Electron effective mass in GaN revisited: New insights from terahertz and mid-infrared optical Hall effect

Author:

Armakavicius Nerijus123ORCID,Knight Sean123ORCID,Kühne Philipp123ORCID,Stanishev Vallery13ORCID,Tran Dat Q.123ORCID,Richter Steffen234ORCID,Papamichail Alexis12ORCID,Stokey Megan5ORCID,Sorensen Preston5ORCID,Kilic Ufuk5ORCID,Schubert Mathias245ORCID,Paskov Plamen P.12ORCID,Darakchieva Vanya1234ORCID

Affiliation:

1. Department of Physics, Chemistry and Biology (IFM), Linköping University 1 , 581 83 Linköping, Sweden

2. Center for III-Nitride Technology, C3NiT–Janzén, Linköping University 2 , 581 83 Linköping, Sweden

3. Terahertz Materials Analysis Center (THeMAC), Linköping University 3 , 581 83 Linköping, Sweden

4. NanoLund and Solid State Physics, Lund University 4 , 22100 Lund, Sweden

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

Abstract

Electron effective mass is a fundamental material parameter defining the free charge carrier transport properties, but it is very challenging to be experimentally determined at high temperatures relevant to device operation. In this work, we obtain the electron effective mass parameters in a Si-doped GaN bulk substrate and epitaxial layers from terahertz (THz) and mid-infrared (MIR) optical Hall effect (OHE) measurements in the temperature range of 38–340 K. The OHE data are analyzed using the well-accepted Drude model to account for the free charge carrier contributions. A strong temperature dependence of the electron effective mass parameter in both bulk and epitaxial GaN with values ranging from (0.18 ± 0.02) m0 to (0.34 ± 0.01) m0 at a low temperature (38 K) and room temperature, respectively, is obtained from the THz OHE analysis. The observed effective mass enhancement with temperature is evaluated and discussed in view of conduction band nonparabolicity, polaron effect, strain, and deviations from the classical Drude behavior. On the other hand, the electron effective mass parameter determined by MIR OHE is found to be temperature independent with a value of (0.200 ± 0.002) m0. A possible explanation for the different findings from THz OHE and MIR OHE is proposed.

Funder

VINNOVA

Vetenskapsrådet

Stiftelsen för Strategisk Forskning

Linkoping University, Faculty Grant

National Science Foundation

Air Force Office of Scientific Research

J. A. Woollam Foundation

Publisher

AIP Publishing

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