Suppression of Antiferromagnetic Order by Strain in Honeycomb Cobaltate: Implication for Quantum Spin Liquid
arXiv:2311.09609 · doi:10.1126/sciadv.adn8694
Abstract
Recently, layered honeycomb cobaltates have been predicted as a new promising system for realizing the Kitaev quantum spin liquid, a many-body quantum entangled ground state characterized by fractional excitations. However, these cobaltates, similar to other candidate materials, exhibit classical antiferromagnetic ordering at low temperatures, which impedes the formation of the expected quantum state. Here, we demonstrate that the control of the trigonal crystal field of Co ions is crucial to suppress classical antiferromagnetic ordering and to locate its ground state in closer vicinity to quantum spin liquid in layered honeycomb cobaltates. By utilizing heterostructure engineering on Cu3Co2SbO6 thin films, we adjust the trigonal distortion of CoO6 octahedra and the associated trigonal crystal field. The original Néel temperature of 16 K in bulk Cu3Co2SbO6 decreases (increases) to 7.8 K (22.7 K) in strained Cu3Co2SbO6 films by decreasing (increasing) the magnitude of the trigonal crystal fields. Our experimental finding substantiates the potential of layered honeycomb cobaltate heterostructures and strain engineering to accomplish the extremely elusive quantum phase of matter.
References in corpus (25)
- Restoring the density-gradient expansion for exchange in solids and surfaces
- Generalized gradient approximation for solids and their surfaces
- Mott Insulators in the Strong Spin-Orbit Coupling Limit: From Heisenberg to a Quantum Compass and Kitaev Models
- Pseudospin exchange interactions in d^7 cobalt compounds: Possible realization of the Kitaev model
- Crystal field splitting and correlation effect on the electronic structure of A2IrO3
- Kitaev-Heisenberg Hamiltonian for High-Spin Mott Insulators
- Anisotropic Ru3+ 4d5 magnetism in the alpha-RuCl3 honeycomb system: susceptibility, specific heat and Zero field NMR
- Magnetic Excitations and Continuum of a Field-Induced Quantum Spin Liquid in -RuCl
- Kitaev interactions in the Co honeycomb antiferromagnets NaCoSbO and NaCoTeO
- Magnetic properties of the honeycomb oxide NaCoTeO
- Weak-field induced nonmagnetic state in a Co-based honeycomb
- Strain Doping: Reversible Single-Axis Control of a Complex Oxide Lattice via Helium Implantation
- Magnetic order in single crystals of Na3Co2SbO6 with a honeycomb arrangement of 3d Co ions
- Geometrical frustration versus Kitaev interactions in BaCo(AsO)
- Dominant Kitaev interactions in the honeycomb materials NaCoSbO and NaCoTeO
- A magnetic continuum observed by terahertz spectroscopy in a quantum spin liquid candidate BaCo(AsO)
- Magnetic Couplings in Edge-Sharing High-Spin Compounds
- Ab initio guided minimal model for the "Kitaev" material BaCo(AsO): Importance of direct hopping, third-neighbor exchange and quantum fluctuations
- Non-Kitaev vs. Kitaev Honeycomb Cobaltates
- Towards Kitaev Spin Liquid in 3d Transition Metal Compounds
- Magnetic phase diagram and possible Kitaev-like behavior of honeycomb-lattice antimonate Na3Co2SbO6
- Exchange interactions in Kitaev materials: From NaIrO to -RuCl
- Proximate Dirac spin liquid in honeycomb lattice - XXZ model: Numerical study and application to cobaltates
- Honeycomb oxide heterostructure: a new platform for Kitaev quantum spin liquid
- Emergent magnetism with continuous control in the ultrahigh conductivity layered oxide PdCoO2
Cited by in corpus (7)
- Polymorphism and Magnetism in a Kitaev Honeycomb Cobaltate KCoAsO
- Spin-orbit entangled moments and magnetic exchange interactions in cobalt-based honeycomb magnets BaCo(O) ( = P, As, Sb)
- Digital Quantum Simulation of the Kitaev Quantum Spin Liquid
- Field-induced magnetic phases in the Kitaev candidate NaCoSbO
- Coexistence of static and dynamic local magnetic fields in an S = 3/2 honeycomb lattice antiferromagnet Co2Te3O8
- Crystalline water intercalation into the Kitaev honeycomb cobaltate NaCoTeO
- Trigonal distortion in the Kitaev candidate honeycomb magnet BaCo2(AsO4)2