δ symmetry in the E0 triplet are resolved for the first time, together with all members of the quadruplet at X. We find the values of critical-point energies Eg and broadening parameters Γ for the following transitions at 4.2 °K (all energies are in meV): E0(1517.7±0.5,<0.3); E0+Δ0(1859±1,6±2); E1(3043.9±1,28±1); E1+Δ1(3263.6±1,38±2); E0 triplet, Γ symmetry: (4488 ± 10, < 40 ± 5), (4659 ± 10, 30 ± 5), (5014 ± 15, 47 ± 10); E0 triplet, M1 transitions, Δ symmetry: (4529 ± 10, < 36 ± 5) and (4712 ± 10, 34 ± 5); E2 complex, Σ: (5137±10,104±10); E2 complex, X quadruplet: (4937 ± 10, 47 ± 10), (5014 ± 10, 47 ± 10), (5339 ± 10, 48 ± 10), (5415 ± 15, 50 ± 15). These values enable us to determine the following spin-orbit-splitting energies: Δ0=341±2 meV, Δ1=220±2 meV, Δ0 (at Γ)=171±15 meV, Δ0(at Δ)=183±15 meV, and Δ2=77±10 meV. The splitting of the lower conduction bands at X due to the antisymmetric potential is Δ2=402±10 meV. The E0 transitions of Δ symmetry are shown to lie about 10% of the way from Γ to X. By comparing the period of the large number of Franz-Keldysh oscillations observed at the E1+Δ1 transition with those of the E0+Δ0 transitions observed in the high-field measurements, we determine a value μT=(0.055±008)me for the transverse reduced mass at E1+Δ1. These results are compared to previous experimental measurements and to calculated energy-band structures for GaAs. The determination of critical-point symmetry in surface-barrier geometries in terms of the transformation properties of the third- and fourth-rank low-field ER line-shape tensors is also discussed. Finally, the vanishing of an ER spectrum at a hyperbolic critical point, a reduced-mass effect predicted by the general theory of the Franz-Keldysh effect, is observed for the first time.