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Volumn 92, Issue 2, 2015, Pages

Hidden symmetries of the extended Kitaev-Heisenberg model: Implications for the honeycomb-lattice iridates A2IrO3

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Indexed keywords


EID: 84938217345     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.92.024413     Document Type: Article
Times cited : (259)

References (79)
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    • note
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    • ab| ≃ 1.9 [74].
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    • Regarding the terminology used here, we have in mind that the compass-type and Kitaev-type interactions are very distinct in their physical appearance and origin. While the compass-spins (pseudodipoles) as introduced in Ref. [4] align themselves along the bond direction as real compasses do (hence the name), the spins in the Kitaev honeycomb model tend rather to avoid the bond directions. Placed on a honeycomb lattice, the bond-directional compasses would feel much less frustrated than the Kitaev spins, and show "order-from-disorder" behavior instead. As to the physical origin, the compass-type and Kitaev-type spin anisotropy terms arise in compounds with distinct chemical bonding geometries - corner-shared [16,9] and edge-shared [6,9] structures, correspondingly
    • Regarding the terminology used here, we have in mind that the compass-type and Kitaev-type interactions are very distinct in their physical appearance and origin. While the compass-spins (pseudodipoles) as introduced in Ref. [4] align themselves along the bond direction as real compasses do (hence the name), the spins in the Kitaev honeycomb model tend rather to avoid the bond directions. Placed on a honeycomb lattice, the bond-directional compasses would feel much less frustrated than the Kitaev spins, and show "order-from-disorder" behavior instead. As to the physical origin, the compass-type and Kitaev-type spin anisotropy terms arise in compounds with distinct chemical bonding geometries-corner-shared [16,9] and edge-shared [6,9] structures, correspondingly.
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    • 3 is a manifestation of the other anisotropy terms beyond the "Heisenberg plus Kitaev" spin model
    • 3 is a manifestation of the other anisotropy terms beyond the "Heisenberg plus Kitaev" spin model.
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    • note
    • Ref. [46] has estimated the angle a ≃ 44° based on the fits that did not account for a trigonal field splitting. Positive (negative) Δ values may decrease (increase) the actual value of a from this estimate.
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