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Zigzag magnetic order in the iridium oxide Na2IrO3
Jiří Chaloupka1, George Jackeli, Giniyat Khaliullin
1Max Planck Institute for Solid State Research, Heisenbergstrasse 1, D-70569 Stuttgart, Germany.
We mapped the phase diagram for spin-orbit Mott insulators on a honeycomb lattice. Zigzag magnetic order is prevalent, originating from interorbital hopping, and validated with experimental data for Na2IrO3 and Li2IrO3.
Area of Science:
- Condensed Matter Physics
- Quantum Materials
- Solid State Physics
Background:
- Spin-orbit Mott insulators on honeycomb lattices exhibit complex magnetic phases.
- The Kitaev-Heisenberg model is a key theoretical framework for understanding these materials.
- Understanding the interplay of spin-orbit coupling and electron correlations is crucial.
Purpose of the Study:
- To explore the complete phase diagram of spin-orbit Mott insulators within the Kitaev-Heisenberg model.
- To identify the prevalence and origin of zigzag magnetic order.
- To determine spin coupling constants for specific iridate materials.
Main Methods:
- Investigated the phase diagram of the Kitaev-Heisenberg model across its full parameter space.
- Analyzed the physical origin of magnetic ordering, specifically zigzag-type order.
- Calculated magnetic susceptibility, spin wave spectra, and the zigzag order parameter.
Main Results:
- Zigzag-type magnetic order dominates a significant portion of the model's phase diagram.
- The emergence of zigzag order is attributed to interorbital t(2g)-e(g) hopping.
- Calculated parameters show good agreement with experimental data for Na2IrO3 and Li2IrO3.
Conclusions:
- The Kitaev-Heisenberg model accurately describes the magnetic properties of honeycomb spin-orbit Mott insulators.
- Interorbital hopping is a key mechanism driving zigzag magnetic order in these systems.
- The study provides crucial spin coupling constants for Na2IrO3 and Li2IrO3, aiding experimental verification.
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