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Symmetry of the Hidden Order in URu<sub>2</sub>Si<sub>2</sub>from Nuclear Magnetic Resonance Studies
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Citations
19
References
2012
Year
Crystal StructureEngineeringMagnetic ResonanceRu NmrNuclear Quadrupole ResonanceSymmetry (Physics)Quantum MaterialsExotic StateHidden OrderPhysicsQuantum Field TheoryCrystallographyQuantum MagnetismTransition Metal ChalcogenidesSpintronicsNatural SciencesApplied PhysicsCondensed Matter PhysicsTopological Heterostructures
The hidden order (HO) in URu 2 Si 2 has been investigated by both 29 Si and 99 Ru NMR on a single crystal. Tiny, but finite additional broadening of the spectrum in the HO phase in both 29 Si and 99 Ru NMR with external magnetic field applied along the crystallographic [100] or [110] direction, and its persistence as H ext →0 in 29 Si NMR clearly indicate the existence of internal hyperfine field, and the breaking of the time-reversal symmetry in the HO phase can therefore be concluded. We discuss which symmetry of the D 4 h symmetry group of the URu 2 Si 2 crystal structure is compatible with the observed dependence on the crystal-axis direction of the existence or nonexistence of the internal hyperfine field. Then, by imposing a strong constraint that the wave-vector of the HO is also Q 0 =[0,0,1], the wave-vector of the pressure-induced antiferromagnetism, we show that the two-dimensional representation E - remains as the only possible candidate for the HO symmetry. Since dipoles are obviously excluded from the major HO parameter, we conclude the E - multipole (octupole or triakontadipole) to be the HO parameter. We further discuss that the E - multipole, but with no associated dipoles, seems to be a key feature of the HO in URu 2 Si 2 .
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