Low energy magnetic excitations in Spin-1 honeycomb antiferromagnet Na<sub>3</sub>Ni<sub>2</sub>BiO<sub>6</sub> using Far-Infrared Magnetospectroscopy.
ORAL
Abstract
The spin-½ Kitaev model on a honeycomb lattice is an exactly solvable model for realizing Quantum Spin Liquids (QSLs). The model has been extensively studied in effective spin-½ compounds such as 5d7 Iridates and 4d7 a-RuCl3, with recent attention on Co-based systems (3d7). We extend this investigation to the 3d8 Nickel-based compound Na3Ni2BiO6, a spin-1 antiferromagnet with a honeycomb lattice structure that exhibits Kitaev physics.[1]
We map the low-energy magnetic excitations of the compound utilizing Far-Infrared Magnetospectroscopy (FIRMS), with energy signatures visible down to 10 cm-1, in both Faraday and Voigt configurations in magnetic fields up to 17.5T. In the Voigt configuration, we observe a spin-flop transition, marked by a sharp change in optical weight distribution and a kink in a magnon mode. In the Faraday configuration, we observe a magnon mode along with a gradual optical weight transfer when the material gets into fully spin polarized state. We also compare our experimental results with linear spin wave calculations. Our FIRMS measurements show agreement with the B-T phase diagram present in the literature.[1]
[1] Shangguan, Y., Bao, S., Dong, ZY. et al. Nat. Phys. 19, 1883 (2023).
We map the low-energy magnetic excitations of the compound utilizing Far-Infrared Magnetospectroscopy (FIRMS), with energy signatures visible down to 10 cm-1, in both Faraday and Voigt configurations in magnetic fields up to 17.5T. In the Voigt configuration, we observe a spin-flop transition, marked by a sharp change in optical weight distribution and a kink in a magnon mode. In the Faraday configuration, we observe a magnon mode along with a gradual optical weight transfer when the material gets into fully spin polarized state. We also compare our experimental results with linear spin wave calculations. Our FIRMS measurements show agreement with the B-T phase diagram present in the literature.[1]
[1] Shangguan, Y., Bao, S., Dong, ZY. et al. Nat. Phys. 19, 1883 (2023).
*This work is supported by the Department of Energy, Basic Energy Sciences, under Contract No. DE- FG02-07ER46451 and No. DE-SC-0020254 (L.C. & H.Z.). The National High Magnetic Field Laboratory is supported by the NSF through DMR-2128556 and the State of Florida.
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Presenters
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Sumedh Rathi
- Georgia Institute of Technology