Direct transition from a disordered to a multiferroic phase on a triangular lattice
M. Kenzelmann, G. Lawes, A.B. Harris, G. Gasparovic, C. Broholm, A.P., Ramirez, G.A. Jorge, M. Jaime, S. Park, Q. Huang, A.Ya. Shapiro, and L.A., Demianets

TL;DR
This paper reports the first direct transition from a paramagnetic and paraelectric phase to an incommensurate multiferroic in a triangular lattice antiferromagnet, demonstrating ferroelectricity arising from chiral magnetic order.
Contribution
It introduces a simplified system where ferroelectricity appears simultaneously with a magnetic phase transition, linked to chiral magnetic order and geometric frustration.
Findings
Direct transition from paramagnetic to multiferroic phase observed
Magnetic field suppresses electric polarization by altering magnetic symmetry
Theoretical model explains ferroelectricity via chiral magnetic order
Abstract
Competing interactions and geometric frustration provide favourable conditions for exotic states of matter. Such competition often causes multiple phase transitions as a function of temperature and can lead to magnetic structures that break inversion symmetry, thereby inducing ferroelectricity [1-4]. Although this phenomenon is understood phenomenologically [3-4], it is of great interest to have a conceptually simpler system in which ferroelectricity appears coincident with a single magnetic phase transition. Here we report the first such direct transition from a paramagnetic and paraelectric phase to an incommensurate multiferroic in the triangular lattice antiferromagnet RbFe(MoO4)2 (RFMO). A magnetic field extinguishes the electric polarization when the symmetry of the magnetic order changes and ferroelectricity is only observed when the magnetic structure has chirality and breaks…
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