Weak uncorrelated quenched disorder drives the topological transition of the 3D Z2 gauge model into a new universality class, consistent with the Harris criterion.
Vojta, Disorder in quantum many-body systems, Annu
2 Pith papers cite this work. Polarity classification is still indexing.
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K₂Fe₂(MoO₄)(PO₄)₂ single crystals exhibit weak magnetic order at 5.2 K coexisting with persistent spin dynamics and two distinct short-range correlation regimes at 34 K and 10 K on a double trillium lattice.
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Finite-temperature topological transitions in the presence of quenched uncorrelated disorder
Weak uncorrelated quenched disorder drives the topological transition of the 3D Z2 gauge model into a new universality class, consistent with the Harris criterion.
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Multistage development of short-range spin correlations and weak magnetic order in the two coupled trillium lattices of K2Fe2(MoO4)(PO4)2
K₂Fe₂(MoO₄)(PO₄)₂ single crystals exhibit weak magnetic order at 5.2 K coexisting with persistent spin dynamics and two distinct short-range correlation regimes at 34 K and 10 K on a double trillium lattice.