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Reentrant multiple-$\mathbf{q}$ magnetic order and a "spin-cholesteric" phase in Sr$_3$Fe$_2$O$_7$

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abstract

Spin-nematic and spin-smectic phases have been reported in magnetic materials, which break rotational symmetry while preserving translational symmetry along certain directions. However, until now the analogy to liquid crystals remained incomplete because no magnetic analog of cholesteric order was known. Here we show that the bilayer perovskite Sr$_3$Fe$_2$O$_7$, previously believed to adopt a simple single-$\mathbf{q}$ spin-helical order, hosts two distinct types of multi-$\mathbf{q}$ spin textures and the first "spin-cholesteric". Its ground state represents a novel multi-$\mathbf{q}$ spin texture with unequally intense spin modulations at the two ordering vectors. This is followed in temperature by the new "spin-cholesteric" phase with spontaneously broken chiral symmetry, in which the translational symmetry is broken only along one of the crystal directions while the weaker orthogonal modulation melts, giving rise to intense short-range dynamical fluctuations. Shortly before the transition to the paramagnetic state, vortex-crystal order spanned by two equivalent $\mathbf{q}$ vectors emerges. The "spin-cholesteric" phase completes the spin analogy with liquid crystals and renders Sr$_3$Fe$_2$O$_7$ a touchstone for studying transitions among multiple-$\mathbf{q}$ spin textures in a centrosymmetric host.

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representative citing papers

A Magnon Band Analysis of GdRu2Si2 in the Field-Polarized State

cond-mat.str-el · 2025-01-02 · conditional · novelty 6.0

Inelastic neutron scattering in the field-polarized state of GdRu2Si2 yields a magnon dispersion fitted by bilinear Heisenberg exchange interactions J1 through J8, with no sign of higher-order or anisotropic terms.

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  • A Magnon Band Analysis of GdRu2Si2 in the Field-Polarized State cond-mat.str-el · 2025-01-02 · conditional · none · ref 30 · internal anchor

    Inelastic neutron scattering in the field-polarized state of GdRu2Si2 yields a magnon dispersion fitted by bilinear Heisenberg exchange interactions J1 through J8, with no sign of higher-order or anisotropic terms.