Evidence for a three-dimensional quantum spin liquid in PbCuTe2O6

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作者
Shravani Chillal
Yasir Iqbal
Harald O. Jeschke
Jose A. Rodriguez-Rivera
Robert Bewley
Pascal Manuel
Dmitry Khalyavin
Paul Steffens
Ronny Thomale
A. T. M. Nazmul Islam
Johannes Reuther
Bella Lake
机构
[1] Helmholtz-Zentrum Berlin für Materialien und Energie,Department of Physics
[2] Indian Institute of Technology Madras,Research Institute for Interdisciplinary Science
[3] Okayama University,NIST Center for Neutron Research
[4] National Institute of Standards and Technology,Department of Materials Science
[5] University of Maryland,ISIS Facility
[6] STFC Rutherford Appleton Laboratory,Institute for Theoretical Physics and Astrophysics
[7] Institut Laue-Langevin,Dahlem Center for Complex Quantum Systems and Fachbereich Physik
[8] Julius-Maximilians-Universität Würzburg,Institut für Festkörperphysik
[9] Am Hubland,undefined
[10] Freie Universität Berlin,undefined
[11] Technische Universität Berlin,undefined
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摘要
The quantum spin liquid is a highly entangled magnetic state characterized by the absence of static magnetism in its ground state. Instead, the spins fluctuate in a highly correlated way down to the lowest temperatures. Quantum spin liquids are very rare and are confined to a few specific cases where the interactions between the magnetic ions cannot be simultaneously satisfied (known as frustration). Lattices with magnetic ions in triangular or tetrahedral arrangements, which interact via isotropic antiferromagnetic interactions, can generate such a frustration. Three-dimensional isotropic spin liquids have mostly been sought in materials where the magnetic ions form pyrochlore or hyperkagome lattices. Here we present a three-dimensional lattice called the hyper-hyperkagome that enables spin liquid behaviour and manifests in the compound PbCuTe2O6. Using a combination of experiment and theory, we show that this system exhibits signs of being a quantum spin liquid with no detectable static magnetism together with the presence of diffuse continua in the magnetic spectrum suggestive of fractional spinon excitations.
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