Abstract:Temperature. -The thermoelectric and structural properties of the title compound are studied below 300 K for samples with x = 0.0, 0.1, 0.2, 0.3, and 0.4. The electrical resistivity is found to increase with increasing Cd content x and to be lower below the β→α phase transition. The Seebeck coefficient also increases with x. The β→α phase transition temperature is almost independent of the Cd content. Although the power factor at 300 K has a maximum of 6·10 -6 Wcm -1 K -2 at x = 0.2, the thermoelectric perform… Show more
“…The lattice parameters ( a ‐ c ) of the double‐doping (SnCd) system in β‐Zn 4 Sb 3 increase monotonically as the Cd content increased. The larger values of lattice parameters ( a ‐ c ) of the samples are the fact that the introduction of Cd and Sn atoms randomly occupy special occupation sites of Zn and reduce Zn atom in the host, resulting in diminishing the number of the total cation in per unit cell . The similar observation is found in previous works…”
Section: Resultssupporting
confidence: 86%
“…The change of lattice parameters ( a ‐ c ) is summarized in Table . Compared with un‐doping β‐Zn 4 Sb 3, the increase of lattice parameters ( a ‐ c ) is in accordance with the different atom radius of the dopants (CdSn), which the atom radius of Cd (1.71 Å) and Sn (1.72 Å) are relatively larger than that of Zn (1.53 Å). The lattice parameters ( a ‐ c ) of the double‐doping (SnCd) system in β‐Zn 4 Sb 3 increase monotonically as the Cd content increased.…”
In this work, the effect of Cd and Sn atoms partly substitution for Zn on among crystal growth, thermal stability, mechanical, and electrical transport property in β‐Zn4Sb3 is reported. In a series of samples prepared from the atomic ratios of Zn:Sb:Cd:Sn = 4.4:3:x:3 (x = 0.2, 0.4, 0.6, and 0.8). Carrier concentration of all samples varies from 4.52 × 1019 to 6.42 × 1019 cm−3 as carrier mobility changes from 58.27 to 67.93 cm2 V−1 s−1 at room temperature. As a result, electrical transport properties of the samples are optimized by CdSn co‐doped. The experimental density of all the samples varies from 6.26 × 103 to 6.34 × 103 kg m−3 consistent with the theoretical value. The weight loss and melting point of the sample are determined to discuss thermal stability in the heating process in air, indicating that the single crystals β‐Zn4Sb3 possess an excellent thermal stability and it is practical importance in the TE application at high temperature. Consequently, the maximal power factor of 1.70 × 10−3 W m−1 K−2 is achieved at 540 K for the sample with initial Cd content x = 0.2, which is enhanced by 40% compared with the single‐doping system in β‐Zn4Sb3.
“…The lattice parameters ( a ‐ c ) of the double‐doping (SnCd) system in β‐Zn 4 Sb 3 increase monotonically as the Cd content increased. The larger values of lattice parameters ( a ‐ c ) of the samples are the fact that the introduction of Cd and Sn atoms randomly occupy special occupation sites of Zn and reduce Zn atom in the host, resulting in diminishing the number of the total cation in per unit cell . The similar observation is found in previous works…”
Section: Resultssupporting
confidence: 86%
“…The change of lattice parameters ( a ‐ c ) is summarized in Table . Compared with un‐doping β‐Zn 4 Sb 3, the increase of lattice parameters ( a ‐ c ) is in accordance with the different atom radius of the dopants (CdSn), which the atom radius of Cd (1.71 Å) and Sn (1.72 Å) are relatively larger than that of Zn (1.53 Å). The lattice parameters ( a ‐ c ) of the double‐doping (SnCd) system in β‐Zn 4 Sb 3 increase monotonically as the Cd content increased.…”
In this work, the effect of Cd and Sn atoms partly substitution for Zn on among crystal growth, thermal stability, mechanical, and electrical transport property in β‐Zn4Sb3 is reported. In a series of samples prepared from the atomic ratios of Zn:Sb:Cd:Sn = 4.4:3:x:3 (x = 0.2, 0.4, 0.6, and 0.8). Carrier concentration of all samples varies from 4.52 × 1019 to 6.42 × 1019 cm−3 as carrier mobility changes from 58.27 to 67.93 cm2 V−1 s−1 at room temperature. As a result, electrical transport properties of the samples are optimized by CdSn co‐doped. The experimental density of all the samples varies from 6.26 × 103 to 6.34 × 103 kg m−3 consistent with the theoretical value. The weight loss and melting point of the sample are determined to discuss thermal stability in the heating process in air, indicating that the single crystals β‐Zn4Sb3 possess an excellent thermal stability and it is practical importance in the TE application at high temperature. Consequently, the maximal power factor of 1.70 × 10−3 W m−1 K−2 is achieved at 540 K for the sample with initial Cd content x = 0.2, which is enhanced by 40% compared with the single‐doping system in β‐Zn4Sb3.
“…β-Zn 4 Sb 3 is one of the promising thermoelectric materials in the temperature range of 300-700 K due to its low thermal conductivity and good electrical properties [1][2][3] . Recently, some attempts were reported to optimize the thermoelectric performance of β-Zn 4 Sb 3 by substituting Zn with In [4] , Cd [5] , Mg [6] , and Pb [7] or Sb with Te [8] , which brought out the lattice distortion and then decreased the lattice thermal conductivity and increased Seebeck coefficient. However, more and more studies show that the doping is inefficient in improving the thermoelectric performance ofβ-Zn 4 Sb 3 materials.…”
A series of SiO 2 /β-Zn 4 Sb 3 core-shell composite particles with 3, 6, 9, and 12 nm of SiO 2 shell in thickness were prepared by coatingβ-Zn 4 Sb 3 microparticles with SiO 2 nanoparticles formed by hydrolyzing the tetraethoxysilane in alcohol-alkali-water solution. SiO 2 /β-Zn 4 Sb 3 nanocomposite thermoelectric materials were fabricated with these core-shell composite particles by spark plasma sintering (SPS) method. Microstructure, phase composition, and thermoelectric properties of SiO 2 /β-Zn 4 Sb 3 nanocomposite thermoelectric materials were systemically investigated. The results show thatβ-Zn 4 Sb 3 microparticles are uniformly coated by SiO 2 nanoparticles, and no any phase transformation reaction takes place during SPS process. The electrical and thermal conductivity gradually decreases, and the Seebeck coefficient increases compared to that ofβ-Zn 4 Sb 3 bulk material, but the increment of Seebeck coefficient in high temperature range remarkably increases. The thermal conductivity of SiO 2 /β-Zn 4 Sb 3 nanocomposite material with 12 nm of SiO 2 shell is the lowest and only 0.56 W·m -1 ·K -1 at 460 K. As a result, the ZT value of the SiO 2 /β-Zn 4 Sb 3 nanocomposite material reaches 0.87 at 700 K and increases by 30%.
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