论文标题
(111)Permalloy/PT多层剪裁界面混合和磁性
Tailoring interface mixing and magnetic properties in (111) Permalloy/Pt multilayers
论文作者
论文摘要
我们介绍了由20个重复的15 $Å厚的pomperaly ni $ _ {80} $ fe $ _ {20} $组成的多层的沉积和表征。 \%(py)和5 $Å$ pt。样品是通过两种不同的溅射沉积方法(即DC磁控溅射(DCM)和高功率脉冲磁控溅射(HIPIMS)分别代表膜形成材料的低和中度电离通量分数,以用于PY层的沉积。研究了底物粗糙度,工作气压和溅射功率对膜内部单轴磁各向异性的影响。多层的特征是X射线反射率和衍射,以及磁光kerr效应(MOKE)。结果表明,HIPIMS沉积会产生具有独特表面粗糙度的多层,而不管底物表面粗糙度如何。由DCMS和HIPIMS沉积制备的多层构成的质地强(111)与薄膜平面正常。结果表明,与在溅射功率下执行的DCMS沉积相比,使用HIPIM进行沉积PY层的沉积会导致各个层之间的最小界面混合。这与HIPIM沉积的PY的光滑表面有关。然而,这种尖锐的界面会导致更高的矫正性和硬轴磁滞回路的开口,而与当前定义良好的平面单轴各向异性(即线性硬轴)相互混合的多层。与使用HIPIMS在相同条件下制备的PY/CU和PY/PY/CUPT多层的比较表明,在PY/PT的情况下,在PY/PT情况下获得了较差的平面单轴各向异性,这是由PY和PTY和PT之间的大晶状体不匹配引起的。展示界面混合的PY/PT多层具有更轻松的界面,因此表现出可以忽略不计的磁盘,并且更好地定义了各向异性。
We present deposition and characterization of multilayers consisting of 20 repetitions of 15 $Å$ thick permalloy Ni$_{80}$Fe$_{20}$ at. \% (Py) and 5 $Å$ Pt. The samples were prepared by two different sputter deposition methods, namely dc magnetron sputtering (dcMS) and high power impulse magnetron sputtering (HiPIMS), that represent low and moderate ionized flux fraction of the film forming material, respectively, for deposition of the Py layers. The effect of substrate roughness, working gas pressure and sputter power on the in-plane uniaxial magnetic anisotropy of the films are studied. The multilayers were characterized by X-ray reflectivity and diffraction, and by magneto-optical Kerr effect (MOKE). It is shown that HiPIMS deposition produces multilayers with unique surface roughness regardless of the substrate surface roughness. Multilayers prepared by both dcMS and HiPIMS deposition present a strong (111) texture normal to the film plane. The results show that utilizing HiPIMS for deposition of the Py layer leads to a minimum interface mixing between individual layers compared to dcMS deposition performed at sputter power. This is associated with the smooth surface of Py deposited by HiPIMS. However, this sharp interface results in higher coercivity and an opening in the hard axis hysteresis loops while multilayers with intermixing present well defined in-plane uniaxial anisotropy i.e. a linear hard axis. Comparison with Py/Cu and Py/CuPt multilayers, prepared under identical conditions using HiPIMS, suggests that poor in-plane uniaxial anisotropy is obtained in the Py/Pt case, caused by the inverse magnetostriction arising from the large lattice mismatch between Py and Pt. The Py/Pt multilayers that exhibit interface mixing have a more relaxed interface and thus presents negligible inverse magnetostriction and have better defined anisotropy.