<p>Ternary compounds of the Cu–X–Q system (where X = Fe, Sb, Sn and Q = S, Se), such as Cu<sub>5</sub>FeS<sub>4</sub>, Cu<sub>3</sub>SbS<sub>4</sub>, and Cu<sub>2</sub>SnSe<sub>3</sub>, have garnered considerable attention for their potential applications in electronics, optics, and energy technologies. These compounds are noted for their low thermal conductivity and narrow band gaps, making them promising candidates for thermoelectric materials. However, detailed experimental investigations into the phase transitions and thermoelectric properties of synthetic hakite, particularly with Ni substitution, have been limited. This study focused on synthesizing Ni-substituted hakite (Ni<sub>x</sub>Cu<sub>12−x</sub>Sb<sub>4</sub>Se<sub>13</sub>; x = 0.5–2) through mechanical alloying and hot pressing techniques, while also exploring the phase transitions and thermoelectric characteristics as a function of Ni content. Despite the charge compensation effect of Ni, a pure hakite phase could not be achieved. Instead, the resultant phases comprised mixtures of secondary phases including bytizite, pribramite, and permingeatite, or their composites. This indicates that the introduction of Ni into the system did not promote the formation of a single-phase hakite but rather stabilized a multi-phase system. The introduction of Ni resulted in a decrease in electrical conductivity across all specimens. Notably, the materials exhibited non-degenerate semiconductor behavior. The measured Seebeck coefficients were significantly high and positive, confirming p-type behavior. However, these coefficients decreased with increasing temperature. The thermal conductivity of the materials displayed minimal temperature dependence, consistently remaining below 0.65 Wm<sup>−1</sup>&#xa0;K<sup>−1</sup>. This low thermal conductivity is advantageous for thermoelectric efficiency, as it minimizes heat loss while maintaining charge transport. For the composition Ni<sub>0.5</sub>Cu<sub>11.5</sub>Sb<sub>4</sub>Se<sub>13</sub>, we achieved a maximum power factor of 0.09 mWm<sup>−1</sup>&#xa0;K<sup>−2</sup> and a peak dimensionless figure of merit (ZT) of 0.18 at 623&#xa0;K.</p> Graphical Abstract <p></p>

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Phase Transition and Thermoelectric Performance of NixCu12−xSb4Se13

  • Sang Jun Park,
  • Il-Ho Kim

摘要

Ternary compounds of the Cu–X–Q system (where X = Fe, Sb, Sn and Q = S, Se), such as Cu5FeS4, Cu3SbS4, and Cu2SnSe3, have garnered considerable attention for their potential applications in electronics, optics, and energy technologies. These compounds are noted for their low thermal conductivity and narrow band gaps, making them promising candidates for thermoelectric materials. However, detailed experimental investigations into the phase transitions and thermoelectric properties of synthetic hakite, particularly with Ni substitution, have been limited. This study focused on synthesizing Ni-substituted hakite (NixCu12−xSb4Se13; x = 0.5–2) through mechanical alloying and hot pressing techniques, while also exploring the phase transitions and thermoelectric characteristics as a function of Ni content. Despite the charge compensation effect of Ni, a pure hakite phase could not be achieved. Instead, the resultant phases comprised mixtures of secondary phases including bytizite, pribramite, and permingeatite, or their composites. This indicates that the introduction of Ni into the system did not promote the formation of a single-phase hakite but rather stabilized a multi-phase system. The introduction of Ni resulted in a decrease in electrical conductivity across all specimens. Notably, the materials exhibited non-degenerate semiconductor behavior. The measured Seebeck coefficients were significantly high and positive, confirming p-type behavior. However, these coefficients decreased with increasing temperature. The thermal conductivity of the materials displayed minimal temperature dependence, consistently remaining below 0.65 Wm−1 K−1. This low thermal conductivity is advantageous for thermoelectric efficiency, as it minimizes heat loss while maintaining charge transport. For the composition Ni0.5Cu11.5Sb4Se13, we achieved a maximum power factor of 0.09 mWm−1 K−2 and a peak dimensionless figure of merit (ZT) of 0.18 at 623 K.

Graphical Abstract