Topological chiral magnonic edge mode in a magnonic crystal

Ryuichi Shindou, Ryo Matsumoto, Shuichi Murakami, and Jun-ichiro Ohe
Phys. Rev. B 87, 174427 – Published 24 May 2013

Abstract

Topological phases have been explored in various fields in physics such as spintronics, photonics, liquid helium, correlated electron system, and cold-atomic system. This leads to the recent foundation of emerging materials such as topological band insulators, topological photonic crystals, and topological superconductors/superfluid. In this paper, we propose a topological magnonic crystal which provides protected chiral edge modes for magnetostatic spin waves. Based on a linearized Landau-Lifshitz equation, we show that a magnonic crystal with the dipolar interaction acquires a spin-wave volume-mode band with nonzero Chern integer. We argue that such magnonic systems are accompanied by the same integer numbers of chiral spin-wave edge modes within a band gap for the volume-mode bands. In these edge modes, the spin wave propagates in a unidirectional manner without being scattered backward, which implements novel fault-tolerant spintronic devices.

  • Received 6 April 2013

DOI:https://doi.org/10.1103/PhysRevB.87.174427

©2013 American Physical Society

Authors & Affiliations

Ryuichi Shindou*, Ryo Matsumoto, and Shuichi Murakami

  • Department of Physics, Tokyo Institute of Technology, 2-12-1 Ookayama, Meguro-ku, Tokyo, Japan

Jun-ichiro Ohe

  • Department of Physics, Toho University, 2-2-1 Miyama, Funabashi, Chiba, Japan

  • *Present address: International Center for Quantum Materials (ICQM), Peking University, No. 5 Yiheyuan Road, Haidian District, Beijing, 100871, China.

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Issue

Vol. 87, Iss. 17 — 1 May 2013

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