ePrints@IIScePrints@IISc Home | About | Browse | Latest Additions | Advanced Search | Contact | Help

Topological magnons in a kagome-lattice spin system with &ITXXZ&IT and Dzyaloshinskii-Moriya interactions

Seshadri, Ranjani and Sen, Diptiman (2018) Topological magnons in a kagome-lattice spin system with &ITXXZ&IT and Dzyaloshinskii-Moriya interactions. In: PHYSICAL REVIEW B, 97 (13).

[img] PDF
Phy_Rev-B_97-13_134411_2018.pdf - Published Version
Restricted to Registered users only

Download (2MB) | Request a copy
Official URL: http://dx.doi.org/10.1103/PhysRevB.97.134411

Abstract

We study the phases of a spin system on the kagome lattice with nearest-neighbor XXZ interactions with anisotropy ratio Delta and Dzyaloshinskii-Moriya interactions with strength D. In the classical limit where the spin S at each site is very large, we find a rich phase diagram of the ground state as a function of Delta and D. There are five distinct phases which correspond to different ground-state spin configurations in the classical limit. We use spin-wave theory to find the bulk energy bands of the magnons in some of these phases. We also study a strip of the system which has infinite length and finite width; we find states which are localized near one of the edges of the strip with energies which lie in the gaps of the bulk states. In the ferromagnetic phase in which all the spins point along the +(z)over-cap or -(z)over-cap direction, the bulk bands are separated from each other by finite energy gaps. This makes it possible to calculate the Berry curvature at all momenta, and hence the Chern numbers for every band; the number of edge states is related to the Chern numbers. Interestingly, we find that there are four different regions in this phase where the Chern numbers are different. Hence there are four distinct topological phases even though the ground-state spin configuration is identical in all these phases. We calculate the thermal Hall conductivity of the magnons as a function of the temperature in the above ferromagnetic phase; we find that this can distinguish between the various topological phases. These results are valid for all values of S. In the other phases, there are no gaps between the different bands; hence the edge states are not topologically protected.

Item Type: Journal Article
Publication: PHYSICAL REVIEW B
Publisher: AMER PHYSICAL SOC, ONE PHYSICS ELLIPSE, COLLEGE PK, MD 20740-3844 USA
Additional Information: Copy right for this article belong to AMER PHYSICAL SOC, ONE PHYSICS ELLIPSE, COLLEGE PK, MD 20740-3844 USA
Department/Centre: Division of Physical & Mathematical Sciences > Centre for High Energy Physics
Date Deposited: 04 May 2018 18:48
Last Modified: 04 May 2018 18:48
URI: http://eprints.iisc.ac.in/id/eprint/59715

Actions (login required)

View Item View Item