Giant bowing of the band gap and spin-orbit splitting energy in GaP1−xBix dilute bismide alloys
Using spectroscopic ellipsometry measurements on GaP 1− x Bi x /GaP epitaxial layers up to x = 3.7% we observe a giant bowing of the direct band gap ( E g Γ ) and valence band spin-orbit splitting energy (Δ SO ). E g Γ (Δ SO ) is measured to decrease (increase) by approximately 200 meV (240 meV) wi...
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Published in | Scientific reports Vol. 9; no. 1; p. 6835 |
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Main Authors | , , , , , , , |
Format | Journal Article |
Language | English |
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Nature Publishing Group UK
02.05.2019
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Abstract | Using spectroscopic ellipsometry measurements on GaP
1−
x
Bi
x
/GaP epitaxial layers up to
x
= 3.7% we observe a giant bowing of the direct band gap (
E
g
Γ
) and valence band spin-orbit splitting energy (Δ
SO
).
E
g
Γ
(Δ
SO
) is measured to decrease (increase) by approximately 200 meV (240 meV) with the incorporation of 1% Bi, corresponding to a greater than fourfold increase in Δ
SO
in going from GaP to GaP
0.99
Bi
0.01
. The evolution of
E
g
Γ
and Δ
SO
with
x
is characterised by strong, composition-dependent bowing. We demonstrate that a simple valence band-anticrossing model, parametrised directly from atomistic supercell calculations, quantitatively describes the measured evolution of
E
g
Γ
and Δ
SO
with
x
. In contrast to the well-studied GaAs
1−
x
Bi
x
alloy
,
in GaP
1−
x
Bi
x
substitutional Bi creates localised impurity states lying energetically within the GaP host matrix band gap. This leads to the emergence of an optically active band of Bi-hybridised states, accounting for the overall large bowing of
E
g
Γ
and Δ
SO
and in particular for the giant bowing observed for
x
≲ 1%. Our analysis provides insight into the action of Bi as an isovalent impurity, and constitutes the first detailed experimental and theoretical analysis of the GaP
1−
x
Bi
x
alloy band structure. |
---|---|
AbstractList | Using spectroscopic ellipsometry measurements on GaP
1−
x
Bi
x
/GaP epitaxial layers up to
x
= 3.7% we observe a giant bowing of the direct band gap (
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\begin{document}$${E}_{g}^{{\rm{\Gamma }}}$$\end{document}
E
g
Γ
) and valence band spin-orbit splitting energy (Δ
SO
).
\documentclass[12pt]{minimal}
\usepackage{amsmath}
\usepackage{wasysym}
\usepackage{amsfonts}
\usepackage{amssymb}
\usepackage{amsbsy}
\usepackage{mathrsfs}
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\setlength{\oddsidemargin}{-69pt}
\begin{document}$${E}_{g}^{{\rm{\Gamma }}}$$\end{document}
E
g
Γ
(Δ
SO
) is measured to decrease (increase) by approximately 200 meV (240 meV) with the incorporation of 1% Bi, corresponding to a greater than fourfold increase in Δ
SO
in going from GaP to GaP
0.99
Bi
0.01
. The evolution of
\documentclass[12pt]{minimal}
\usepackage{amsmath}
\usepackage{wasysym}
\usepackage{amsfonts}
\usepackage{amssymb}
\usepackage{amsbsy}
\usepackage{mathrsfs}
\usepackage{upgreek}
\setlength{\oddsidemargin}{-69pt}
\begin{document}$${E}_{g}^{{\rm{\Gamma }}}$$\end{document}
E
g
Γ
and Δ
SO
with
x
is characterised by strong, composition-dependent bowing. We demonstrate that a simple valence band-anticrossing model, parametrised directly from atomistic supercell calculations, quantitatively describes the measured evolution of
\documentclass[12pt]{minimal}
\usepackage{amsmath}
\usepackage{wasysym}
\usepackage{amsfonts}
\usepackage{amssymb}
\usepackage{amsbsy}
\usepackage{mathrsfs}
\usepackage{upgreek}
\setlength{\oddsidemargin}{-69pt}
\begin{document}$${E}_{g}^{{\rm{\Gamma }}}$$\end{document}
E
g
Γ
and Δ
SO
with
x
. In contrast to the well-studied GaAs
1−
x
Bi
x
alloy
,
in GaP
1−
x
Bi
x
