Abstract |
Speaker : Dr. Andrés F. Santander-Syro
Language : ENGLISH
Affiliation : CSNSM, Université Paris-Sud and CNRS/IN2P3
Title : Momentum-resolved 'hidden-order' gap structure, symmetries, and entropy loss in URu2Si2
Abstract:
Due to their exceptionally strong correlations, ƒ-electron systems present a wide realm of original phase transitions and often poorly understood states of matter. One of the most intriguing is the so-called hidden-order (HO) state forming below THO =17.5 K in URu2Si2. Extensive macroscopic characterizations gathered during the last 30 years show a reduction of almost 60% in the electronic specific heat across the transition, and suggest that a gap of about 10 meV opens over more than 50% of its Fermi surface. However, the identification of the associated broken symmetry and gap structure remain longstanding riddles [1-3].
In this talk, I will present our state-of-the-art ARPES measurements imaging the reconstruction of the electronic structure of URu2Si2 across the hidden-order transition [4-6]. We observe a change of the electronic structure symmetry from body-centred tetragonal in the paramagnetic state to simple-tetragonal in the ordered state, described by the ordering vector Q0 = (1, 0, 0) (reciprocal-lattice units). This is accompanied by the opening of a gap of 7 meV over 70% of a large heavy-fermion Fermi surface, and the formation of four small “Fermi petals” at the incommensurate wave-vector Q1 = (0.6, 0, 0) showing another gap of 5 meV with respect to the states that defined the heavy-fermion Fermi surface above THO. Furthermore, the Fermi sheets measured in the HO state are in quantitative agreement with those determined by Shubnikov–de Haas experiments. Thus, our results provide a unified microscopic picture of the large entropy loss in the HO state, of the emergence of sharp inelastic peaks in the magnetic excitation spectrum at Q0 and the gap of magnetic excitations at Q1 observed by inelastic neutron scattering, and of the similarity found by magneto-transport measurements between the HO phase and the high-pressure antiferromagnetic phase, which would then be a consequence of both phases having the same simple-tetragonal electronic symmetry described by the ordering vector Q0.
[1] T. M. Palstra et al. Superconducting and magnetic transitions in the heavy-fermion system URu2Si2. Phys Rev Lett. 55, 2727-2730 (1985).
[2] M. B. Maple et al. Partially gapped Fermi surface in the heavy-electron superconductor URu2Si2. Phys. Rev. Lett. 56, 185-188 (1986).
[3] J. A. Mydosh and P. M. Oppeneer. Colloquium: Hidden order, superconductivity, and magnetism: The unsolved case of URu2Si2. Rev. Mod. Phys. 83, 1301 (2011).
[4] A. F. Santander-Syro et al. Fermi-surface instability at the ’hidden-order’ transition of URu2Si2. Nature Phys. 5, 637-641 (2009).
[5] F. L. Boariu et al. Momentum-resolved evolution of the Kondo lattice into “hidden-order” in URu2Si2. Phys. Rev. Lett. 110, 156404 (2013).
[6] C. Bareille et al. Momentum-resolved “hidden-order” gap structure, symmetries, and entropy loss in URu2Si2. Nature Communications (Accepted, 2014).
Organizer : Shin-ichi Fujimori
Mail : fujimori@spring8.or.jp
PHS : 3914
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