We determine the composition dependence of the transverse and longitudinal optical infrared-active phonon modes in rhombohedral α-(AlxGa1−x)2O3 alloys by far-infrared and infrared generalized spectroscopic ellipsometry. Single-crystalline high quality undoped thin-films grown on m-plane oriented α-Al2O3 substrates with x = 0.18, 0.37, and 0.54 were investigated. A single mode behavior is observed for all phonon modes, i.e., their frequencies shift gradually between the equivalent phonon modes of the isostructural binary parent compounds. We also provide physical model line shape functions for the anisotropic dielectric functions. We use the anisotropic high-frequency dielectric constants for polarizations parallel and perpendicular to the lattice c axis measured recently by Hilfiker et al. [Appl. Phys. Lett. 119, 092103 (2021)], and we determine the anisotropic static dielectric constants using the Lyddane–Sachs–Teller relation. The static dielectric constants can be approximated by linear relationships between those of α-Ga2O3 and α-Al2O3. The optical phonon modes and static dielectric constants will become useful for device design and free charge carrier characterization using optical techniques.
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14 March 2022
Research Article|
March 16 2022
Infrared-active phonon modes and static dielectric constants in α-(AlxGa1−x)2O3 (0.18 x 0.54) alloys Available to Purchase
Special Collection:
Wide- and Ultrawide-Bandgap Electronic Semiconductor Devices
Megan Stokey
;
Megan Stokey
a)
1
Department of Electrical and Computer Engineering, University of Nebraska-Lincoln
, Lincoln, Nebraska 68588, USA
a)Author to whom correspondence should be addressed: [email protected]. URL: http://ellipsometry.unl.edu
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Teresa Gramer
;
Teresa Gramer
1
Department of Electrical and Computer Engineering, University of Nebraska-Lincoln
, Lincoln, Nebraska 68588, USA
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Rafał Korlacki
;
Rafał Korlacki
1
Department of Electrical and Computer Engineering, University of Nebraska-Lincoln
, Lincoln, Nebraska 68588, USA
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Sean Knight
;
Sean Knight
2
Terahertz Materials Analysis Center and Center for III-N Technology, C3NiT–Janzèn, Department of Physics, Chemistry and Biology (IFM), Linköping University
, 58183 Linköping, Sweden
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Steffen Richter
;
Steffen Richter
2
Terahertz Materials Analysis Center and Center for III-N Technology, C3NiT–Janzèn, Department of Physics, Chemistry and Biology (IFM), Linköping University
, 58183 Linköping, Sweden
3
NanoLund and Solid State Physics, Lund University
, 22100 Lund, Sweden
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Riena Jinno
;
Riena Jinno
4
School of Electrical and Computer Engineering, Cornell University
, Ithaca, New York 14853, USA
5
Department of Electronic Science and Engineering, Kyoto University
, Kyoto 615-8510, Japan
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Yongjin Cho
;
Yongjin Cho
4
School of Electrical and Computer Engineering, Cornell University
, Ithaca, New York 14853, USA
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Huili Grace Xing
;
Huili Grace Xing
4
School of Electrical and Computer Engineering, Cornell University
, Ithaca, New York 14853, USA
6
Department of Material Science and Engineering, Cornell University
, Ithaca, New York 14853, USA
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Debdeep Jena
;
Debdeep Jena
4
School of Electrical and Computer Engineering, Cornell University
, Ithaca, New York 14853, USA
6
Department of Material Science and Engineering, Cornell University
, Ithaca, New York 14853, USA
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Matthew Hilfiker
;
Matthew Hilfiker
1
Department of Electrical and Computer Engineering, University of Nebraska-Lincoln
, Lincoln, Nebraska 68588, USA
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Vanya Darakchieva
;
Vanya Darakchieva
2
Terahertz Materials Analysis Center and Center for III-N Technology, C3NiT–Janzèn, Department of Physics, Chemistry and Biology (IFM), Linköping University
, 58183 Linköping, Sweden
3
NanoLund and Solid State Physics, Lund University
, 22100 Lund, Sweden
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Mathias Schubert
Mathias Schubert
1
Department of Electrical and Computer Engineering, University of Nebraska-Lincoln
, Lincoln, Nebraska 68588, USA
2
Terahertz Materials Analysis Center and Center for III-N Technology, C3NiT–Janzèn, Department of Physics, Chemistry and Biology (IFM), Linköping University
, 58183 Linköping, Sweden
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Megan Stokey
1,a)
Teresa Gramer
1
Rafał Korlacki
1
Sean Knight
2
Steffen Richter
2,3
Riena Jinno
4,5
Yongjin Cho
4
Huili Grace Xing
4,6
Debdeep Jena
4,6
Matthew Hilfiker
1
Vanya Darakchieva
2,3
Mathias Schubert
1,2
1
Department of Electrical and Computer Engineering, University of Nebraska-Lincoln
, Lincoln, Nebraska 68588, USA
2
Terahertz Materials Analysis Center and Center for III-N Technology, C3NiT–Janzèn, Department of Physics, Chemistry and Biology (IFM), Linköping University
, 58183 Linköping, Sweden
3
NanoLund and Solid State Physics, Lund University
, 22100 Lund, Sweden
4
School of Electrical and Computer Engineering, Cornell University
, Ithaca, New York 14853, USA
5
Department of Electronic Science and Engineering, Kyoto University
, Kyoto 615-8510, Japan
6
Department of Material Science and Engineering, Cornell University
, Ithaca, New York 14853, USA
a)Author to whom correspondence should be addressed: [email protected]. URL: http://ellipsometry.unl.edu
Note: This paper is part of the APL Special Collection on Wide- and Ultrawide-Bandgap Electronic Semiconductor Devices.
Appl. Phys. Lett. 120, 112202 (2022)
Article history
Received:
January 20 2022
Accepted:
February 24 2022
Citation
Megan Stokey, Teresa Gramer, Rafał Korlacki, Sean Knight, Steffen Richter, Riena Jinno, Yongjin Cho, Huili Grace Xing, Debdeep Jena, Matthew Hilfiker, Vanya Darakchieva, Mathias Schubert; Infrared-active phonon modes and static dielectric constants in α-(AlxGa1−x)2O3 (0.18 x 0.54) alloys. Appl. Phys. Lett. 14 March 2022; 120 (11): 112202. https://doi.org/10.1063/5.0085958
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