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Theoretical formalism for collective spin-wave edge excitations in arrays of dipolarly interacting magnetic nanodots

机译:中国集体自旋波边激励的理论形式   偶极相互作用的磁性纳米点阵列

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摘要

A general theory of edge spin wave excitations in semi-infinite and finiteperiodic arrays of magnetic nanodots existing in a spatially uniformmagnetization ground state is developed. The theory is formulated using aformalism of multi-vectors of magnetization dynamics, which allows one to studyedge excitations in arrays having arbitrary complex primitive cells and latticegeometry. The developed formalism can describe edge excitations localized bothat the physical edges of the array and at the internal "domain walls"separating array regions existing in different static magnetization states.Using a perturbation theory in the framework of the developed formalism it ispossible to calculate damping of edge modes and their excitation by externalvariable magnetic fields. The theory is illustrated on the followingpractically important examples: (i) calculation of the FMR absorption in afinite nanodot array having the shape of a right triangle, (ii) calculation ofnonreciprocal spin wave spectra of edge modes, including modes at the physicaledges of an array and modes at the domain walls inside an array, (iii) study ofthe influence of the domain wall modes on the FMR spectrum of an array existingin a non-ideal chessboard antiferromagnetic ground state.
机译:提出了在空间均匀磁化基态下存在的磁性纳米点的半无限和有限周期阵列中的边缘自旋波激发的一般理论。该理论是用磁化动力学的多个向量的形式主义来表述的,它可以使人们研究具有任意复杂原始单元和晶格几何形状的阵列中的边缘激发。发达的形式主义可以描述位于阵列的物理边缘和内部“畴壁”处的边缘激励,这些边缘激励将存在于不同静态磁化状态的阵列区域分开。在发达的形式主义的框架中使用微扰理论,有可能计算阻尼系数。边缘模式及其外部可变磁场的激发。在以下实际的重要示例中说明了该理论:(i)计算具有直角三角形形状的无限纳米点阵列中的FMR吸收,(ii)计算边缘模式(包括阵列物理边缘的模式)的不可逆自旋波谱(iii)研究畴壁模态对存在于非理想棋chess反铁磁基态的阵列FMR谱的影响。

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