Metallicity of Ca2Cu6P5 with single and double copper-pnictide layers

Li Li, David Parker, Miaofang Chi, Georgiy M. Tsoi, Yogesh K. Vohra, Athena S. Sefat

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Abstract

We report thermodynamic and transport properties, and also theoretical calculations, for Cu-based compound Ca2Cu6P5 and compare with CaCu2-δP2. Both materials have layers of edge-sharing copper pnictide tetrahedral CuP4, similar to Fe-As and Fe-Se layers (with FeAs4, FeSe4) in the iron-based superconductors. Despite the presence of this similar transition-metal pnictide layer, we find that both Ca2Cu6P5 and CaCu2-δP2 have temperature-independent magnetic susceptibility and show metallic behavior with no evidence of either magnetic ordering or superconductivity down to 1.8 K CaCu2-δP2 is slightly off-stoichiometric, with δ = 0.14. Theoretical calculations suggest that unlike Fe 3d-based magnetic materials with a large density of states (DOS) at the Fermi surface, Cu have comparatively low DOS, with the majority of the 3d spectral weight located well below Fermi level. The room-temperature resistivity value of Ca2Cu6P5 is only 9 μΩ-cm, due to a substantial plasma frequency and an inferred electron-phonon coupling λ of 0.073 (significantly smaller than that of metallic Cu). Also, microscopy result shows that Cu-Cu distance along the c-axis within the double layers can be very short (2.5 Å), even shorter than metallic elemental copper bond (2.56 Å). The value of dρ/dT for CaCu2-δP2 at 300 K is approximately three times larger than in Ca2Cu6P5, which suggests the likelihood of stronger electron-phonon coupling. This study shows that the details of Cu-P layers and bonding are important for their transport characteristics. In addition, it emphasizes the remarkable character of the DOS of '122' iron-based materials, despite much structural similarities.

Original languageEnglish
Pages (from-to)334-339
Number of pages6
JournalJournal of Alloys and Compounds
Volume671
DOIs
StatePublished - Jun 25 2016

Funding

This work was supported by the U.S. Department of Energy , Office of Science, Basic Energy Sciences, Materials Science and Engineering Division (A.S.S.) . This study was partially funded (L.L., D.P.) by ORNL's Lab-directed Research & Development (LDRD) . The electron microscopy work was performed at the ORNL's Center for Nanophase Materials Sciences (CNMS), which is an Office of Science User Facility. We finally acknowledge support from the Department of Energy - National Nuclear Security Administration under Grant No. DE-NA0002014 (Y.V., G.M.T.) for pressure measurements.

FundersFunder number
Materials Science and Engineering Division
ORNL's Lab-directed Research & Development
U.S. Department of Energy
Office of Science
Basic Energy Sciences
National Nuclear Security Administration
Laboratory Directed Research and Development

    Keywords

    • Copper pnictide
    • Superconductivity
    • Thermal conductivity

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