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Frustrated spin chain physics near the Majumdar-Ghosh point in szenicsite Cu3(MoO4)(OH)4

MPG-Autoren
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Lebernegg,  Stefan
Physics of Quantum Materials, Max Planck Institute for Chemical Physics of Solids, Max Planck Society;

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Rosner,  H.
Physics of Quantum Materials, Max Planck Institute for Chemical Physics of Solids, Max Planck Society;

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Zitation

Lebernegg, S., Janson, O., Rousochatzakis, I., Nishimoto, S., Rosner, H., & Tsirlin, A. A. (2017). Frustrated spin chain physics near the Majumdar-Ghosh point in szenicsite Cu3(MoO4)(OH)4. Physical Review B, 95(3): 035145, pp. 1-10. doi:10.1103/PhysRevB.95.035145.


Zitierlink: https://hdl.handle.net/11858/00-001M-0000-002D-2DCA-6
Zusammenfassung
In this joint experimental and theoretical work magnetic properties of the Cu2+ mineral szenicsite Cu-3(MoO4)(OH)(4) are investigated. This compound features isolated triple chains in its crystal structure, where the central chain involves an edge-sharing geometry of the CuO4 plaquettes, while the two side chains feature a corner-sharing zigzag geometry. The magnetism of the side chains can be described in terms of antiferromagnetic dimers with a coupling larger than 200 K. The central chain was found to be a realization of the frustrated antiferromagnetic J(1)-J(2) chain model with J(1) similar or equal to 68 K and a sizable second-neighbor coupling J(2). The central and side chains are nearly decoupled owing to interchain frustration. Therefore, the low-temperature behavior of szenicsite should be entirely determined by the physics of the central frustrated J(1)-J(2) chain. Our heat-capacity measurements reveal an accumulation of magnetic entropy at low temperatures and suggest a proximity of the system to the Majumdar-Ghosh point of the antiferromagnetic J(1)-J(2) spin chain, J(2)/J(1) = 0.5.