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Research Article | Open Access

Understanding secondary phase inclusion and composition variations in the microstructure design of n-type Bi2Te3 alloys via selective dissolution of KCl

Gwang Min Parka,bSeunghyeok Leeb,cJun-Yun KangdSeung-Hyub BaekbHeesuk KimeJin-Sang KimfSeong Keun Kima,b()
KU-KIST Graduate School of Converging Science and Technology, Korea University, Seoul 02841, Republic of Korea
Electronic Materials Research Center, Korea Institute of Science and Technology, Seoul 02792, Republic of Korea
Department of Materials Science and Chemical Engineering, Hanyang University, Ansan 15588, Republic of Korea
Ferrous Alloy Department, Korea Institute of Materials Science, Changwon 51508, Republic of Korea
Soft Hybrid Materials Research Center, Korea Institute of Science and Technology, Seoul 02792, Republic of Korea
Institute of Advanced Composite Materials, Korea Institute of Science and Technology, Wanju 55324, Republic of Korea
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Abstract

This study investigated the effects of KCl treatment on microstructure and thermoelectric properties of n-type Bi2Te2.7Se0.3 (BTS) thermoelectric materials. The innovative KCl treatment was originally intended to introduce nanopores through selective dissolution of KCl from a mixture of thermoelectric materials and KCl. However, it unexpectedly induced substantial variations in material composition and microstructure during the subsequent spark plasma sintering (SPS) process. Hydroxyl groups adsorbed on the powder surface during the dissolution resulted in the emergence of a Bi2TeO5 secondary phase within the BTS matrix after the SPS process at 450 ℃. The concentration of Bi2TeO5 increased with an increase in the KCl content. Furthermore, a remarkable grain growth occurred at low KCl concentrations, likely due to the liquid-phase formation in a Te-rich composition during SPS. However, excessive Bi2TeO5 at higher KCl concentrations hindered grain growth. These variations in the microstructure had complex effects on electrical properties: The TeBi antisite defects increased the electron concentration, and Bi2TeO5 reduced electron mobility. Additionally, the lattice thermal conductivity decreased due to the presence of Bi2TeO5, from 0.8 W∙m−1∙K−1 at 298 K for the pristine BTS to 0.6 W∙m−1∙K−1 at 298 K for BTS treated with 1 wt% KCl. These insights allowed precise adjustments of the electrical and thermal conductivities, leading to an enhancement in the maximum value of figure-of-merit (ZT) from 0.76 to 0.96 through the selective dissolution of KCl approach. We believe that our observations potentially enable advances in thermoelectric materials by engineering microstructures.

