Melting of charge order in the low-temperature state of an electronic ferroelectric
arXiv:1905.12740 · doi:10.1038/s41535-020-0217-5
Abstract
Strong electronic interactions can drive a system into a state with a symmetry breaking. Lattice frustration or competing interactions tend to prevent a symmetry breaking, leading to quantum disordered phases. In spin systems frustration can produce a spin liquid state. Frustration of a charge degree of freedom also can result in various exotic states, however, experimental data on these effects is scarce. In this work we demonstrate how a charge ordered ferroelectric looses the order on cooling to low temperatures using an example of a Mott insulator on a weakly anisotropic triangular lattice -(BEDT-TTF)Hg(SCN)Cl. Typically, a low temperature ordered state is a ground state of a system, and the demonstrated re-entrant behavior is unique. Raman scattering spectroscopy finds that this material enters an insulating ferroelectric `dipole solid' state at , but below the order melts, while preserving the insulating energy gap. The resulting phase diagram is relevant to other quantum paraelectric materials.
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Cited by in corpus (12)
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