AI summary · arXiv: 2311.05004v1 · cond-mat.stat-mech

Fluctuation-induced spin nematic order in magnetic charge-ice

A. Hemmatzade, K. Essafi, M. Taillefumier, M. Müller, T. Fennell, P. M. Derlet
Original paper Submitted to arXiv on 08 Nov. 2023 16 pages, 9 figures, submitted License: CC BY 4.0

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The essentials

  • Researchers investigate the effects of correlated structural disorder on material behavior
  • Focus on charge-ice phenomenon with strong and long-range correlated disorder
  • Correlated disorder characterized by randomly packed loops of a single cation-type
  • Magnetic cations interact antiferromagnetically, leading to intertwined Heisenberg spin chains
  • Spin liquid phase observed at intermediate temperatures
  • Discontinuous transition to spin nematic phase at lower temperatures
  • Spin symmetry reduced in nematic phase, resulting in slower spin relaxation
  • Transition sensitive to statistics of cation loops, providing thermodynamic signature and route to engineering stability
  • Correlated structural disorder gives rise to non-local degrees of freedom associated with lower dimensional clusters or strings
  • Implications for materials with similar forms of correlated disorder and potential for new universality classes in continuous phase transitions
  • Disorder can be used to tune functionalities and reveal new behaviors

Key points written by AI: they may contain errors, check them against the paper.

AI-generated keywords: Charge-ice Spin Liquid Spin Nematic Correlated Disorder Algebraic Spin Liquid

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  • Original abstract
In this study, the researchers investigate the effects of correlated structural disorder on the behavior of materials. They focus specifically on a phenomenon called charge-ice, where structural disorder is not weak and local, but strong and long-range correlated. In charge-ice, two cations of different charge occupy a pyrochlore lattice in such a way that each tetrahedron hosts two cations of each type. The resulting correlated disorder is characterized by randomly packed loops of a single cation-type. If these cations are magnetic and interact antiferromagnetically, a new type of magnet with strong interactions along the loops but frustrated interactions between loops emerges. This leads to an ensemble of intertwined Heisenberg spin chains that form an algebraic spin liquid at intermediate temperatures. At lower temperatures, the researchers observe that these non-local degrees of freedom undergo a discontinuous transition to a spin nematic phase. Although this phase does not break time reversal symmetry, its spin symmetry is reduced, resulting in a dramatically slower spin relaxation. The transition is found to be sensitive to the statistics of the cation loops, providing both a direct thermodynamic signature of otherwise elusive structural information and a structural route to engineering nematic phase stability. The study highlights that correlated structural disorder can give rise to non-trivial behavior due to the emergence of non-local degrees of freedom associated with lower dimensional clusters or strings. This finding has implications for various types of materials with similar forms of correlated disorder and suggests that transferring the concept could lead to new universality classes in continuous phase transitions. Moreover, it provides insights into how disorder in materials can be used to tune their functionalities and reveals entirely new behaviors arising from strong and long-range correlated structural disorder.

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