• Anand, V.K.; Dhaka, R.S.; Lee, Y.; Harmon, B.N.; Kaminski, A.; Johnston, D.C.: Physical properties of metallic antiferromagnetic CaCo1.86As2 single crystals. Physical Review B 89 (2014), p. 214409/1-17

10.1103/PhysRevB.89.214409
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Abstract:
X-ray powder diffraction (XRD), magnetic susceptibility 𝜒, isothermal magnetization 𝑀, heat capacity 𝐶p, and in-plane electrical resistivity 𝜌 measurements as a function of temperature 𝑇 and magnetic field 𝐻 are presented for CaCo1.86⁢As2 single crystals. The electronic structure is probed by angle-resolved photoemission spectroscopy (ARPES) measurements of CaCo1.86⁢As2 and by full-potential linearized augmented-plane-wave calculations for the supercell Ca8⁢Co15⁢As16 (CaCo1.88⁢As2 ). Our XRD crystal structure refinement is consistent with the previous combined refinement of x-ray and neutron powder diffraction data showing a collapsed-tetragonal ThCr2⁢Si2 -type structure with 7(1)% vacancies on the Co sites corresponding to the composition CaCo1.86⁢As2. The anisotropic 𝜒⁡(𝑇) data are consistent with the magnetic neutron diffraction data of Quirianale et al. that demonstrate the presence of A-type collinear antiferromagnetic order below the Néel temperature 𝑇N=52 (1) K with the easy axis being the tetragonal 𝑐 axis. However, no clear evidence from the 𝜌⁡(𝑇) and 𝐶p⁡(𝑇) data for a magnetic transition at 𝑇N is observed. A metallic ground state is demonstrated from the band calculations and the 𝜌⁡(𝑇) , 𝐶p⁡(𝑇) , and ARPES data, and spin-polarized calculations indicate a competition between the A-type AFM and FM ground states. The 𝐶p⁡(𝑇) data exhibit a large Sommerfield electronic coefficient reflecting a large density of states at the Fermi energy 𝒟⁡(𝐸F) that is enhanced compared with the band structure calculation where the bare 𝒟⁡(𝐸F) arises from Co 3⁢𝑑 bands. At 1.8 K, the 𝑀⁡(𝐻) data for 𝐻∥𝑐 exhibit a well-defined first-order spin-flop transition at an applied field of 3.5 T. The small ordered moment of ≈ 0.3⁢𝜇B /Co obtained from the 𝑀⁡(𝐻) data at low 𝑇 , the large exchange enhancement of 𝜒 and the lack of a self-consistent interpretation of the 𝜒⁡(𝑇) and 𝑀⁡(𝐻,𝑇) data in terms of a local moment Heisenberg model together indicate that the magnetism of CaCo1.86⁢As2 is itinerant.