Abstract

A promising route to realize entangled magnetic states combines geometrical frustration with quantum-tunneling effects. Spin-ice materials are canonical examples of frustration, and Ising spins in a transverse magnetic field are the simplest many-body model of quantum tunneling. Here, we show that the tripod-kagome lattice material Ho3Mg2Sb3O14 unites an icelike magnetic degeneracy with quantum-tunneling terms generated by an intrinsic splitting of the Ho3+ ground-state doublet, which is further coupled to a nuclear spin bath. Using neutron scattering and thermodynamic experiments, we observe a symmetry-breaking transition at to a remarkable state with three peculiarities: a concurrent recovery of magnetic entropy associated with the strongly coupled electronic and nuclear degrees of freedom; a fragmentation of the spin into periodic and icelike components; and persistent inelastic magnetic excitations down to . These observations deviate from expectations of classical spin fragmentation on a kagome lattice, but can be understood within a model of dipolar kagome ice under a homogeneous transverse magnetic field, which we survey with exact diagonalization on small clusters and mean-field calculations. In Ho3Mg2Sb3O14, hyperfine interactions dramatically alter the single-ion and collective properties, and suppress possible quantum correlations, rendering the fragmentation with predominantly single-ion quantum fluctuations. Our results highlight the crucial role played by hyperfine interactions in frustrated quantum magnets and motivate further investigations of the role of quantum fluctuations on partially ordered magnetic states.

Highlights

  • Quantum spin liquids are exotic states of magnetic matter in which conventional magnetic order is suppressed by strong quantum fluctuations [1]

  • Such dynamics may stabilize a putative “quantum spin fragmented” (QSF) state that remains characterized by the coexistence of Bragg peaks and highly structured diffuse scattering in magnetic neutron scattering experiments, but with dynamic magnetic correlations reflecting coherent collective excitations, akin to the emergent monopole and photonlike excitations in quantum spin ice [10,45]

  • We observe structured dynamic magnetic correlations at low temperature, indicating persistent spin dynamics in sharp contrast to the Dy3þ compound. We show that this stems from the low symmetry of the tripod-kagome structure and the non-Kramers nature of the Ho3þ ion, the combination of which generates an effective local magnetic field transverse to the Ising magnetic dipole moments

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Summary

INTRODUCTION

Quantum spin liquids are exotic states of magnetic matter in which conventional magnetic order is suppressed by strong quantum fluctuations [1]. Such dynamics may stabilize a putative “quantum spin fragmented” (QSF) state that remains characterized by the coexistence of Bragg peaks and highly structured diffuse scattering in magnetic neutron scattering experiments, but with dynamic magnetic correlations reflecting coherent collective excitations, akin to the emergent monopole and photonlike excitations in quantum spin ice [10,45]. It is unclear if such a partially disordered quantum state can theoretically prevail as an extended phase at finite temperature. VII with a discussion of the general implications of our study

METHODS
Crystal structure and interactions
Crystal-field Hamiltonian
Nuclear hyperfine Hamiltonian
Transverse Ising model
Jijσzi σzi : ð10Þ
SPECIFIC-HEAT MEASUREMENTS
INELASTIC NEUTRON-SCATTERING MEASUREMENTS
THEORETICAL MODELING
Exact diagonalization
10 Perturbative region
Mean-field Monte Carlo simulations
Findings
DISCUSSION AND CONCLUSIONS
Full Text
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