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APS -Annual Meeting of the APS Four Corners Section- Event - Parallel pumping of a ferromagetic nanostripe: confinement quantization and off-resonance driving

机译:APS-APS四角分会年会-活动-铁磁纳米带的平行泵送:限制量化和失谐驱动

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The parametric excitation of spin waves in a rectangular, ferromagnetic nanowire in the parallel pump configuration and with applied field along the long axis of the wire is studied theoretically, using a semi-classical and semi-analytic Hamiltonian approach. We find that as a function of static applied field strength, there are jumps in the pump power needed to excite thermal spin waves. At these jumps, there is the possibility to non-resonantly excite spin waves near $k_z=0$. Spin waves with negative or positive group velocity and with different standing wave structure across the wire width can be excited by tuning the applied field. By using a magnetostatic Green's function that depends on both the nanowire's width and thickness -- rather than just its aspect ratio -- we also find that the threshold field strength varies considerably for nanowires with the same aspect ratio but of different sizes, in contrast to previous work.
机译:理论上,使用半经典半解析汉密尔顿方法,研究了平行泵浦结构的矩形铁磁纳米线中自旋波的参量激发,并沿线的长轴施加了电场。我们发现,作为静态施加场强的函数,激发热自旋波所需的泵浦功率会发生跳跃。在这些跳跃中,有可能非共振地激发$ k_z = 0 $附近的自旋波。可以通过调整外加磁场来激发具有负或正群速度并且在整个导线宽度上具有不同驻波结构的自旋波。通过使用取决于纳米线宽度和厚度的静磁格林函数-不仅取决于其长宽比-我们还发现,与长宽比相同但尺寸不同的纳米线相比,阈值场强变化很大之前的工作。

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