European Journal of Inorganic Chemistry · 2011 · 23 citations · 33 references
Natural SciencesMaterials SciencePhysicsCondensed Matter PhysicsMaterials ChemistrySolid State PhysicsAb Initio MethodsCluster ChemistryCrystal ChemistryElectronic Band StructureElectronic Structure Of SolidsThermoelectric MaterialsBand GapBand Gap EnergyBand Structure CalculationChalcogenide Host MaterialsChalcogenide SynthesisCubic LatticesFermi LevelThermoelectric Properties
Abstract BaCu 6– x STe 6 and BaCu 6– x Se 1– y Te 6+ y were synthesized from the elements at 663 K. These chalcogenides adopt a new structure type, cubic space group Pm $\bar {3}$ , with a = 6.9680(2) Å in the case of BaCu 5.93 SeTe 6 . Therein, the Cu atoms form cubic clusters, centered by Se atoms, where statistically 2.07 corners are unoccupied. All Te atoms are part of Te 2 2– dumbbells, leading to a charge‐balanced formula when x = 0: Ba 2+ (Cu + ) 6 Se 2– (Te 2 2– ) 3 . While Te atoms can be incorporated on the Se site, no evidence was found for the ability of Se atoms to replace Te in the Te 2 2– pairs. Band structure calculations on different BaCu 6 SeTe 6 models revealed a very small band gap at the Fermi level; all these chalcogenides with x > 0 should thus be p ‐doped semiconductors, which we experimentally confirmed for BaCu 5.7 Se 0.6 Te 6.4 .
33
A short history of<i>SHELX</i>
George M. Sheldrick · Acta Crystallographica Section A Foundations of Crystallography · 2007 · 87.4K citations · Full text
Issues and challenges facing rechargeable lithium batteries
J. M. Tarascon, Michel Armand · Nature · 2001 · 20.7K citations
OK Andersen · Physical review. B, Solid state · 1975 · 6.5K citations · Full text