Journal
STUDIA GEOPHYSICA ET GEODAETICA
Volume 66, Issue 3-4, Pages 187-205Publisher
SPRINGER
DOI: 10.1007/s11200-022-0829-2
Keywords
out-of-phase susceptibility; hematite; single crystals
Categories
Funding
- Czech Science Foundation [19-17442S]
- Institute of Geology of the Czech Academy of Sciences [RVO 67985831]
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This study investigated the unknown anisotropic properties of out-of-phase magnetic susceptibility (opMS) of hematite and their impact on understanding the origin of hematite magnetism. The research found that opMS shows strong field dependence along the basal plane and weak field dependence along the c-axis. The study also revealed that the second rank tensor is only an approximate representation of the directional opMS of hematite single crystals, and the distribution of measured and theoretical values differs significantly.
So far unknown anisotropic properties of out-of-phase magnetic susceptibility (opMS) of hematite and their bearing on understanding the origin of hematite magnetism were investigated on example of four single crystals from Minas Gerais, Brazil. The research comprised measurement of directional variation of field-dependent and frequency-dependent opMS and testing whether the anisotropy of opMS can be represented by the second rank tensor. It was found that the opMS shows strong field dependence along basal plane and only weak field dependence along c-axis. As for the frequency dependence, it is virtually non-existent along the basal plane. Along the c-axis, the opMS is similar at frequencies 976 and 3904 Hz, while at 15616 Hz it is clearly higher. Consequently, opMS is dominantly due to weak field hysteresis. The minimum opMS directions are parallel to the c-axis, while the other two principal directions lie within basal plane. The degree of anisotropy is extremely high (ratio of maximum opMS to minimum opMS >> 100) and the anisotropy ellipsoid is very oblate. In stereographic diagrams, the opMS contours very roughly resemble the theoretical contours calculated from opMS tensor. However, the differences between measured and theoretical values in directional opMS are clearly higher than the measuring error and are distributed very non-homogeneously. This indicates that the second rank tensor is only very approximate representative of the spatial variation of the directional opMS of hematite single crystals. Earlier model of hematite magnetism assuming slightly scanted antiferromagnetism along the c-axis and strongly canted antiferromagnetism or even weak ferromagnetism along the basal plane is supported.
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