Physical Review Letters· 2012Q1
Relevance of the Heisenberg-Kitaev Model for the Honeycomb Lattice Iridates<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mi>A</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>IrO</mml:mi><mml:mn>3</mml:mn></mml:msub></mml:math>
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- 2012year
Short summary
The Heisenberg-Kitaev model, including interactions beyond nearest neighbors, accurately describes the magnetic ordering in honeycomb lattice iridates (A2IrO3), explaining experimental thermodynamic measurements and low-temperature zigzag magnetic order.
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Key points
- Honeycomb lattice iridates (A2IrO3) are magnetic Mott insulators with effective S=1/2 moments.
- An extended Heisenberg-Kitaev model, including beyond nearest-neighbor interactions, describes their magnetism.
- The model explains experimental thermodynamic data (Curie-Weiss temperature, ordering temperature) and low-temperature zigzag magnetic order.
- Na2IrO3 is in a magnetically ordered regime, while Li2IrO3 is near a spin-liquid regime.
AI-generated from the title and abstract; the full text is not read.
Abstract
Combining thermodynamic measurements with theoretical calculations we demonstrate that the iridates ${A}_{2}{\mathrm{IrO}}_{3}$ ($A=\mathrm{Na}$, Li) are magnetically ordered Mott insulators where the magnetism of the effective spin-orbital $S=1/2$ moments can be captured by a Heisenberg-Kitaev (HK) model with interactions beyond nearest-neighbor exchange. Experimentally, we observe an increase of the Curie-Weiss temperature from $\ensuremath{\theta}\ensuremath{\approx}\ensuremath{-}125\text{ }\text{ }\mathrm{K}$ for ${\mathrm{Na}}_{2}{\mathrm{IrO}}_{3}$ to $\ensuremath{\theta}\ensuremath{\approx}\ensuremath{-}33\text{ }\text{ }\mathrm{K}$ for ${\mathrm{Li}}_{2}{\mathrm{IrO}}_{3}$, while the ordering temperature remains roughly the same ${T}_{N}\ensuremath{\approx}15\text{ }\text{ }\mathrm{K}$. Using functional renormalization group calculations we show that this evolution of $\ensuremath{\theta}$ and ${T}_{N}$ as well as the low temperature zigzag magnetic order can be captured within this extended HK model. We estimate that ${\mathrm{Na}}_{2}{\mathrm{IrO}}_{3}$ is deep in a magnetically ordered regime, while ${\mathrm{Li}}_{2}{\mathrm{IrO}}_{3}$ appears to be close to a spin-liquid regime.
The authors' abstract, as published at the source. Physical Review Letters, 2012 · DOI ↗
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Field: Condensed Matter Physics
Condensed Matter PhysicsPhysics and Astronomy