Room temperature two-dimensional electron gas scattering time, effective mass, and mobility parameters in AlxGa1−xN/GaN heterostructures (0.07 ≤ x ≤ 0.42)

Author:

Knight Sean123ORCID,Richter Steffen123ORCID,Papamichail Alexis12ORCID,Kühne Philipp12,Armakavicius Nerijus12ORCID,Guo Shiqi12ORCID,Persson Axel R.14ORCID,Stanishev Vallery12ORCID,Rindert Viktor3ORCID,Persson Per O. Å.4ORCID,Paskov Plamen P.1ORCID,Schubert Mathias235ORCID,Darakchieva Vanya123ORCID

Affiliation:

1. Center for III-Nitride Technology (C3NiT—Janzén), Department of Physics, Chemistry and Biology (IFM), Linköping University 1 , 581 83 Linköping, Sweden

2. Terahertz Materials Analysis Center (THeMAC), Department of Physics, Chemistry and Biology (IFM), Linköping University 2 , 581 83 Linköping, Sweden

3. Solid State Physics and NanoLund, Lund University 3 , 22100 Lund, Sweden

4. Thin Film Physics Division, Department of Physics, Chemistry and Biology (IFM), Linköping University 4 , 581 83 Linköping, Sweden

5. Department of Electrical and Computer Engineering, University of Nebraska-Lincoln 5 , Lincoln, Nebraska 68588, USA

Abstract

AlxGa1−xN/GaN high-electron-mobility transistor (HEMT) structures are key components in electronic devices operating at gigahertz or higher frequencies. In order to optimize such HEMT structures, understanding their electronic response at high frequencies and room temperature is required. Here, we present a study of the room temperature free charge carrier properties of the two-dimensional electron gas (2DEG) in HEMT structures with varying Al content in the AlxGa1−xN barrier layers between x=0.07 and x=0.42. We discuss and compare 2DEG sheet density, mobility, effective mass, sheet resistance, and scattering times, which are determined by theoretical calculations, contactless Hall effect, capacitance-voltage, Eddy current, and cavity-enhanced terahertz optical Hall effect (THz-OHE) measurements using a low-field permanent magnet (0.6 T). From our THz-OHE results, we observe that the measured mobility reduction from x=0.13 to x=0.42 is driven by the decrease in 2DEG scattering time, and not the change in effective mass. For x<0.42, the 2DEG effective mass is found to be larger than for electrons in bulk GaN, which in turn, contributes to a decrease in the principally achievable mobility. From our theoretical calculations, we find that values close to 0.3m0 can be explained by the combined effects of conduction band nonparabolicity, polarons, and hybridization of the electron wavefunction through penetration into the barrier layer.

Publisher

AIP Publishing

Subject

General Physics and Astronomy

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