Heterostructural interface engineering for ultrawide-gap nitrides from first principles: <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><mml:mrow><mml:mi>Ta</mml:mi><mml:mi mathvariant="normal">C</mml:mi><

Epitaxial lattice matching is an important condition for the formation of coherent interfaces with low defect densities. However, lattice-matched substrates with the same crystal structure as the active layer are often not available, suggesting opportunities for utilizing heterostructural interfaces. For example, at high <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><a:mi>Al</a:mi></a:math> contents that are interesting for ultrawide-gap applications in power electronics, <d:math xmlns:d="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><d:msub><d:mi>Al</d:mi><d:mi>x</d:mi></d:msub><d:msub><d:mi>Ga</d:mi><d:mrow><d:mn>1</d:mn><d:mo>−</d:mo><d:mi>x</d:mi></d:mrow></d:msub><d:mrow><d:mi mathvariant="normal">N</d:mi></d:mrow></d:math> semiconductor alloys in the (0001) orientation of the wurtzite (wz) structure become lattice-matched to (111)-oriented rocksalt (rs) <h:math xmlns:h="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><h:mrow><h:mi>Ta</h:mi><h:mi mathvariant="normal">C</h:mi></h:mrow></h:math> substrates. To predict the expected interface atomic structures under different synthesis conditions, we perform high-throughput density-functional-theory calculations, using an algorithm for systematic sampling of the possible stacking sequences of the atomic layers on the in-plane hexagonal lattice. The approach considers octahedral, tetrahedral, and prismatic coordination motifs, and is generally applicable for the modeling of commensurate rs/wz heterostructural interfaces. Our results provide guidance for synthesis control of substrate-film bonding and the polarity of ultrawide-gap <l:math xmlns:l="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><l:msub><l:mi>Al</l:mi><l:mi>x</l:mi></l:msub><l:msub><l:mi>Ga</l:mi><l:mrow><l:mn>1</l:mn><l:mo>−</l:mo><l:mi>x</l:mi></l:mrow></l:msub><l:mrow><l:mi mathvariant="normal">N</l:mi></l:mrow></l:math> alloys on <p:math xmlns:p="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><p:mrow><p:mi>Ta</p:mi><p:mi mathvariant="normal">C</p:mi></p:mrow></p:math> substrates. Published by the American Physical Society 2024

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Publication Details

Journal
Physical Review Applied
Published
2024-11-15
DOI
https://doi.org/10.1103/physrevapplied.22.054044
Citations
2
Primary Topic
GaN-based semiconductor devices and materials
Type
article
Field-Weighted Citation Impact
0.62

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article

Heterostructural interface engineering for ultrawide-gap nitrides from first principles: <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><mml:mrow><mml:mi>Ta</mml:mi><mml:mi mathvariant="normal">C</mml:mi><

Stephan Lany, Sharad Mahatara
2 citations
Physical Review Applied
GaN-based semiconductor devices and materials
0.62
article

Heterostructural interface engineering for ultrawide-gap nitrides from first principles: <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><mml:mrow><mml:mi>Ta</mml:mi><mml:mi mathvariant="normal">C</mml:mi><

Stephan Lany, Sharad Mahatara
article en
2 citations

Abstract

Epitaxial lattice matching is an important condition for the formation of coherent interfaces with low defect densities. However, lattice-matched substrates with the same crystal structure as the active layer are often not available, suggesting opportunities for utilizing heterostructural interfaces. For example, at high <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><a:mi>Al</a:mi></a:math> contents that are interesting for ultrawide-gap applications in power electronics, <d:math xmlns:d="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><d:msub><d:mi>Al</d:mi><d:mi>x</d:mi></d:msub><d:msub><d:mi>Ga</d:mi><d:mrow><d:mn>1</d:mn><d:mo>−</d:mo><d:mi>x</d:mi></d:mrow></d:msub><d:mrow><d:mi mathvariant="normal">N</d:mi></d:mrow></d:math> semiconductor alloys in the (0001) orientation of the wurtzite (wz) structure become lattice-matched to (111)-oriented rocksalt (rs) <h:math xmlns:h="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><h:mrow><h:mi>Ta</h:mi><h:mi mathvariant="normal">C</h:mi></h:mrow></h:math> substrates. To predict the expected interface atomic structures under different synthesis conditions, we perform high-throughput density-functional-theory calculations, using an algorithm for systematic sampling of the possible stacking sequences of the atomic layers on the in-plane hexagonal lattice. The approach considers octahedral, tetrahedral, and prismatic coordination motifs, and is generally applicable for the modeling of commensurate rs/wz heterostructural interfaces. Our results provide guidance for synthesis control of substrate-film bonding and the polarity of ultrawide-gap <l:math xmlns:l="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><l:msub><l:mi>Al</l:mi><l:mi>x</l:mi></l:msub><l:msub><l:mi>Ga</l:mi><l:mrow><l:mn>1</l:mn><l:mo>−</l:mo><l:mi>x</l:mi></l:mrow></l:msub><l:mrow><l:mi mathvariant="normal">N</l:mi></l:mrow></l:math> alloys on <p:math xmlns:p="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"><p:mrow><p:mi>Ta</p:mi><p:mi mathvariant="normal">C</p:mi></p:mrow></p:math> substrates. Published by the American Physical Society 2024

Physical Review AppliedVol. 22(5)
National Laboratory of the Rockies (US)
U.S. Department of Energy, National Energy Research Scientific Computing Center, Office of Science, Basic Energy Sciences, Advanced Scientific Computing Research, National Renewable Energy Laboratory, Lawrence Berkeley National Laboratory
Openalex Percentile: Top 32%
GaN-based semiconductor devices and materials
0.62
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