scholarly journals Ultra-high Seebeck coefficient and low thermal conductivity of a centimeter-sized perovskite single crystal acquired by a modified fast growth method

2017 ◽  
Vol 5 (5) ◽  
pp. 1255-1260 ◽  
Author(s):  
Tao Ye ◽  
Xizu Wang ◽  
Xianqiang Li ◽  
Alex Qingyu Yan ◽  
Seeram Ramakrishna ◽  
...  
Keyword(s):  
Thermal Conductivity ◽  
Seebeck Coefficient ◽  
Single Crystal ◽  
Fast Growth ◽  
Inverse Temperature ◽  
Temperature Growth ◽  
Inorganic Hybrid ◽  
Low Thermal Conductivity ◽  
Growth Method ◽  
High Seebeck Coefficient

A centimeter-sized organic–inorganic hybrid lead-based perovskite CH3NH3PbI3(MAPbI3) single crystal was obtained by using a modified fast and inverse-temperature growth method.

Thin Film Thermoelectric Metal-Organic Framework with High Seebeck Coefficient and Low Thermal Conductivity

2015 ◽  
Vol 27 (22) ◽  
pp. 3453-3459 ◽  
Author(s):  
Kristopher J. Erickson ◽  
François Léonard ◽  
Vitalie Stavila ◽  
Michael E. Foster ◽  
Catalin D. Spataru ◽  
...  
Keyword(s):  
Thin Film ◽  
Thermal Conductivity ◽  
Seebeck Coefficient ◽  
Metal Organic Framework ◽  
Low Thermal Conductivity ◽  
Metal Organic ◽  
High Seebeck Coefficient ◽  
Organic Framework

scholarly journals High Seebeck Coefficient and Unusually Low Thermal Conductivity Near Ambient Temperatures in Layered Compound Yb2–xEuxCdSb2

2017 ◽  
Vol 30 (2) ◽  
pp. 484-493 ◽  
Author(s):  
Joya A. Cooley ◽  
Phichit Promkhan ◽  
Shruba Gangopadhyay ◽  
Davide Donadio ◽  
Warren E. Pickett ◽  
...  
Keyword(s):  
Thermal Conductivity ◽  
Seebeck Coefficient ◽  
Layered Compound ◽  
Low Thermal Conductivity ◽  
Ambient Temperatures ◽  
High Seebeck Coefficient

Observation of High Seebeck Coefficient and Low Thermal Conductivity in [SrO]-Intercalated CuSbSe2 Compound

2018 ◽  
Vol 30 (16) ◽  
pp. 5539-5543 ◽  
Author(s):  
Kejun Bu ◽  
Jian Huang ◽  
Mengjia Luo ◽  
Mengjia Guan ◽  
Chong Zheng ◽  
...  
Keyword(s):  
Thermal Conductivity ◽  
Seebeck Coefficient ◽  
Low Thermal Conductivity ◽  
High Seebeck Coefficient

scholarly journals SYNTHESIS OF Cu2ZnSnS4 BY MECHANICAL ALLOYING METHOD FOR THERMOELECTRIC APPLICATION

2019 ◽  
Vol 25 (3) ◽  
pp. 174 ◽  
Author(s):  
Long Duc Bui ◽  
Khanh Van Nguyen ◽  
Binh Ngoc Duong ◽  
Thang Hong Le ◽  
Bang Thi Le ◽  
...  
Keyword(s):  
Thermal Conductivity ◽  
Mechanical Alloying ◽  
Seebeck Coefficient ◽  
Particle Distribution ◽  
Title Page ◽  
Potential Candidate ◽  
Low Thermal Conductivity ◽  
Milling Duration ◽  
High Seebeck Coefficient ◽  
Thermoelectric Application

