Resonant torsion magnetometry in anisotropic quantum materials
arXiv:1802.08211 · doi:10.1038/s41467-018-06412-w
Abstract
Unusual behavior of quantum materials commonly arises from their effective low-dimensional physics, which reflects the underlying anisotropy in the spin and charge degrees of freedom. Torque magnetometry is a highly sensitive technique to directly quantify the anisotropy in quantum materials, such as the layered high-T superconductors, anisotropic quantum spin-liquids, and the surface states of topological insulators. Here we introduce the magnetotropic coefficient , the second derivative of the free energy F with respect to the angle between the sample and the applied magnetic field, and report a simple and effective method to experimentally detect it. A sub-g crystallite is placed at the tip of a commercially available atomic force microscopy cantilever, and we show that can be quantitatively inferred from a shift in the resonant frequency under magnetic field. While related to the magnetic torque , takes the role of torque susceptibility, and thus provides distinct insights into anisotropic materials akin to the difference between magnetization and magnetic susceptibility. The thermodynamic coefficient is discontinuous at second-order phase transitions and subject to Ehrenfest relations with the specific heat and magnetic susceptibility. We apply this simple yet quantitative method on the exemplary cases of the Weyl-semimetal NbP and the spin-liquid candidate RuCl, yet it is broadly applicable in quantum materials research.
arXiv comment7 pages including 6 figures and methods section
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Cited by in corpus (22)
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