Experimental and computational phase boundary mapping of Co4Sn6Te6

Caitlin M. Crawford, Brenden R. Ortiz, Prashun Gorai, Vladan Stevanovic, Eric S. Toberer

Research output: Contribution to journalArticlepeer-review

24 Scopus citations

Abstract

Binary Co4Sb12 skutterudite (also known as CoSb3) has been extensively studied; however, its mixed-anion counterparts remain largely unexplored in terms of their phase stability and thermoelectric properties. In the search for complex anionic analogs of the binary skutterudite, we begin by investigating the Co4Sb12-Co4Sn6Te6 pseudo-binary phase diagram. We observe no quaternary skutterudite phases and as such, focus our investigations on the ternary Co4Sn6Te6via experimental phase boundary mapping, transport measurements, and first-principles calculations. Phase boundary mapping using traditional bulk syntheses reveals that the Co4Sn6Te6 exhibits electronic properties ranging from a degenerate p-type behavior to an intrinsic behavior. Under Sn-rich conditions, Hall measurements indicate degenerate p-type carrier concentrations and high hole mobility. The acceptor defect SnTe, and donor defects TeSn and Coi are the predominant defects and rationally correspond to regions of high Sn, Te, and Co, respectively. Consideration of the defect energetics indicates that p-type extrinsic doping is plausible; however, SnTe is likely a killer defect that limits n-type dopability. We find that the hole carrier concentration in Co4Sn6Te6 can be further optimized by extrinsic p-type doping under Sn-rich growth conditions.

Original languageEnglish
Pages (from-to)24175-24185
Number of pages11
JournalJournal of Materials Chemistry A
Volume6
Issue number47
DOIs
StatePublished - 2018
Externally publishedYes

Funding

This work was performed at the California Institute of Technology/Jet Propulsion Laboratory under contract with the National Aeronautics and Space Administration. This work was supported by the NASA Science Mission Directorate's Radioisotope Power Systems Thermoelectric Technology Development Project under Grant/Contract/Agreement No. NNX16AT18H. We also acknowledge support from the National Science Foundation (NSF) (DMR grants 1729594 and 1555340). The research was performed using computational resources sponsored by the Department of Energy's Office of Energy Efficiency and Renewable Energy located at the NREL. Use of the Advanced Photon Source at Argonne National Laboratory was supported by the U. S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357.

FundersFunder number
Office of Basic Energy Sciences
U. S. Department of Energy
National Science Foundation1729487
U.S. Department of Energy
Division of Materials Research1729594, 1555340
National Aeronautics and Space Administration
Office of Science
Office of Energy Efficiency and Renewable Energy
National Renewable Energy Laboratory

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