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References

[1]
DiSalvo F. Thermoelectric cooling and power generation. Science 1999, 285: 703706.
[2]
Poudel B, Hao Q, Ma Y, et al. High-thermoelectric performance of nanostructured bismuth antimony telluride bulk alloys. Science 2008, 320: 634638.
[3]
Snyder GJ, Toberer ES. Complex thermoelectric materials. Nat Mater 2008, 7: 105114.
[4]
Liu WS, Yan X, Chen G, et al. Recent advances in thermoelectric nanocomposites. Nano Energy 2012, 1: 4256.
[5]
Vineis CJ, Shakouri A, Majumdar A, et al. Nanostructured thermoelectrics: Big efficiency gains from small features. Adv Mater 2010, 22: 39703980.
[6]
Yang L, Chen ZG, Dargusch MS, et al. High performance thermoelectric materials: Progress and their applications. Adv Energy Mater 2018, 8: 1701797.
[7]
Pourkiaei SM, Ahmadi MH, Sadeghzadeh M, et al. Thermoelectric cooler and thermoelectric generator devices: A review of present and potential applications, modeling and materials. Energy 2019, 186: 115849.
[8]
Lan YC, Minnich AJ, Chen G, et al. Enhancement of thermoelectric figure-of-merit by a bulk nanostructuring approach. Adv Funct Mater 2010, 20: 357376.
[9]
Xie WJ, Tang XF, Yan YG, et al. Unique nanostructures and enhanced thermoelectric performance of melt-spun BiSbTe alloys. Appl Phys Lett 2009, 94: 102111.
[10]
Kanatzidis MG. Nanostructured thermoelectrics: The new paradigm? Chem Mater 2010, 22: 648659.
[11]
Chen C, Wang BH, Chen C, et al. Greatly enhanced mechanical properties of thermoelectric SnSe through microstructure engineering. J Adv Ceram 2023, 12: 10811089.
[12]
Zhang YC, Stucky GD. Heterostructured approaches to efficient thermoelectric materials. Chem Mater 2014, 26: 837848.
[13]
Jung SJ, Park SY, Kim BK, et al. Hardening of Bi–Te based alloys by dispersing B4C nanoparticles. Acta Mater 2015, 97: 6874.
[14]
Ginting D, Lin CC, Rathnam L, et al. High thermoelectric performance due to nano-inclusions and randomly distributed interface potentials in n-type (PbTe0.93−xSe0.07Clx)0.93(PbS)0.07 composites. J Mater Chem A 2017, 5: 1353513543.
[15]
Kim KC, Lim SS, Lee SH, et al. Precision interface engineering of an atomic layer in bulk Bi2Te3 alloys for high thermoelectric performance. ACS Nano 2019, 13: 71467154.
[16]
Li SK, Liu YD, Liu FS, et al. Effective atomic interface engineering in Bi2Te2.7Se0.3 thermoelectric material by atomic-layer-deposition approach. Nano Energy 2018, 49: 257266.
[17]
Lim SS, Kim KC, Jeon H, et al. Enhanced thermal stability of Bi2Te3-based alloys via interface engineering with atomic layer deposition. J Eur Ceram Soc 2020, 40: 35923599.
[18]
Lee S, Jung SJ, Park GM, et al. Grain boundary engineering strategy for simultaneously reducing the electron concentration and lattice thermal conductivity in n-type Bi2Te2.7Se0.3-based thermoelectric materials. J Eur Ceram Soc 2023, 43: 33763382.
[19]
Zhuang HL, Hu HH, Pei J, et al. High ZT in p-type thermoelectric (Bi,Sb)2Te3 with built-in nanopores. Energy Environ Sci 2022, 15: 20392048.
[20]
Wang Y, Liu WD, Gao H, et al. High porosity in nanostructured n-type Bi2Te3 obtaining ultralow lattice thermal conductivity. ACS Appl Mater Inter 2019, 11: 3123731244.
[21]
Xu B, Feng TL, Agne MT, et al. Highly porous thermoelectric nanocomposites with low thermal conductivity and high figure of merit from large-scale solution-synthesized Bi2Te2.5Se0.5 hollow nanostructures. Angew Chem Int Ed 2017, 56: 35463551.
[22]
Zheng ZH, Shi XL, Ao DW, et al. Harvesting waste heat with flexible Bi2Te3 thermoelectric thin film. Nat Sustain 2023, 6: 180191.
[23]
Wei M, Shi XL, Zheng ZH, et al. Directional thermal diffusion realizing inorganic Sb2Te3/Te hybrid thin films with high thermoelectric performance and flexibility. Adv Funct Mater 2022, 32: 2207903.
[24]
Jabar B, Mansoor A, Chen YX, et al. High thermoelectric performance of BixSb2−xTe3 alloy achieved via structural manipulation under optimized heat treatment. Chem Eng J 2022, 435: 135062.
[25]
Ao DW, Liu WD, Zheng ZH, et al. Assembly-free fabrication of high-performance flexible inorganic thin-film thermoelectric device prepared by a thermal diffusion. Adv Energy Mater 2022, 12: 2202731.
[26]
Ao DW, Liu WD, Chen YX, et al. Novel thermal diffusion temperature engineering leading to high thermoelectric performance in Bi2Te3-based flexible thin-films. Adv Sci 2022, 9: 2103547.
[27]
Lee S, Jung SJ, Park GM, et al. Selective dissolution-derived nanoporous design of impurity-free Bi2Te3 alloys with high thermoelectric performance. Small 2023, 19: 2205202.
[28]
Yu HJ, Jeong M, Lim YS, et al. Effects of Cu addition on band gap energy, density of state effective mass and charge transport properties in Bi2Te3 composites. RSC Adv 2014, 4: 4381143814.
[29]
Chen S, Cai KF, Li FY, et al. The effect of Cu addition on the system stability and thermoelectric properties of Bi2Te3. J Electron Mater 2014, 43: 19661971.
[30]
Peranio N, Winkler M, Dürrschnabel M, et al. Assessing antisite defect and impurity concentrations in Bi2Te3 based thin films by high-accuracy chemical analysis. Adv Funct Mater 2013, 23: 49694976.
[31]
Cho S, Kim Y, DiVenere A, et al. Antisite defects of Bi2Te3 thin films. Appl Phys Lett 1999, 75: 14011403.
[32]
Sun YX, Qin HX, Wang W, et al. Simultaneous regulation of electrical and thermal transport properties of n-type Bi2Te3 via adding excessive Te followed by Se doping. ACS Appl Energy Mater 2021, 4: 49864992.
[33]
Jung SJ, Lim SS, Lee BH, et al. Study of the relationship between process parameters, volatility of Te, and physical properties in n-type Bi2Te3-based alloys for the reproducible fabrication of high-performance thermoelectric materials. J Alloys Compd 2023, 937: 168476.
[34]
Humphry-Baker SA, Schuh CA. Spontaneous solid-state foaming of nanocrystalline thermoelectric compounds at elevated temperatures. Nano Energy 2017, 36: 223232.
[35]
Fleurial JP, Gailliard L, Triboulet R, et al. Thermal properties of high quality single crystals of bismuth telluride—Part I: Experimental characterization. J Phys Chem Solids 1988, 49: 12371247.
[36]
Zhang M, Liu W, Zhang C, et al. Identifying the manipulation of individual atomic-scale defects for boosting thermoelectric performances in artificially controlled Bi2Te3 films. ACS Nano 2021, 15: 57065714.
[37]
Winter MR, Clarke DR. Oxide materials with low thermal conductivity. J Am Ceram Soc 2007, 90: 533540.
[38]
Liu S, Liu F, Zhu XQ, et al. Lemental ratio controlled semiconductor type of bismuth telluride alloy thin films. Rare Met Mater Eng 2015, 44: 30413044.
Journal of Advanced Ceramics
Pages 2360-2370
Cite this article:
Park GM, Lee S, Kang J-Y, et al. Understanding secondary phase inclusion and composition variations in the microstructure design of n-type Bi2Te3 alloys via selective dissolution of KCl. Journal of Advanced Ceramics, 2023, 12(12): 2360-2370. https://doi.org/10.26599/JAC.2023.9220825
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