Ultra-high purity delafossite metals
MPI-CPfS co-workers: Pallavi Kushwaha, Veronika Sunko, Nabhanila Nandi, Helge Rosner, Markus Schmidt, Horst Bormann, Clifford Hicks, Frank Arnold, Elena Hassinger. Philip Moll and Andy Mackenzie
The delafossite structural series of general formula ABO2 features a wide range of physical properties including transparent conductors, candidate magneto- and thermoelectrics and magnetic insulators. Arguably less well-known are an astonishing series of metals such as PdCoO2, PtCoO2 and PdCrO2. Quasi-two-dimensional and with conduction taking place in planes of triangular lattice noble metals, they have both the highest known conductivity. Our work has established that, at low temperatures, resisitivities of only a few nWcm, corresponding to mean free paths as high as 50 μm, can be obtained in PdCoO2. The microscopic origins of these record-breaking electrical properties are not well understood.
Although first synthesized over forty years ago, full appreciation of the properties and potential of the delafossite metals has been reached only relatively recently. To put their purity levels in context, a 50 μm mean free path in the impurity scattering limit would correspond to there being only one defect approximately every 200000 lattice spacings. For this to be observed in melt-grown single crystals implies either unprecedented chemical perfection of the noble metal conducting layers or some suppression of electron scattering.
After becoming interested in this problem five years ago following discussions with our collaborators in the group of Yoshi Maeno at Kyoto University, we performed a series of de Haas-van Alphen effect and transport studies on PdCoO2 and PdCrO2, confirming the extremely high purity of PdCoO2 [1] and the existence of weak coupling between Cr3+ spins and Pd conduction electrons in PdCrO2 [2]. We then embarked on a programme of in-house crystal growth, succeeding in growing the first ‘large’ single crystals of PtCoO2 (sub-mm plates a few μm thick). Using modern focused ion beam technology of the kind now set up in our department at the Institute, we cut samples such as the one shown in Fig. 1c for precise transport measurements. These revealed that the room temperature resistivity of PtCoO2 is only 2.1 μΩcm, corresponding to a room temperature conductivity per carrier nearly double that of elemental copper.