4.8 Article

Synthesis and Transport Properties of the Family of Zintl Phases Ca3RESb3 (RE = La-Nd, Sm, Gd-Tm, Lu): Exploring the Roles of Crystallographic Disorder and Core 4f Electrons for Enhancing Thermoelectric Performance

期刊

CHEMISTRY OF MATERIALS
卷 33, 期 23, 页码 9382-9392

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AMER CHEMICAL SOC
DOI: 10.1021/acs.chemmater.1c03300

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  1. US Department of Energy [DE-SC0008885]
  2. U.S. Department of Energy (DOE) [DE-SC0008885] Funding Source: U.S. Department of Energy (DOE)

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Zintl phases with complex crystal structures have been synthesized in the form of Ca4-xRExSb3, where Ca and RE atoms exhibit disorder and enhance phonon scattering. Incorporation of rare-earth metals leads to narrow bandgaps and semiconductor behavior with dominant hole charge carriers.
Zintl phases with complex crystal structures have been studied as promising candidate materials for thermoelectric (TE) applications. Here, we report the syntheses of the family of rare-earth metal Zintl phases with the general formula Ca4-xRExSb3 (x approximate to 1; RE = La-Nd, Sm, Gd-Tm, Lu). The structural elucidation is based on refinements of single-crystal X-ray diffraction data for 12 unique chemical compositions. The cubic structure is confirmed as belonging to the anti-Th3P4 structure type (space group I (4) over bar 3d, no. 220, Z = 4), where the Ca and RE atoms share the same atomic site with ca. 75 and 25% occupancies, respectively. Such crystallographic disordering of divalent Ca and trivalent RE atoms in the structure provides a pathway to intricate bonding. The latter, together with the presence of heavy elements such as Sb and the lanthanides, are expected to enhance the scattering probability of phonons, thereby leading to low thermal conductivity kappa comparable to that of the ordered RE4Sb3. The drive of the hypothetical parent compound Ca4Sb3 to be stabilized by alloying with rare-earth metals can be understood following the Zintl-Klemm concept, as the resultant formula may be rationalized as (Ca2+)(3)RE3+(Sb3-)(3), indicating the realization of closed-shell electronic configurations for all elements. This notion is confirmed by electronic structure calculations, which reveal narrow bandgaps E-g = 0.77 and 0.53 eV for Ca3LaSb3 and Ca3LuSb3, respectively. In addition, the incorporation of RE atoms into the structure drives the phase into a state of a degenerate semiconductor with dominant hole charge carriers.

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