Rotational Symmetry Breaking in the Hidden-Order Phase of URu2Si2
R. Okazaki, T. Shibauchi, H. J. Shi, Y. Haga, T. D. Matsuda, E., Yamamoto, Y. Onuki, H. Ikeda, Y. Matsuda

TL;DR
This study reveals that the hidden order phase in URu2Si2 involves spontaneous breaking of four-fold rotational symmetry, indicating an electronic nematic phase characterized by in-plane magnetic susceptibility anisotropy below 17.5 K.
Contribution
The paper provides direct experimental evidence of rotational symmetry breaking in URu2Si2's hidden order phase, suggesting it is an electronic nematic state.
Findings
Detection of in-plane magnetic susceptibility anisotropy below T_h
Observation of two-fold magnetic torque oscillations
Evidence for rotational symmetry breaking in the hidden order phase
Abstract
A second-order phase transition is characterized by spontaneous symmetry breaking. The nature of the broken symmetry in the so-called "hidden order" phase transition in the heavy fermion compound URu2Si2, at transition temperature T_h=17.5 K, has posed a long-standing mystery. We report the emergence of an in-plane anisotropy of the magnetic susceptibility below T_h, which breaks the four-fold rotational symmetry of the tetragonal URu2Si2. Two-fold oscillations in the magnetic torque under in-plane field rotation were sensitively detected in small pure crystals. Our findings suggest that the hidden-order phase is an electronic "nematic" phase, a translationally invariant metallic phase with spontaneous breaking of rotational symmetry.
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