Characterization of Bipolar Transport in Hf(Te1-xSex)2 Thermoelectric Alloys
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Hwang, Seong-Mee
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Univ Seoul, Dept Mat Sci & Engn, 163 Seoulsiripdae ro, Seoul 02504, South KoreaUniv Seoul, Dept Mat Sci & Engn, 163 Seoulsiripdae ro, Seoul 02504, South Korea
Hwang, Seong-Mee
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Kim, Sang-il
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Univ Seoul, Dept Mat Sci & Engn, 163 Seoulsiripdae ro, Seoul 02504, South KoreaUniv Seoul, Dept Mat Sci & Engn, 163 Seoulsiripdae ro, Seoul 02504, South Korea
Kim, Sang-il
[1
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Kim, Jeong-Yeon
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Univ Seoul, Dept Mat Sci & Engn, 163 Seoulsiripdae ro, Seoul 02504, South KoreaUniv Seoul, Dept Mat Sci & Engn, 163 Seoulsiripdae ro, Seoul 02504, South Korea
Kim, Jeong-Yeon
[1
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Heo, Minsu
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Univ Seoul, Dept Mat Sci & Engn, 163 Seoulsiripdae ro, Seoul 02504, South KoreaUniv Seoul, Dept Mat Sci & Engn, 163 Seoulsiripdae ro, Seoul 02504, South Korea
Heo, Minsu
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Kim, Hyun-Sik
[1
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[1] Univ Seoul, Dept Mat Sci & Engn, 163 Seoulsiripdae ro, Seoul 02504, South Korea
Control of bipolar conduction is essential to improve the high-temperature thermoelectric performance of materials for power generation applications. Recently, Hf(Te1-xSex)(2) alloys have gained much attention due to their potential use in thermoelectric power generation. Increasing the Se alloying content significantly increases the band gap while decreasing its carrier concentration. These two factors affect bipolar conduction substantially. In addition, the weighted mobility ratio is estimated from the experimental electronic transport properties of Hf(Te1-xSex)(2) alloys (x = 0.0, 0.025, 0.25, 0.5, 1.0) by using the Two-Band model. From the bipolar thermal conductivity also calculated using the Two-Band model, we find that it peaks near x = 0.5. The initial bipolar conductivity increase of x < 0.5 is mostly due to the decrease in the weighted mobility ratio and carrier concentration with increasing x. For x > 0.5, the drop in the bipolar conductivity can be understood with significant band gap enlargement.
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Tamkang Univ, Dept Phys, New Taipei 25137, TaiwanTamkang Univ, Dept Phys, New Taipei 25137, Taiwan
Pandian, Mannu
Krishnaprasanth, Alageshwaramoorthy
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Kongunadu Arts & Sci Coll, Dept Phys, Coimbatore 641029, Tamil Nadu, IndiaTamkang Univ, Dept Phys, New Taipei 25137, Taiwan
Krishnaprasanth, Alageshwaramoorthy
Palanisamy, Matheswaran
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Kongunadu Arts & Sci Coll, Dept Phys, Coimbatore 641029, Tamil Nadu, IndiaTamkang Univ, Dept Phys, New Taipei 25137, Taiwan
Palanisamy, Matheswaran
Bangaru, Gokul
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Kongunadu Arts & Sci Coll, Dept Phys, Coimbatore 641029, Tamil Nadu, IndiaTamkang Univ, Dept Phys, New Taipei 25137, Taiwan
Bangaru, Gokul
Meena, Ramcharan
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Interuniv Accelerator Ctr, Mat Sci Div, New Delhi 110067, IndiaTamkang Univ, Dept Phys, New Taipei 25137, Taiwan
Meena, Ramcharan
Dong, Chung-Li
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Tamkang Univ, Dept Phys, New Taipei 25137, TaiwanTamkang Univ, Dept Phys, New Taipei 25137, Taiwan
Dong, Chung-Li
Kandasami, Asokan
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Univ Petr & Energy Studies UPES Dehradun, Dept Phys & Ctr Interdisciplinary Res, Dehra Dun 248007, Uttarakhand, IndiaTamkang Univ, Dept Phys, New Taipei 25137, Taiwan