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Antiferromagnetic Mott insulating state in single crystals of the honeycomb lattice materialNa2IrO3
Abstract
We have synthesized single crystals of ${\text{Na}}_{2}{\text{IrO}}_{3}$ and studied their structure, transport, magnetic, and thermal properties using powder x-ray diffraction, electrical resistivity, isothermal magnetization $M$ versus magnetic field $H$, magnetic susceptibility $\ensuremath{\chi}$ versus temperature $T$, and heat capacity $C$ versus $T$ measurements. ${\text{Na}}_{2}{\text{IrO}}_{3}$ crystallizes in the monoclinic $C2/c$ (No. 15) type structure which is made up of Na and ${\text{NaIr}}_{2}{\text{O}}_{6}$ layers alternately stacked along the $c$ axis. The $\ensuremath{\chi}(T)$ data show Curie-Weiss behavior at high $T>200\text{ }\text{K}$ with an effective moment ${\ensuremath{\mu}}_{\text{eff}}=1.82(1){\ensuremath{\mu}}_{\text{B}}$ indicating an effective spin ${S}_{\text{eff}}=1/2$ on the ${\text{Ir}}^{4+}$ moments. A large Weiss temperature $\ensuremath{\theta}=\ensuremath{-}116(3)\text{ }\text{K}$ indicates substantial antiferromagnetic interactions between these ${S}_{\text{eff}}=1/2$, ${\text{Ir}}^{4+}$ moments. Anomalies in $\ensuremath{\chi}(T)$ and $C(T)$ data indicate that ${\text{Na}}_{2}{\text{IrO}}_{3}$ undergoes a transition into a long-range antiferromagnetically ordered state below ${T}_{\text{N}}=15\text{ }\text{K}$. The magnetic entropy at ${T}_{\text{N}}$ is only about 20% of what is expected for ${S}_{\text{eff}}=1/2$ moment ordering. The reduced entropy and the large ratio $\ensuremath{\theta}/{T}_{N}\ensuremath{\approx}8$ suggest geometrical magnetic frustration and/or low-dimensional magnetic interactions in ${\text{Na}}_{2}{\text{IrO}}_{3}$. In plane resistivity measurements show insulating behavior. This behavior together with the local-moment magnetism indicates that bulk ${\text{Na}}_{2}{\text{IrO}}_{3}$ is a Mott insulator.
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Cites
Z 2 Topological Order and the Quantum Spin Hall Effect
Kane, C. L., & Mele, E. J. (2005) · Physical Review Letters · doi:10.1103/physrevlett.95.146802 · Cited by 6,460
Anyons in an exactly solved model and beyond
Kitaev, A. (2006) · Annals of Physics · doi:10.1016/j.aop.2005.10.005 · Cited by 5,245
Cited by
Wan, X., Turner, A. M., Vishwanath, A., & Savrasov, S. Y. (2011) · Physical Review B · doi:10.1103/physrevb.83.205101 · Cited by 4,718
Long-range magnetic ordering in Na2IrO3
Liu, X., Berlijn, T., Yin, W.-G., Ku, W., Tsvelik, A., Kim, Y.-J., Gretarsson, H., Singh, Y., Gegenwart, P., & Hill, J. P. (2011) · Physical Review B · doi:10.1103/physrevb.83.220403 · Cited by 353
Self-citationSuccessive magnetic phase transitions inα−RuCl3: XY-like frustrated magnet on the honeycomb lattice
Kubota, Y., Tanaka, H., Ono, T., Narumi, Y., & Kindo, K. (2015) · Physical Review B · doi:10.1103/physrevb.91.094422 · Cited by 317
Metadata
- Authors
- Singh, Y., & Gegenwart, P.
- Venue
- Physical Review B
- Publisher
- American Physical Society (APS)
- Published
- 2010-08-12
- Volume
- 82
- Issue
- 6
- ISSN
- 1098-0121 (ISSN-L)
- 1550-235X
- OpenAlex
- W2962821121
- Cited by
- 649
- References
- 2
- FWCI
- 14.29
- Type
- journal article
- Language
- en
- Open access
- closed
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