亚100nm自旋波在磁导波导中的直接观测

N. Träger, P. Gruszecki, F. Lisiecki, J. Förster, M. Weigand, P. Kuświk, J. Dubowik, G. Schütz, M. Krawczyk, J. Gräfe
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Here, we use scanning transmission x-ray microscopy (STXM, MAXYMUS@BESSY II) with magnetic contrast and a spatial and temporal resolution of 18 nm and 35 ps respectively to investigate such wave-guides. These were structured in 50 nm thin Py stripes with a width of 350, 700 or 1400 nm and a length of 11 μm. A coplanar waveguide (Cr/Cu/Al) was deposited on top to allow RF excitation of spin waves in the structures (cf.Fig. 1 for a schematic sketch and a microscopy image). After time-domain STXM acquisition of the magnetization movie under RF excitation, a temporal Fourier transformation is performed to gain the spatial distribution of the spin wave amplitude and phase. This is shown exemplary in Fig. 2(a) for a 1400 nm wide Py stripe under CW excitation at 4.6 GHz and in an external field of 15 mT applied parallel to the long axis of the wave-guide (BV configuration). One can clearly observe that highly directed spin waves emerge from the edges of the wave-guide [5]. 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引用次数: 0

摘要

在磁振学研究中,由自旋波介导的数据处理能力是目前CMOS以外数据处理技术的兴趣所在,有前途的非布尔计算算法或多数门取代了几十个CMOS晶体管,使其成为下一级计算的令人兴奋的候选物[1-3]。此外,由于磁振子在技术相关无线电频率上的波长较短,因此更小的结构元件和各种设备的小型化将成为可能[4]。然而,对于磁逻辑运算,可靠的自旋波波导是必不可少的。在这里,我们使用扫描透射x射线显微镜(STXM, MAXYMUS@BESSY II),磁性对比,空间和时间分辨率分别为18 nm和35 ps来研究这种波导。它们被构造成50 nm的细Py条纹,宽度为350、700或1400 nm,长度为11 μm。共面波导(Cr/Cu/Al)沉积在顶部,允许自旋波在结构中被射频激发(参见图2)。1为示意图草图和显微镜图像)。对射频激励下的磁化膜进行时域STXM采集后,进行时域傅里叶变换,得到自旋波振幅和相位的空间分布。如图2(a)所示,在4.6 GHz连续波激励下,在平行于波导长轴(BV配置)的15mt外场中,1400 nm宽的Py条纹显示了这一点。人们可以清楚地观察到,高度定向的自旋波从波导的边缘出现[5]。由于两侧的发射,沿Py条纹形成驻波。为了量化自旋波的特性,我们进行了空间傅里叶变换,得出了波矢量的k空间分布,如图2(b)所示。图中,在中心的直流电峰旁边,有两个组分突出显示出这些微结构充当多模波导。第一种自旋波模式的波矢量k1 = 4.7 μm-1,对应波长为$\lambda _{1} \quad =210$ nm;第二种自旋波模式的波矢量k为$\mathrm {k}_{2} \quad = 10.5 \mu \mathrm {m}^{-1}$。因此,我们能够在显微镜下观察到波长为$\lambda _{2} =95$ nm的自旋波,并在实验上突破100 nm的极限。此外,我们还对不同波导宽度的激发频率进行了系统的变化,并施加了外场。通过改变这些参数,波长和传播方向被调谐,也表明自旋波的对角线和弯曲传播,类似于光在渐变折射率光纤中的传播。此外,我们通过使用突发激励方案重建了数据传输场景,即四个周期的射频激励之后是一个自由衰减时间。因此,同时激发的多个模式被Py波导携带。它们相互交错而不互相干扰,进一步证实了波导的多模特性。令人惊讶的是,这些模式在衰减时间内不会分散频率,使该系统成为数据传输的理想候选者。总之,我们用时间分辨STXM直接观测到了Py波导中低于100 nm的自旋波。发现简单波导能够同时非色散地携带多个模式。因此,它们是逻辑元件之间基于磁振子的数据传输的理想候选者,并为未来的技术发展提供了有希望的基础。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Direct Observation of Sub-100 nm Spin Wave Propagation in Magnonic Wave-Guides
In magnonics research, capabilities of data processing mediated by spin waves are of current interest for beyond-CMOS data processing technologies, promising non-Boolean computing algorithms or majority gates substituting several tens of CMOS transistors and making this an exciting candidate for next level computing [1–3]. Furthermore, due to the short wavelength of magnons at technological relevant radio frequencies, smaller structural elements and, thus, miniaturization of various devices will be possible [4]. However, for magnonic logic operations, reliable spin wave guides are indispensable. Here, we use scanning transmission x-ray microscopy (STXM, MAXYMUS@BESSY II) with magnetic contrast and a spatial and temporal resolution of 18 nm and 35 ps respectively to investigate such wave-guides. These were structured in 50 nm thin Py stripes with a width of 350, 700 or 1400 nm and a length of 11 μm. A coplanar waveguide (Cr/Cu/Al) was deposited on top to allow RF excitation of spin waves in the structures (cf.Fig. 1 for a schematic sketch and a microscopy image). After time-domain STXM acquisition of the magnetization movie under RF excitation, a temporal Fourier transformation is performed to gain the spatial distribution of the spin wave amplitude and phase. This is shown exemplary in Fig. 2(a) for a 1400 nm wide Py stripe under CW excitation at 4.6 GHz and in an external field of 15 mT applied parallel to the long axis of the wave-guide (BV configuration). One can clearly observe that highly directed spin waves emerge from the edges of the wave-guide [5]. Due to the emission from both edges, a standing wave forms along the Py stripe. To quantify the spinwave properties a spatial Fourier transformation was performed to derive the k-space distribution of the wave vectors, which is shown in Fig. 2(b). Here, two components stand out beside the DC peak in the center showing that these microstructures act as multimode wave-guide. The first spin-wave modes has a wave vector k1 = 4.7 μm-1, which corresponds to a wavelength of $\lambda _{1} \quad =210$ nm, and a second mode with a k-vector $\mathrm {k}_{2} \quad = 10.5 \mu \mathrm {m}^{-1}$ is visible. Thus, we are able to microscopically observe a spin-wave with a wavelength of $\lambda _{2} =95$ nm and experimentally break through the 100 nm limit. Furthermore, we have performed a systematic variation of excitation frequency and applied external field for the different wave-guide widths. By varying these parameters, the wavelength as well as the propagation direction are tuned, indicating also diagonal and curved propagating of spin-waves that resembles the propagation of light in a graded-index fiber. Additionally, we recreated a data transmission scenario by using a Burst excitation scheme, i.e. four periods of RF excitation followed by a free decay time. Thereby, simultaneously excited multiple modes are carried by the Py wave-guide. They are interleaving without disrupting each other, further confirming the multimode properties of the wave-guide. Surprisingly, these modes did not disperse in frequency during the decay time making this system an ideal candidate for data transmission. In summary, we have directly observed sub-100 nm spin waves in a Py wave-guide by time-resolved STXM. The simple wave-guides were found to be able to non-dispersively carry multiple modes simultaneously. Thus, they are ideal candidates for magnon based data transmission between logic elements and provide a promising basis for future technology developments.
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