Abstract
Exotic electronic states resulting from entangled spin and orbital degrees of freedom are hallmarks of strongly correlated f-electron systems. A spectacular example is the so-called hidden-order (HO) phase transition in the heavy-electron metal URu 2 Si 2 , which is characterized by the huge amount of entropy lost at T HO =17.5K (refs 2,3). However, no evidence of magnetic/structural phase transition has been found below T HO so far. The origin of the HO phase transition has been a long-standing mystery in condensed-matter physics. Here, on the basis of a first-principles theoretical approach, we examine the complete set of multipole correlations allowed in this material. The results uncover that the HO parameter is a rank-5 multipole (dotriacontapole) order with nematic E - symmetry, which exhibits staggered pseudospin moments along the [110] direction. This naturally provides comprehensive explanations of all key features in the HO phase including anisotropic magnetic excitations, the nearly degenerate antiferromagnetic-ordered state and spontaneous rotational-symmetry breaking.
Original language | English |
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Pages (from-to) | 528-533 |
Number of pages | 6 |
Journal | Nature Physics |
Volume | 8 |
Issue number | 7 |
DOIs | |
Publication status | Published - 2012 Jul |
Externally published | Yes |
ASJC Scopus subject areas
- Physics and Astronomy(all)