Measurements on the triangular antiferromagnet MnSnB2O6 find static order below TN≈1 K coexisting with persistent spin dynamics, short-range correlations above TN, and C∝T^1.37 deep in the ordered state.
Melting upon cooling in a quantum magnet
2 Pith papers cite this work. Polarity classification is still indexing.
abstract
Heating enhances thermal fluctuations and typically leads to melting of solids, but in exceptional cases, heating can also cause liquids to solidify. The paradigm of this counterintuitive phenomenon is solidification of liquid $^3$He upon increasing temperature, known as the Pomeranchuk effect. Here we show that such inverse melting also appears in quantum magnetism. We find that, on cooling, the Ising-like triangular-lattice antiferromagnet erbium heptatantalate first develops a three-sublattice long-range magnetic order -- analogous to a solid -- which then, unexpectedly, melts at even lower temperatures into a short-range correlated spin-stripe state -- analogous to a liquid. We propose that such an unprecedented ``spin Pomeranchuk effect" can generically arise from strong competition between spin-spin interactions in frustrated magnets, and provides a novel avenue to transformations between exotic magnetic phases.
fields
cond-mat.str-el 2years
2026 2representative citing papers
Experiments on K3NdTe2O9 show a frustrated Jeff=1/2 triangular lattice antiferromagnet with persistent spin dynamics and no ordering or freezing down to 50 mK.
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Coexistence of static order and spin dynamics in an S = 5/2 frustrated triangular antiferromagnet
Measurements on the triangular antiferromagnet MnSnB2O6 find static order below TN≈1 K coexisting with persistent spin dynamics, short-range correlations above TN, and C∝T^1.37 deep in the ordered state.
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Exotic magnetism and persistent spin dynamics in a frustrated Jeff = 1/2 triangular lattice antiferromagnet
Experiments on K3NdTe2O9 show a frustrated Jeff=1/2 triangular lattice antiferromagnet with persistent spin dynamics and no ordering or freezing down to 50 mK.