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Structure and magnetic properties of Mn/Pt(110)-(1x2): A joint x-ray diffraction and theoretical study

机译:Mn / Pt(110)-(1x2)的结构和磁性能:联合x射线衍射和理论研究

摘要

The growth of a Mn submonolayer on Pt(110)-(1x2) was studied by surface x-ray diffraction. At room temperature, Mn fills in the empty rows of the clean substrate's missing row structure. At a coverage of 0.5 ML (monolayer), a (1x2) surface alloy is formed, with alternating Pt and Mn dense rows. Upon annealing (or depositing at a substrate temperature of about 570 K), another surface alloy forms with a (2x1) symmetry. It exhibits mixed dense rows where Pt and Mn sites alternate, as in bulk Pt3Mn. The top layer is corrugated for both the (1x2) and (2x1) surfaces, with Mn lying 0.19 +/- 0.03 and 0.16 +/- 0.02 A above the Pt site, respectively. A Pt3Mn-like slab forms when annealing a 3-ML-thick Mn film. The observed symmetries are at variance with the NiMn and CuMn surfaces where c(2x2) arrangements were found. Theoretical calculations were performed for (1x2), c(2x2), and (2x1) PtMn two-dimensional (2D) alloys on Pt(110). Among them, the latter was found to be the ground state. Both the (1x2) and (2x1) surface alloys form antiferromagnetic (AF) Mn chains running in the [1 (1) over bar0] and [001] directions, respectively. The ordering within the surface layer switches to ferromagnetic (F) for a 5-ML-thick Pt3Mn(110) film albeit with a surface structure quite identical to the (2x1) 2D case. The magnetic moment per Mn atom at the surface is close to 4 mu(B), in all cases, among the largest values ever found in similar metal-Mn surface alloys: it is directly related to the surface corrugation and to the Mn volume as already observed for other Mn-based surface alloys. The magnetic order, F or AF, is strongly influenced by the local chemical environment of the Mn sites.
机译:通过表面X射线衍射研究了Mn亚单层在Pt(110)-(1x2)上的生长。在室温下,Mn填充干净基材缺失的行结构的空行。在0.5 ML(单层)的覆盖率下,形成(1x2)表面合金,并交替排列Pt和Mn致密行。退火后(或在约570 K的衬底温度下沉积),另一种表面合金形成(2x1)对称性。它显示出混合的密集行,其中Pt和Mn位置交替出现,就像散装的Pt3Mn。顶层在(1x2)和(2x1)表面均为波纹状,Mn分别位于Pt位置上方0.19 +/- 0.03和0.16 +/- 0.02A。退火3ML厚的Mn膜时会形成Pt3Mn状平板。观察到的对称性与发现c(2x2)排列的NiMn和CuMn表面不一致。在Pt(110)上对(1x2),c(2x2)和(2x1)PtMn二维(2D)合金进行了理论计算。其中,后者被发现是基态。 (1x2)和(2x1)表面合金均形成反铁磁(AF)Mn链,分别在[1(1)上沿bar0]和[001]方向延伸。对于表面厚度与(2x1)2D情况完全相同的5-ML厚Pt3Mn(110)膜,表面层内的顺序切换为铁磁(F)。在所有情况下,表面上每个Mn原子的磁矩都接近4μ(B),在类似金属-Mn表面合金中发现的最大值中:与表面波纹和Mn体积直接相关。对于其他基于Mn的表面合金已经观察到。磁阶F或AF受到Mn位的局部化学环境的强烈影响。

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