Quasiclassical Anderson transition and thermally activated percolative charge transport in single-crystalline ScN

Dheemahi Rao, Debendra Prasad Panda, Ashalatha Indiradevi Kamalasanan Pillai, Akhil Tayal, Magnus Garbrecht, and Bivas Saha
Phys. Rev. B 109, 155307 – Published 25 April 2024

Abstract

Quasiclassical Anderson transition (QAT) represents the crossover from metallic to activated conduction in heavily doped highly compensated semiconductors (HDHCSs) due to large-scale potential fluctuations. The spatial inhomogeneity of the charged dopants in HDHCSs localizes carriers, forming metallic droplets surrounded by potential barriers. Nitride semiconductors are seldom explored for HDHCS studies due to the difficulty in synthesizing stoichiometric high-quality films and self-compensation effects. Here we show conclusive experimental evidence of the QAT in compensated scandium nitride (ScN) single-crystalline films. Mg (hole) doping in n-type ScN increases the resistivity by nine orders and leads to semi-insulating films exhibiting a distinct crossover from the hopping conduction at low temperatures to thermally activated percolative transport at high temperature. The sign reversal of the Seebeck coefficient, anomalously low Hall mobility that increases with raising temperature, and persistent photoconductivity support the QAT and carrier transport mechanisms. QAT in single-crystalline nitrides could lead to lattice-matched devices with lasers, modulators, and dynamic holographic applications.

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  • Received 15 May 2023
  • Revised 21 February 2024
  • Accepted 1 April 2024

DOI:https://doi.org/10.1103/PhysRevB.109.155307

©2024 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Dheemahi Rao1,2, Debendra Prasad Panda1, Ashalatha Indiradevi Kamalasanan Pillai3, Akhil Tayal4, Magnus Garbrecht3, and Bivas Saha1,2,5,*

  • 1Chemistry and Physics of Materials Unit, Jawaharlal Nehru Centre for Advanced Scientific Research, Bangalore 560064, India
  • 2International Centre for Materials Science, Jawaharlal Nehru Centre for Advanced Scientific Research, Bangalore 560064, India
  • 3Sydney Microscopy and Microanalysis, The University of Sydney, Camperdown, New South Wales 2006, Australia
  • 4Deutsches Elektronen-Synchrotron (DESY), 22607 Hamburg, Germany
  • 5School of Advanced Materials (SAMat), Jawaharlal Nehru Centre for Advanced Scientific Research, Bangalore 560064, India

  • *Corresponding author: bsaha@jncasr.ac.in; bivas.mat@gmail.com

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Issue

Vol. 109, Iss. 15 — 15 April 2024

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