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      Effects of Double Doping Germanium and Indium on the Thermoelectric Properties of Permingeatite

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      https://www.riss.kr/link?id=A108631936

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      다국어 초록 (Multilingual Abstract)

      Cu3Sb1–x–yGexInySe4 (0.02 ≤ x ≤ 0.12; 0.04 ≤ y ≤ 0.08) permingeatite compounds doped with Ge andIn were prepared using solid-state synthesis. The phases and microstructures were analyzed, and the chargetransport and thermoelectric properties were evaluated according to the Ge and In doping content. Most ofthe samples contained a single phase of permingeatite with a tetragonal structure; however, secondary phases(Cu0.875InSe2, In2Se3, and InSb) were detected in the samples with x = 0.12 and y = 0.08. Both the a-axis andc-axis lattice constants of permingeatite were increased by Ge and In doping, with a = 0.5651–0.5655 nm andc = 1.1249–1.1255 nm, but the change in lattice constant due to the change in doping amount wasinsignificant. The melting point of the sample double-doped with Ge and In was determined to be 736 K, whichwas lower than the melting point (741 K) of pure Cu3SbSe4. This lowering of the melting point was attributedto the formation of a solid solution. The electrical conductivity exhibited degenerate semiconductor behavior,decreasing with increasing temperature. As the Ge and In doping content increased, the carrier concentrationand electrical conductivity increased; however, when x ≥ 0.12, the electrical conductivity did not increasefurther. The Seebeck coefficient exhibited positive values and p-type conduction characteristics. In addition,intrinsic transitions did not occur in the measurement temperature range, and the Seebeck coefficientincreased as the doping level increased. The power factor exhibited a positive temperature dependence, andCu3Sb0.86Ge0.08In0.06Se4 exhibited the highest value of 0.89 mWm–1K–2 at 623 K. As the temperature increased,the thermal conductivity tended to decrease because of the decreased lattice thermal conductivity and slightlyincreased electronic thermal conductivity. All the samples exhibited minimum thermal conductivities of 0.94–1.11 Wm–1K–1 at 523 K. At high temperatures, the double doping of Ge and In improved the thermoelectricperformance; thus, the dimensionless figure of merit obtained at 623 K for Cu3Sb0.86Ge0.08In0.06Se4, was 0.47.
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      Cu3Sb1–x–yGexInySe4 (0.02 ≤ x ≤ 0.12; 0.04 ≤ y ≤ 0.08) permingeatite compounds doped with Ge andIn were prepared using solid-state synthesis. The phases and microstructures were analyzed, and the chargetransport and thermoelectric properti...

      Cu3Sb1–x–yGexInySe4 (0.02 ≤ x ≤ 0.12; 0.04 ≤ y ≤ 0.08) permingeatite compounds doped with Ge andIn were prepared using solid-state synthesis. The phases and microstructures were analyzed, and the chargetransport and thermoelectric properties were evaluated according to the Ge and In doping content. Most ofthe samples contained a single phase of permingeatite with a tetragonal structure; however, secondary phases(Cu0.875InSe2, In2Se3, and InSb) were detected in the samples with x = 0.12 and y = 0.08. Both the a-axis andc-axis lattice constants of permingeatite were increased by Ge and In doping, with a = 0.5651–0.5655 nm andc = 1.1249–1.1255 nm, but the change in lattice constant due to the change in doping amount wasinsignificant. The melting point of the sample double-doped with Ge and In was determined to be 736 K, whichwas lower than the melting point (741 K) of pure Cu3SbSe4. This lowering of the melting point was attributedto the formation of a solid solution. The electrical conductivity exhibited degenerate semiconductor behavior,decreasing with increasing temperature. As the Ge and In doping content increased, the carrier concentrationand electrical conductivity increased; however, when x ≥ 0.12, the electrical conductivity did not increasefurther. The Seebeck coefficient exhibited positive values and p-type conduction characteristics. In addition,intrinsic transitions did not occur in the measurement temperature range, and the Seebeck coefficientincreased as the doping level increased. The power factor exhibited a positive temperature dependence, andCu3Sb0.86Ge0.08In0.06Se4 exhibited the highest value of 0.89 mWm–1K–2 at 623 K. As the temperature increased,the thermal conductivity tended to decrease because of the decreased lattice thermal conductivity and slightlyincreased electronic thermal conductivity. All the samples exhibited minimum thermal conductivities of 0.94–1.11 Wm–1K–1 at 523 K. At high temperatures, the double doping of Ge and In improved the thermoelectricperformance; thus, the dimensionless figure of merit obtained at 623 K for Cu3Sb0.86Ge0.08In0.06Se4, was 0.47.

