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Fluctuating magnetism in Zn-doped averievite with well-separated kagome layers

G. Simutis1,2,3,*, L. Suárez-García2, H. Zeroual1, I. Villa1,2, M. Georgopoulou4,5, D. Boldrin6, D. Chatterjee1,7, C. N. Wang2, C. Baines2 et al.

T. Shiroka2,8, R. Khasanov2, H. Luetkens2, B. Fåk5, Y. Sassa3,9, M. Bartkowiak2, A. S. Wills4, E. Kermarrec1, F. Bert1, and P. Mendels1

  • *Contact author: gediminas.simutis@psi.ch

Phys. Rev. Materials 9, 074003 – Published 11 July, 2025

DOI: https://doi.org/10.1103/l7gq-cc96

Abstract

Kagome lattice decorated with S=1/2 spins is one of the most discussed ways to realize a quantum spin liquid. However, all previous material realizations of this model have suffered from additional complications, ranging from additional interactions to impurity effects. Recently, a new quantum kagome system has been identified in the form of averievite Cu5−xZnxV2O10(CsCl), featuring a unique double-layer spacing between the kagome planes. Using muon spin spectroscopy we show that only a complete substitution (i.e., x=2) of interplanar copper ions leads to a quantum-disordered ground state. In contrast, the parent compound (x=0) exhibits long-range magnetic order, with a phase transition around 24 K. Experiments performed on the partially substituted material (x=1) show that the transformation proceeds through an intermediate disordered, partially frozen ground state, unaffected by pressures up to 23 kbar. Our study provides a microscopic view of the magnetism of the decoupling of the kagome layers and establishes the averievite as a new material platform for the experimental study of the fully-decoupled kagome layers.

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