Abstract
The conductivity σ, quantum-based magnetoconductivity Δσ = σ(B) − σ(0), and Hall coefficient RH (= µH/σ) of degenerate, homoepitaxial, (010) Si-doped β-Ga2O3, have been measured over a temperature range T = 9–320 K and magnetic field range B = 0–10 kG. With ten atoms in the unit cell, the normal-mode phonon structure of β-Ga2O3 is very complex, with optical-phonon energies ranging from kTpo ~ 20–100 meV. For heavily doped samples, the phonon spectrum is further modified by doping disorder. We explore the possibility of developing a single function Tpo(T) that can be incorporated into both quantum and classical scattering theory such that Δσ vs B, Δσ vs T, and µH vs T are all well fitted. Surprisingly, a relatively simple function, Tpo(T) = 1.6 × 103{1 − exp[−(T + 1)/170]} K, works well for β-Ga2O3 without any additional fitting parameters. In contrast, Δσ vs T in degenerate ScN, which has only one optical phonon branch, is well fitted with a constant Tpo = 550 K. These results indicate that quantum conductivity enables an understanding of classical conductivity in disordered, multi-phonon semiconductors.
Highlights
The conductivity σ, quantum-based magnetoconductivity Δσ = σ(B) − σ(0), and Hall coefficient RH (= μH/σ) of degenerate, homoepitaxial, (010) Si-doped β-Ga2O3, have been measured over a temperature range T = 9–320 K and magnetic field range B = 0–10 kG
Polar-optical-phonon scattering in these materials can be effectively described in terms of only one longitudinal optical phonon, of energy kTpo[6], where k is Boltzmann’s constant and Tpo is the polar optical phonon temperature. (For reference, the table on p. 84 of 6 lists Tpo values for sixteen binary semiconductors.) In contrast, βGAO contains ten atoms in the unit cell and nine branches of optical phonons, greatly complicating the analysis
In this study, we will be concerned with degenerate Si-doped βGAO, which has the additional complication of disorder due to the random positions of the Si-dopant atoms[11,12,13]
Summary
84 of 6 lists Tpo values for sixteen binary semiconductors.) In contrast, βGAO contains ten atoms in the unit cell and nine branches of optical phonons, greatly complicating the analysis. Acoustic phonons scatter electrons elastically, or nearly so, and can affect μ in degenerate semiconductors at low temperatures[14]. On the other hand, lead to inelastic scattering and will have a strong effect on Δσ11–13.
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