APS March Meeting 2015
Volume 60, Number 1
Monday–Friday, March 2–6, 2015;
San Antonio, Texas
Session M53: Invited Session: Iridium-Based Kitaev Materials
11:15 AM–2:15 PM,
Wednesday, March 4, 2015
Room: Grand Ballroom C3
Sponsoring
Unit:
GMAG
Chair: Leon Balents, Kavli Institute of Theoretical Physics
Abstract ID: BAPS.2015.MAR.M53.2
Abstract: M53.00002 : Magnetic and Orbital Excitations in $\alpha $-A$_{2}$IrO$_{3}$ (A $=$ Li, Na) Probed by Resonant Inelastic X-ray Scattering
11:51 AM–12:27 PM
Preview Abstract
Abstract
Author:
James Clancy
(University of Toronto)
The honeycomb lattice iridates Na$_{2}$IrO$_{3}$ and
Li$_{2}$IrO$_{3}$ are two of the most promising candidates
for the experimental realization of Kitaev-like physics. Although the
formation of long-range magnetic order (T$_{N} $ $\sim $ 15 K) excludes
a pure Kitaev model, there are many extended Kitaev models (which include
contributions such as isotropic Heisenberg exchange, further-neighbor
interactions, symmetric off-diagonal exchange, and structural distortions)
that may be relevant to these materials. We have performed high-resolution
Ir L$_{3}$-edge resonant inelastic x-ray scattering (RIXS)
measurements to investigate the excitation spectra of
Na$_{2}$IrO$_{3}$ and Li$_{2}$IrO$_{3}$.
In Na$_{2}$IrO$_{3}$, we observe a new branch of
dispersive magnetic excitations, which reaches a maximum energy of $\sim $35 meV at
the $\Gamma $ point [1]. This mode is distinct from the low energy ($\sim $6 meV)
magnon mode observed in previous inelastic neutron scattering measurements
[2], and implies the presence of a significant bond-dependent Kitaev
interaction. The d-d excitations in Na$_{2}$IrO$_{3}$ and
Li$_{2}$IrO$_{3}$ reveal important information about
crystal electric field effects, and the potential impact of trigonal and
monoclinic structural distortions [3]. New developments in high pressure
RIXS allow us to study the evolution of these excitations up to 6 GPa,
providing insight into future prospects for tuning Kitaev interactions via
applied pressure.\\[4pt]
Work performed in collaboration with H. Gretarsson, J.A. Sears, Y.-J. Kim
(University of Toronto), M.H. Upton, J. Kim, Y. Ding, A.H. Said, D. Casa, T.
Gog (Argonne National Laboratory), S. Desgreniers (University of Ottawa), Y.
Singh (IISER Mohali), S. Manni, P. Gegenwart (University of Gottingen), X.
Liu, J.P. Hill (Brookhaven National Laboratory), V.M. Katukuri, L. Hozoi, J.
van den Brink (IFW Dresden).\\[4pt]
[1] H. Gretarsson et al, Phys. Rev. B 87, 220407(R) (2013).\\[0pt]
[2] S.K. Choi et al, Phys. Rev. Lett. 108, 127204 (2012).\\[0pt]
[3] H. Gretarsson et al, Phys. Rev. Lett. 110, 076402 (2013).
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2015.MAR.M53.2