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Journal Article | FZJ-2023-04627 |
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2023
Americal Physical Society
College Park, Maryland
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Please use a persistent id in citations: doi:10.1103/PhysRevB.107.104104 doi:10.34734/FZJ-2023-04627
Abstract: The gradual ferromagnetic spin reorientation in hexagonal close packed cobalt (hcp-Co) phase between 230 $^\circ$C and 330 $^\circ$C reported for a Co single crystal [Bertaut $\textit{et al.}$, Solid State Commun. $\textbf{1}$, 81 (1963)] suggests that this phase could not have a hexagonal symmetry. This hypothesis is verified positively by synchrotron radiation diffraction and neutron diffraction on polycrystalline powder cobalt. The analysis of diffraction data has been done by using a specific set of Bragg peaks, which are not sensitive to the stacking faults present in abundance in hcp-Co. The crystal structure of the hcp-type ordered areas of cobalt is described by the monoclinic symmetry with the magnetic space group $C2'/m'$. In this monoclinic crystal structure the former hexagonal $[001]$ axis is no longer perpendicular to the hexagonal layers. The hexagonal $[001]$ and $[010]$ axes make an angle equal $\alpha \approx 90.10(1)$ $^\circ$, while the angle between in-plane $[100]$ and $[010]$ axes equals $\gamma \approx 120.11(1)$ $^\circ$. The monoclinic symmetry provides an approximate description of the crystal structure of the stacking faulted hcp-Co areas coexisting with fcc-Co areas.
Keyword(s): Magnetic Materials (1st) ; Crystallography (2nd) ; Magnetism (2nd) ; Condensed Matter Physics (2nd) ; Materials Science (2nd)
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