Elastic properties of hidden order in URuSi are reproduced by a staggered nematic
arXiv:1910.01669 · doi:10.1103/PhysRevB.102.075129
Abstract
We develop a phenomenological mean field theory describing the hidden order phase in URuSi as a nematic of the representation staggered along the -axis. Several experimental features are reproduced by this theory: the topology of the temperature--pressure phase diagram, the response of the elastic modulus above the transition at ambient pressure, and orthorhombic symmetry breaking in the high-pressure antiferromagnetic phase. In this scenario, hidden order is characterized by broken rotational symmetry that is modulated along the -axis, the primary order of the high-pressure phase is an unmodulated nematic, and the triple point joining those two phases with the high-temperature paramagnetic phase is a Lifshitz point.
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