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      참고문헌 (Reference)

      1 F. DiSalvo, 285 : 703-, 1999

      2 D. Li, 15 : 7166-, 2013

      3 G. Snyder, 7 : 105-, 2008

      4 X. Shi, 61 : 1-, 2016

      5 G. Tan, 116 : 12123-, 2016

      6 T. Zhu, 29 : 1605884-, 2017

      7 H. Zhu, 9 : 2497-, 2018

      8 O. R. Fitriani, 64 : 635-, 2016

      9 L. D. Zhao, 508 : 373-, 2014

      10 E. J. Skoug, 98 : 261911-, 2011

      1 F. DiSalvo, 285 : 703-, 1999

      2 D. Li, 15 : 7166-, 2013

      3 G. Snyder, 7 : 105-, 2008

      4 X. Shi, 61 : 1-, 2016

      5 G. Tan, 116 : 12123-, 2016

      6 T. Zhu, 29 : 1605884-, 2017

      7 H. Zhu, 9 : 2497-, 2018

      8 O. R. Fitriani, 64 : 635-, 2016

      9 L. D. Zhao, 508 : 373-, 2014

      10 E. J. Skoug, 98 : 261911-, 2011

      11 K. Tyagi, 105 : 261902-, 2014

      12 M. Rui, 6 : 13-, 2018

      13 C. Yang, 44 : 295404-, 2011

      14 H. Chen, 15 : 6648-, 2013

      15 D. Zhao, 10 : 1524-, 2017

      16 E. Skoug, 41 : 1232-, 2012

      17 J. Ning, 7 : 1043-, 2017

      18 D. Li, 12 : 3886-, 2019

      19 Y. Wu, 17 : 285-, 2015

      20 A. Kumar, 1942 : 14055-, 2018

      21 E. J. Skoug, 3 : 602-, 2011

      22 B. Wang, 124 : 10336-, 2020

      23 Y. Liu, 5 : 2592-, 2017

      24 L. Bell, 321 : 1457-, 2008

      25 L. Zhao, 872 : 159659-, 2021

      26 H. S. Kim, 3 : 041506-, 2015

      27 R. D. Shannon, 32 : 751-, 1976

      28 C. Yang, 44 : 295404-, 2011

      29 C. H. Chang, 186 : 227-, 2017

      30 D. Zhang, 98 : 150-, 2016

      31 V. B. Ghanwat, 4 : 1-, 2016

      32 G. E. Lee, 14 : 1116-, 2021

      33 Y. Li, 5 : 31399-, 2015

      34 G. E. Lee, "Thermoelectric properties of Cu3Sb(S/Se)4 and Cu3Sb(S/Se)3 prepared by solid-state synthesis" Korea National University of Transportation 2021

      35 김호정 ; 김일호, "Solid-State Synthesis and Thermoelectric Performance of Cu3Sb1-yBIII ySe4 (BIII = Al, In) Permingeatites" 대한금속·재료학회 61 (61): 269-276, 2023

      36 피지희 ; 이고은 ; 김일호, "Effects of Ge Doping on the Charge Transport and Thermoelectric Properties of Permingeatites Cu3Sb1−yGeySe4" 대한금속·재료학회 59 (59): 422-429, 2021

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