4.6 Article

Angle-resolved magnetoresistance in the strongly anisotropic quantum magnet TmB4

Journal

PHYSICAL REVIEW B
Volume 107, Issue 14, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.107.144403

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Precise angle-resolved magnetoresistance (ARMR) measurements in TmB4 reveal the anisotropic charge transport and magnetic structure of this strongly Ising anisotropic quantum antiferromagnet. Ap/p(v,H) distributions show that the main magnetoresistance features appear along the easy axis of magnetic anisotropy and are related to magnetic phases and phase transitions. ARMR is a sensitive tool for studying the interplay between charge carriers and magnetic structure.
Precise angle-resolved magnetoresistance (ARMR) measurements in various magnetic fields enabled us to create illustrative distributions of Ap/p(v, H) in TmB4, where v is the angle between the sample c axis and applied magnetic field H. These distributions reveal the charge transport anisotropy in this strongly Ising anisotropic quantum antiferromagnet with a geometrically frustrated Shastry-Sutherland lattice exhibiting frac-tional magnetization plateaus. While in the paramagnetic region Ap/p(v, H) reaches its maxima for H 1c, below the Neel temperature TN = 11.7 K the situation is different. Here the main MR features appear for H II c, i.e., along the easy axis of magnetic anisotropy, and correspond to magnetic phases and phase transitions between them. It is interesting that all the above features (maxima) related with the scattering of conduction electrons on spin magnetic structure are related with fractional magnetization plateaus. With increasing v MR anomalies shift to higher fields. Above the field of magnetic saturation, moreover, significant MR maxima have been observed at certain angles which correspond to specific directions in the crystal lattice, pointing to field directions in which the scattering of conduction electrons on the magnetic structure is the highest. Thus, ARMR appears to be a sensitive experimental tool reflecting the angular dependence of the interplay between charge carriers and magnetic structure as a function of temperature and applied magnetic field.

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