substitutional Bi creates localised impurity states lying energetically within the GaP host matrix band gap. This leads to the emergence of an optically active band of Bi-hybridised states, accounting for the overall large bowing of
\documentclass[12pt]{minimal}
\usepackage{amsmath}
\usepackage{wasysym}
\usepackage{amsfonts}
\usepackage{amssymb}
\usepackage{amsbsy}
\usepackage{mathrsfs}
\usepackage{upgreek}
\setlength{\oddsidemargin}{-69pt}
\begin{document}$${E}_{g}^{{\rm{\Gamma }}}$$\end{document}
E
g
Γ
and Δ
SO
and in particular for the giant bowing observed for
x
≲ 1%. Our analysis provides insight into the action of Bi as an isovalent impurity, and constitutes the first detailed experimental and theoretical analysis of the GaP
1−
x
Bi
x
alloy band structure. Using spectroscopic ellipsometry measurements on GaP 1− x Bi x /GaP epitaxial layers up to x = 3.7% we observe a giant bowing of the direct band gap ( E g Γ ) and valence band spin-orbit splitting energy (Δ SO ). E g Γ (Δ SO ) is measured to decrease (increase) by approximately 200 meV (240 meV) with the incorporation of 1% Bi, corresponding to a greater than fourfold increase in Δ SO in going from GaP to GaP 0.99 Bi 0.01 . The evolution of E g Γ and Δ SO with x is characterised by strong, composition-dependent bowing. We demonstrate that a simple valence band-anticrossing model, parametrised directly from atomistic supercell calculations, quantitatively describes the measured evolution of E g Γ and Δ SO with x . In contrast to the well-studied GaAs 1− x Bi x alloy , in GaP 1− x Bi x substitutional Bi creates localised impurity states lying energetically within the GaP host matrix band gap. This leads to the emergence of an optically active band of Bi-hybridised states, accounting for the overall large bowing of E g Γ and Δ SO and in particular for the giant bowing observed for x ≲ 1%. Our analysis provides insight into the action of Bi as an isovalent impurity, and constitutes the first detailed experimental and theoretical analysis of the GaP 1− x Bi x alloy band structure. Abstract Using spectroscopic ellipsometry measurements on GaP 1− x Bi x /GaP epitaxial layers up to x = 3.7% we observe a giant bowing of the direct band gap ( $${E}_{g}^{{\rm{\Gamma }}}$$ E g Γ ) and valence band spin-orbit splitting energy (Δ SO ). $${E}_{g}^{{\rm{\Gamma }}}$$ E g Γ (Δ SO ) is measured to decrease (increase) by approximately 200 meV (240 meV) with the incorporation of 1% Bi, corresponding to a greater than fourfold increase in Δ SO in going from GaP to GaP 0.99 Bi 0.01 . The evolution of $${E}_{g}^{{\rm{\Gamma }}}$$ E g Γ and Δ SO with x is characterised by strong, composition-dependent bowing. We demonstrate that a simple valence band-anticrossing model, parametrised directly from atomistic supercell calculations, quantitatively describes the measured evolution of $${E}_{g}^{{\rm{\Gamma }}}$$ E g Γ and Δ SO with x . In contrast to the well-studied GaAs 1− x Bi x alloy , in GaP 1− x Bi x substitutional Bi creates localised impurity states lying energetically within the GaP host matrix band gap. This leads to the emergence of an optically active band of Bi-hybridised states, accounting for the overall large bowing of $${E}_{g}^{{\rm{\Gamma }}}$$ E g Γ and Δ SO and in particular for the giant bowing observed for x ≲ 1%. Our analysis provides insight into the action of Bi as an isovalent impurity, and constitutes the first detailed experimental and theoretical analysis of the GaP 1− x Bi x alloy band structure. Using spectroscopic ellipsometry measurements on GaP1−xBix/GaP epitaxial layers up to x = 3.7% we observe a giant bowing of the direct band gap (EgΓ) and valence band spin-orbit splitting energy (ΔSO). EgΓ (ΔSO) is measured to decrease (increase) by approximately 200 meV (240 meV) with the incorporation of 1% Bi, corresponding to a greater than fourfold increase in ΔSO in going from GaP to GaP0.99Bi0.01. The evolution of EgΓ and ΔSO with x is characterised by