<div class="page" title="Page 1"><div class="layoutArea"><div class="column"><p><span>Quaternary chalcogenide Cu</span><span>2</span><span>ZnSnS</span><span>4 </span><span>is a potential candidate for thermoelectric (TE) application due to a number of advantages including containing only non-toxic and abundant elements, high Seebeck coefficient and low thermal conductivity. In this study, Cu</span><span>2</span><span>ZnSnS</span><span>4 </span><span>was synthesized using mechanical alloying method from Cu, Zn, Sn and S powders. In order to study the effect of milling duration on the formation of Cu</span><span>2</span><span>ZnSnS</span><span>4</span><span>, different milling duration of 2, 4, 12 and 16 h were carried out. As the results, Cu</span><span>2</span><span>ZnSnS</span><span>4 </span><span>wasstarted to form after milling for 12 h. The formation of Cu</span><span>2</span><span>ZnSnS</span><span>4 </span><span>was completed after 16 h of milling. In addition, Cu</span><span>2</span><span>ZnSnS</span><span>4 </span><span>nanoparticles were obtained after 16 h of milling with the particle distribution mostly in the range of 50 - 60 nm. </span></p></div></div></div>

Structure and Thermoelectric Properties of New Quaternary Tin and Lead Bismuth Selenides, K1+xM4-2xBi7+xSe15 (M = Sn, Pb) and K1+xSn5-xBi11+xSe22

2000 ◽  
Vol 626 ◽  
Author(s):  
Antje Mrotzek ◽  
Kyoung-Shin Choi ◽  
Duck-Young Chung ◽  
Melissa A. Lane ◽  
John R. Ireland ◽  
...  
Keyword(s):  
Thermal Conductivity ◽  
Single Crystal ◽  
Thermoelectric Properties ◽  
Three Dimensional ◽  
Structure Type ◽  
Narrow Gap ◽  
Low Thermal Conductivity ◽  
Seebeck Coefficients ◽  
Metal Atoms ◽  
Anionic Framework

ABSTRACTWe present the structure and thermoelectric properties of the new quaternary selenides K1+xM4–2xBi7+xSe15 (M = Sn, Pb) and K1-xSn5-xBi11+xSe22. The compounds K1+xM4-2xBi7+xSe15 (M= Sn, Pb) crystallize isostructural to A1+xPb4-2xSb7+xSe15 with A = K, Rb, while K1-xSn5-xBi11+xSe22 reveals a new structure type. In both structure types fragments of the Bi2Te3-type and the NaCl-type are connected to a three-dimensional anionic framework with K+ ions filled tunnels. The two structures vary by the size of the NaCl-type rods and are closely related to β-K2Bi8Se13 and K2.5Bi8.5Se14. The thermoelectric properties of K1+xM4-2xBi7+xSe15 (M = Sn, Pb) and K1-xSn5-xBi11+xSe22 were explored on single crystal and ingot samples. These compounds are narrow gap semiconductors and show n-type behavior with moderate Seebeck coefficients. They have very low thermal conductivity due to an extensive disorder of the metal atoms and possible “rattling” K+ ions.

Thermoelectric Properties of Semiconducting Intermetallic Compounds: FeGa3and RuGa3

2003 ◽  
Vol 793 ◽  
Author(s):  
Y. Amagai ◽  
A. Yamamoto ◽  
C. H. Lee ◽  
H. Takazawa ◽  
T. Noguchi ◽  
...  
Keyword(s):  
Thermal Conductivity ◽  
Electrical Resistivity ◽  
High Temperature ◽  
Seebeck Coefficient ◽  
Transport Properties ◽  
Figure Of Merit ◽  
Room Temperature ◽  
Thermoelectric Figure Of Merit ◽  
Thermoelectric Figure ◽  
High Seebeck Coefficient

ABSTRACTWe report transport properties of polycrystalline TMGa3(TM = Fe and Ru) compounds in the temperature range 313K<T<973K. These compounds exhibit semiconductorlike behavior with relatively high Seebeck coefficient, electrical resistivity, and Hall carrier concentrations at room temperature in the range of 1017- 1018cm−3. Seebeck coefficient measurements reveal that FeGa3isn-type material, while the Seebeck coefficient of RuGa3changes signs rapidly from large positive values to large negative values around 450K. The thermal conductivity of these compounds is estimated to be 3.5Wm−1K−1at room temperature and decreased to 2.5Wm−1K−1for FeGa3and 2.0Wm−1K−1for RuGa3at high temperature. The resulting thermoelectric figure of merit,ZT, at 945K for RuGa3reaches 0.18.

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