Selective flattening of magnon bands in kagome-lattice ferromagnets with Dzyaloshinskii-Moriya interaction  

作　　者：YuHeng Xing FuSheng Ma LiFa Zhang ZhenYu Zhang 

机构地区：[1]NNU-SULI Thermal Energy Research Center(NSTER)Center for Quantum Transport and Thermal Energy Science(CQTES),School of Physics and Technology,Nanjing Normal University,Nanjing 210023,China [2]International Center for Quantum Design of Functional Materials(ICQD),Hefei National Laboratory for Physical Sciences at Microscale,and Synergetic Innovation Center of Quantum Information and Quantum Physics,University of Science and Technology of China,Hefei 230026,China

出　　处：《Science China(Physics,Mechanics & Astronomy)》2020年第10期98-104,共7页中国科学：物理学、力学、天文学（英文版）

基　　金：supported by the National Natural Science Foundation of China(Grant Nos.11890703,11574154,61434002,11704191,and11634011);the National Program on Key Basic Research Project(Grant No.2014CB921103);the National Key Research and Development Program of China(Grant No.2017YFA0303500)。

摘　　要：There is growing interest in revealing exotic properties of collective spin excitations in kagome-lattice ferromagnets such as magnon Hall effects,topological magnon insulators,and flat magnon bands.Using the well-established nearest-neighbor Heisenberg ferromagnet model with Dzyaloshinskii-Moriya interaction(DMI),in this study we uncover intriguing new aspects in the selectivity and topology of flat magnon bands.Among the three magnon bands(except for the top one,which is flat in the absence of DMI),we observe that each of the three bands can be selectively flattened at the critical DMI of D=±√3 J/3 and D=±√3 J.With a general DMI,the magnon bands become non-flat;however,there are nested lines that create a David star pattern for all three magnon bands whose flatness is robust during changing exchange coupling or DMIs.Contrary to prevailing belief,we show that each of the three flat bands is actually topologically trivial at critical DMIs.Furthermore,we show that while the middle band remains topologically trivial,for the other two bands,D=0 corresponds to the topological phase transition where their Chern numbers get interchanged;when D=±√3 J,the system undergoes a phase transition to the nonferromagnetic state.These central findings increase our understanding of spin excitations for future magnonics applications.

关 键 词：flat magnon bands kagome lattice FERROMAGNET Dzyaloshinskii-Moriya interaction 

分 类 号：O482.5[理学—固体物理]