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Structure and magnetic properties of Mn/Pt(110)-(1 X 2): A joint x-ray diffraction and theoretical study

机译:Mn / Pt(110)-(1 X 2)的结构和磁性能:联合X射线衍射和理论研究

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The growth of a Mn submonolayer on Pt(110)-(1 X 2) 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 (1 X 2) 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 (2 X 1) symmetry. It exhibits mixed dense rows where Pt and Mn sites alternate, as in bulk Pt_3Mn. The top layer is corrugated for both the (1 X 2) and (2 X 1) surfaces, with Mn lying 0.19 ± 0.03 and 0.16 ± 0.02 A above the Pt site, respectively. A Pt_3Mn-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(2 X 2) arrangements were found. Theoretical calculations were performed for (1 X 2), c(2 X 2), and (2 X 1) PtMn two-dimensional (2D) alloys on Pt(110). Among them, the latter was found to be the ground state. Both the (1 X 2) and (2 X 1) surface alloys form antiferromagnetic (AF) Mn chains running in the [110] and [001] directions, respectively. The ordering within the surface layer switches to ferromagnetic (F) for a 5-ML-thick Pt_3Mn(110) film albeit with a surface structure quite identical to the (2 X 1) 2D case. The magnetic moment per Mn atom at the surface is close to 4 μ_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)-(1 X 2)上的生长。在室温下,Mn填充干净基材缺失的行结构的空行。以0.5 ML(单层)的覆盖率,形成(1 X 2)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(2 X 1)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Pt_3Mn。顶层在(1 X 2)和(2 X 1)表面均为波纹状,Mn分别位于Pt部位上方0.19±0.03和0.16±0.02A。当退火3-ML厚的Mn膜时,形成Pt_3Mn状平板。观察到的对称性与发现c(2 X 2)排列的NiMn和CuMn表面不一致。在Pt(110)上对(1 X 2),c(2 X 2)和(2 X 1)PtMn二维(2D)合金进行了理论计算。其中,后者被发现是基态。 (1 X 2)和(2 X 1)表面合金均形成分别沿[110]和[001]方向延伸的反铁磁(AF)Mn链。对于表面厚度与(2 X 1)2D情况完全相同的5ML厚Pt_3Mn(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原子的磁矩在所有情况下都接近4μB,这是在类似的金属-Mn表面合金中发现的最大值:与表面波纹和Mn体积直接相关,正如已经观察到的。其他锰基表面合金。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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