Unlocking the thermoelectric potential of the Ca<sub>14</sub>AlSb<sub>11</sub> structure type.
basic_science · Level V
Where this comes from
- Record sourced from PubMed, PMID 36070392.
- Also identified by DOI 10.1126/sciadv.abq3780 and PMC identifier 9451163.
- Licence recorded as CC BY.
- The licence permits redistribution, so the abstract is shown in full and the full text is available from the publisher.
Abstract
Yb<sub>14</sub>MnSb<sub>11</sub> and Yb<sub>14</sub>MgSb<sub>11</sub> are among the best p-type high-temperature (>1200 K) thermoelectric materials, yet other compounds of this Ca<sub>14</sub>AlSb<sub>11</sub> structure type have not matched their stability and efficiency. First-principles computations show that the features in the electronic structures that have been identified to lead to high thermoelectric performances are present in Yb<sub>14</sub>ZnSb<sub>11</sub>, which has been presumed to be a poor thermoelectric material. We show that the previously reported low power factor of Yb<sub>14</sub>ZnSb<sub>11</sub> is not intrinsic and is due to the presence of a Yb<sub>9</sub>Zn<sub>4+<i>x</i></sub>Sb<sub>9</sub> impurity uniquely present in the Zn system. Phase-pure Yb<sub>14</sub>ZnSb<sub>11</sub> synthesized through a route avoiding the impurity formation reveals its exceptional high-temperature thermoelectric properties, reaching a peak <i>zT</i> of 1.2 at 1175 K. Beyond Yb<sub>14</sub>ZnSb<sub>11</sub>, the favorable band structure features for thermoelectric performance are universal among the Ca<sub>14</sub>AlSb<sub>11</sub> structure type, opening the possibility for high-performance thermoelectric materials.