Department of Applied Physics, Osaka University, 2-1 Yamada-oka Suita, Osaka 565-0871, Japan.
J Phys Condens Matter. 2011 Oct 5;23(39):394207. doi: 10.1088/0953-8984/23/39/394207. Epub 2011 Sep 15.
First-principles calculations were performed to investigate magnetic phenomena in surface reactions involving O(2). We present two magnetized surface cases: (1) oxidation of paramagnetic Ag, and magnetic properties of the high coverage oxide phase, which correspond to a magnetic impurity superlattice on paramagnetic surfaces and (2) oxidation of ferromagnetic Pt, represented by the Pt layer on M (M = Fe and Co) relevant to the oxidation reduction reaction (ORR) on Pt, in relation to both fundamental and application interests. In the first case, we found that the dissociative adsorption of O(2), resulting in oxide phases in Ag(111), reveals interesting magnetic interactions. We note that the magnetic states are induced by the ferromagnetic superexchange interactions and Ruderman-Kittel-Kasuya-Yosida (RKKY) interactions. Specifically, the superlattice structures with short O-O distances have an effective ferromagnetic superexchange and RKKY interaction. In the second case, we found that a magnetic moment is induced on the Pt layer by the M substrate. The spin polarization of Pt-d states is due to hybridization with M-d states. The d-band center (ε(d)) of Pt (on M), is shifted downwards with respect to pure Pt. However, because of the spin polarization, the otherwise filled spin-down d(zz) orbital in paramagnetic pure Pt is shifted towards the Fermi level. This promotes π(z↑)-d(zz↓) interactions, which influences the O(2)-Pt interaction at O(2) far from the surface. Details and mechanisms of these two magnetic phenomena are discussed.
采用第一性原理计算研究了涉及 O(2)的表面反应中的磁现象。我们提出了两种磁化表面情况:(1)顺磁 Ag 的氧化,以及高覆盖率氧化物相的磁性,这对应于顺磁表面上的磁性杂质超晶格,(2)铁磁 Pt 的氧化,由与 Pt 上的氧化还原反应 (ORR) 相关的 M (M = Fe 和 Co) 上的 Pt 层表示,这与基础和应用兴趣有关。在第一种情况下,我们发现 O(2)的离解吸附导致 Ag(111)中的氧化物相,揭示了有趣的磁相互作用。我们注意到磁状态是由铁磁超交换相互作用和 Ruderman-Kittel-Kasuya-Yosida (RKKY) 相互作用诱导的。具体来说,具有短 O-O 距离的超晶格结构具有有效的铁磁超交换和 RKKY 相互作用。在第二种情况下,我们发现 M 衬底在 Pt 层上诱导出磁矩。Pt-d 态的自旋极化是由于与 M-d 态的杂化。Pt (在 M 上)的 d 带中心 (ε(d)) 相对于纯 Pt 向下移动。然而,由于自旋极化,原本在顺磁纯 Pt 中填满的自旋向下 d(zz)轨道被移向费米能级。这促进了 π(z↑)-d(zz↓)相互作用,从而影响了远离表面的 O(2)-Pt 相互作用。讨论了这两种磁现象的细节和机制。