strong, composition-dependent bowing. We demonstrate that a simple valence band-anticrossing model, parametrised directly from atomistic supercell calculations, quantitatively describes the measured evolution of EgΓ and ΔSO with x. In contrast to the well-studied GaAs1−xBix alloy, in GaP1−xBix substitutional Bi creates localised impurity states lying energetically within the GaP host matrix band gap. This leads to the emergence of an optically active band of Bi-hybridised states, accounting for the overall large bowing of EgΓ and ΔSO and in particular for the giant bowing observed for x ≲ 1%. Our analysis provides insight into the action of Bi as an isovalent impurity, and constitutes the first detailed experimental and theoretical analysis of the GaP1−xBix alloy band structure. |
ArticleNumber | 6835 |
Author | Sweeney, Stephen J. Nattermann, Lukas Bushell, Zoe L. Rorison, Judy M. Broderick, Christopher A. Volz, Kerstin Joseph, Rita Keddie, Joseph L. |
Author_xml | – sequence: 1 givenname: Zoe L. orcidid: 0000-0002-7353-2847 surname: Bushell fullname: Bushell, Zoe L. organization: Advanced Technology Institute and Department of Physics, University of Surrey – sequence: 2 givenname: Christopher A. orcidid: 0000-0002-5370-7582 surname: Broderick fullname: Broderick, Christopher A. email: c.broderick@umail.ucc.ie organization: Tyndall National Institute, Lee Maltings, Dyke Parade, Department of Electrical and Electronic Engineering, University of Bristol – sequence: 3 givenname: Lukas surname: Nattermann fullname: Nattermann, Lukas organization: Materials Science Center and Faculty of Physics, Philipps-Universität Marburg – sequence: 4 givenname: Rita surname: Joseph fullname: Joseph, Rita organization: Advanced Technology Institute and Department of Physics, University of Surrey – sequence: 5 givenname: Joseph L. surname: Keddie fullname: Keddie, Joseph L. organization: Advanced Technology Institute and Department of Physics, University of Surrey – sequence: 6 givenname: Judy M. surname: Rorison fullname: Rorison, Judy M. organization: Department of Electrical and Electronic Engineering, University of Bristol – sequence: 7 givenname: Kerstin surname: Volz fullname: Volz, Kerstin organization: Materials Science Center and Faculty of Physics, Philipps-Universität Marburg – sequence: 8 givenname: Stephen J. surname: Sweeney fullname: Sweeney, Stephen J. email: s.sweeney@surrey.ac.uk organization: Advanced Technology Institute and Department of Physics, University of Surrey |
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Snippet | Using spectroscopic ellipsometry measurements on GaP
1−
x
Bi
x
/GaP epitaxial layers up to
x
= 3.7% we observe a giant bowing of the direct band gap (
E
g
Γ
)... Abstract Using spectroscopic ellipsometry measurements on GaP 1− x Bi x /GaP epitaxial layers up to x = 3.7% we observe a giant bowing of the direct band gap... Using spectroscopic ellipsometry measurements on GaP1−xBix/GaP epitaxial layers up to x = 3.7% we observe a giant bowing of the direct band gap (EgΓ) and... Using spectroscopic ellipsometry measurements on GaP 1− x Bi x /GaP epitaxial layers up to x = 3.7% we observe a giant bowing of the direct band gap (... |
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SourceType | Open Access Repository Aggregation Database Publisher |
StartPage | 6835 |
SubjectTerms | 132/122 639/301/119/1000 639/301/119/995 Alloys Humanities and Social Sciences multidisciplinary Science Science (multidisciplinary) Splitting |
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Title | Giant bowing of the band gap and spin-orbit splitting energy in GaP1−xBix dilute bismide alloys |
URI | https://link.springer.com/article/10.1038/s41598-019-43142-5 https://www.proquest.com/docview/2218969114 https://search.proquest.com/docview/2229228744 https://pubmed.ncbi.nlm.nih.gov/PMC6497675 |
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