Journal of the Physical Society of Japan · 2005 · 17 citations · 14 references
Natural SciencesPhysicsCondensed Matter PhysicsNuclear PhysicsQuantum MechanicsCrystal SymmetryHyperfine StructureStrongly Correlated Electron SystemsSymmetry BreakingAtomic NucleusElectric Quadrupole Hyperfine InteractionHyperfine InteractionsNuclear Quadrupole CouplingQuadrupole InteractionQuadrupole ModesQuadrupole SplittingSymmetry Breaking In Crystals
The still unclarified hidden order phase below T 0 =17.5 K in the heavy-electron system URu 2 Si 2 has been studied by 101 Ru NQR on a single crystal under H ext =0 and ambient P . Considering an invariant form of the quadrupole coupling between a 101 Ru nucleus and U 5 f electrons, which is compatible with the symmetry of the U–Ru bonds, it is shown that U 5 f quadrupoles can be probed by 101 Ru NQR and that the singlet ground-state models for the (5 f ) 2 configuration of U can naturally explain the observed large T -dependence of the NQR frequency 101 ν 2Q ( T ) above T 0 . 101 ν 2Q ( T ) shows a slight but significant increase below \(T_{\text{Q}}\cong13.5\) K. Combining with general considerations on the effects on 101 Ru NQR of a possible symmetry-breaking electric field gradient (EFG) or hyperfine field due to hidden order, we discuss that the increase can be interpreted as arising from symmetry-breaking EFG components of V y z and/or V z x due to quadrupole order. In this interpretation the onset of the quadrupole order is retarded by about 4 K below T 0 , which is discussed in connection with related measurements.
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