Crystal structure and thermoelectric performance of p–type Bi0.86Ba0.14CuSeO/Cu2–ySe composites

Bi0.86Ba0.14CuSeO/xCu2–ySe (0.05 ≤ x ≤ 0.15; y = 0 and 0.2) composites were fabricated by spark plasma sintering, and the crystal structure and thermoelectric properties of the Bi0.86Ba0.14CuSeO/xCu2–ySe composites were studied. The composites contained Cu2–ySe (y = 0 and 0.2) nanoinclusions in a te...

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Main Authors: H.Y. Hong, D.H. Kim, S.O. Won, J.K. Lee, S.D. Park, S.–M. Choi, S.H. Bae, K. Park
Format: Article
Language:English
Published: Elsevier 2021-07-01
Series:Journal of Materials Research and Technology
Subjects:
Online Access:http://www.sciencedirect.com/science/article/pii/S2238785421003604
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author H.Y. Hong
D.H. Kim
S.O. Won
J.K. Lee
S.D. Park
S.–M. Choi
S.H. Bae
K. Park
author_facet H.Y. Hong
D.H. Kim
S.O. Won
J.K. Lee
S.D. Park
S.–M. Choi
S.H. Bae
K. Park
author_sort H.Y. Hong
collection DOAJ
description Bi0.86Ba0.14CuSeO/xCu2–ySe (0.05 ≤ x ≤ 0.15; y = 0 and 0.2) composites were fabricated by spark plasma sintering, and the crystal structure and thermoelectric properties of the Bi0.86Ba0.14CuSeO/xCu2–ySe composites were studied. The composites contained Cu2–ySe (y = 0 and 0.2) nanoinclusions in a tetragonal Bi0.86Ba0.14CuSeO matrix. To increase the electrical conductivities of Bi0.86Ba0.14CuSeO, we introduced Cu2–ySe nanoinclusions with a high electrical conductivity into the matrix. The introduction of Cu2–ySe nanoinclusions reduced the structural distortion of CuSe4 tetrahedra and the effective mass, thereby enhancing the carrier mobility. A significant increase in electrical conductivities was achieved with increasing Cu2–ySe nanoinclusion, i.e., 117, 165, and 214 Ω−1cm−1 at 673 K for x = 0.05, 0.10, and 0.15 composites. The Cu2–ySe nanoinclusions reduced the lattice thermal conductivity because they strengthened the long–wavelength phonon scattering at the Bi0.86Ba0.14CuSeO/Cu2–ySe interface. The largest dimensionless figure–of–merit (0.33 at 673 K) was obtained for x = 0.15 composite, which was attributed to the highest electrical conductivity and the lowest lattice thermal conductivity.
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spelling doaj.art-77e5ad6d2e904dd4b11ebec0058486f52022-12-21T18:51:18ZengElsevierJournal of Materials Research and Technology2238-78542021-07-0113894905Crystal structure and thermoelectric performance of p–type Bi0.86Ba0.14CuSeO/Cu2–ySe compositesH.Y. Hong0D.H. Kim1S.O. Won2J.K. Lee3S.D. Park4S.–M. Choi5S.H. Bae6K. Park7Faculty of Nanotechnology and Advanced Materials Engineering, Sejong University, Seoul, 05006, South KoreaFaculty of Nanotechnology and Advanced Materials Engineering, Sejong University, Seoul, 05006, South KoreaAdvanced Analysis Center, Korea Institute of Science and Technology (KIST), Seoul, 02792, South KoreaEnergy Conversion Research Center, Korea Electrotechnology Research Institute, Changwon, 51543, Republic of KoreaEnergy Conversion Research Center, Korea Electrotechnology Research Institute, Changwon, 51543, Republic of KoreaSchool of Energy, Materials and Chemical Engineering, Korea University of Technology and Education, Cheonan, 330−708, South KoreaSchool of Energy, Materials and Chemical Engineering, Korea University of Technology and Education, Cheonan, 330−708, South KoreaFaculty of Nanotechnology and Advanced Materials Engineering, Sejong University, Seoul, 05006, South Korea; Corresponding author.Bi0.86Ba0.14CuSeO/xCu2–ySe (0.05 ≤ x ≤ 0.15; y = 0 and 0.2) composites were fabricated by spark plasma sintering, and the crystal structure and thermoelectric properties of the Bi0.86Ba0.14CuSeO/xCu2–ySe composites were studied. The composites contained Cu2–ySe (y = 0 and 0.2) nanoinclusions in a tetragonal Bi0.86Ba0.14CuSeO matrix. To increase the electrical conductivities of Bi0.86Ba0.14CuSeO, we introduced Cu2–ySe nanoinclusions with a high electrical conductivity into the matrix. The introduction of Cu2–ySe nanoinclusions reduced the structural distortion of CuSe4 tetrahedra and the effective mass, thereby enhancing the carrier mobility. A significant increase in electrical conductivities was achieved with increasing Cu2–ySe nanoinclusion, i.e., 117, 165, and 214 Ω−1cm−1 at 673 K for x = 0.05, 0.10, and 0.15 composites. The Cu2–ySe nanoinclusions reduced the lattice thermal conductivity because they strengthened the long–wavelength phonon scattering at the Bi0.86Ba0.14CuSeO/Cu2–ySe interface. The largest dimensionless figure–of–merit (0.33 at 673 K) was obtained for x = 0.15 composite, which was attributed to the highest electrical conductivity and the lowest lattice thermal conductivity.http://www.sciencedirect.com/science/article/pii/S2238785421003604CeramicsOxide materialsElectrical transportMicrostructureThermoelectric
spellingShingle H.Y. Hong
D.H. Kim
S.O. Won
J.K. Lee
S.D. Park
S.–M. Choi
S.H. Bae
K. Park
Crystal structure and thermoelectric performance of p–type Bi0.86Ba0.14CuSeO/Cu2–ySe composites
Journal of Materials Research and Technology
Ceramics
Oxide materials
Electrical transport
Microstructure
Thermoelectric
title Crystal structure and thermoelectric performance of p–type Bi0.86Ba0.14CuSeO/Cu2–ySe composites
title_full Crystal structure and thermoelectric performance of p–type Bi0.86Ba0.14CuSeO/Cu2–ySe composites
title_fullStr Crystal structure and thermoelectric performance of p–type Bi0.86Ba0.14CuSeO/Cu2–ySe composites
title_full_unstemmed Crystal structure and thermoelectric performance of p–type Bi0.86Ba0.14CuSeO/Cu2–ySe composites
title_short Crystal structure and thermoelectric performance of p–type Bi0.86Ba0.14CuSeO/Cu2–ySe composites
title_sort crystal structure and thermoelectric performance of p type bi0 86ba0 14cuseo cu2 yse composites
topic Ceramics
Oxide materials
Electrical transport
Microstructure
Thermoelectric
url http://www.sciencedirect.com/science/article/pii/S2238785421003604
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