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首页> 外文期刊>Physical Review, B. Condensed Matter >Metal oxide heteroepitaxy: Stranski-Krastanov growth for iron oxides on Pt(111)
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Metal oxide heteroepitaxy: Stranski-Krastanov growth for iron oxides on Pt(111)

机译:金属氧化物异质外延:Pt(111)上铁氧化物的Stranski-Krastanov生长

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The epitaxial growth of iron oxide films on Pt(lll) substrates was investigated by scanning tunneling microscopy and low-energy electron diffraction. The film growth was accomplished by repeated cycles of iron deposition and subsequent oxidation at p(O-2)= 10(-6) mbar. For oxidation temperatures of 870 K second and third FeO(lll) layers grow layer by layer, whereas for oxidation temperatures of 1000 K only one FeO(lll) monolayer is formed. On top of the FeO(lll) films a homogeneous nucleation of Fe3O4(111) islands takes place, resulting in a Stranski-Krastanov growth for iron oxides on Pt(lll). The islands grow in the Fe3O4 bulk structure laterally much faster than vertically, forming hat platelets with heights up to 100 Angstrom and hexagonal and triangular basal planes 1000-5000 Angstrom in diameter. The islands only expose low index ((1) over bar 11) and {2 (1) over bar (1) over bar} facet planes, and their growth can be described by an Ostwald ripening mechanism that takes place during each oxidation cycle. Eventually the islands coalesce and form smooth Fe3O4(111) films at least 150 Angstrom thick. The atomic and mesoscopic surface roughness bf these films depends on the growth temperature, where the latter ranges between 40 and 100 Angstrom on a length scale of mu m. By a high-pressure oxidation at p(O-2) = 10(-1) mbar the Fe3O4(111) films were transformed into well-ordered alpha-Fe2O3(0001) films with similar surface morphologies. In all oxide phases formed the hexagonal oxygen (Ill)planes are aligned to the Pt(111) substrate surface lattice. The film growth is discussed in terms of surface and interfacial energies, oxidation and growth kinetics, as well as thermodynamic stability ranges of the: different oxide phases. [S0163-1829(99)11007-5]. [References: 56]
机译:通过扫描隧道显微镜和低能电子衍射研究了Pt(III)衬底上氧化铁膜的外延生长。通过重复的铁沉积循环和随后在p(O-2)= 10(-6)mbar的氧化来完成膜的生长。对于870 K的氧化温度,第二和第三FeO(III)层逐层生长,而对于1000 K的氧化温度,仅形成一个FeO(III)单层。在FeO(III)膜的顶部,发生了Fe3O4(111)岛的均匀成核,从而导致Pt(III)上的铁氧化物的Stranski-Krastanov生长。这些岛在Fe3O4块状结构的横向生长比垂直生长快得多,形成了高度高达100埃的帽状小板,直径为1000-5000埃的六边形和三角形基面。这些岛仅暴露低折射率(在条11上的(1)和在条}面上的条(1)上的{2(1)),并且它们的生长可以通过在每个氧化循环期间发生的Ostwald成熟机制来描述。最终,这些岛聚结并形成至少150埃厚的光滑Fe3O4(111)膜。这些膜的原子表面和介观表面粗糙度取决于生长温度,生长温度在μm的长度范围内在40至100埃之间。通过在p(O-2)= 10(-1)mbar下进行高压氧化,将Fe3O4(111)膜转变为表面形貌相似的有序α-Fe2O3(0001)膜。在所有形成的氧化物相中,六角形氧(III)平面与Pt(111)衬底表面晶格对齐。根据表面和界面能,氧化和生长动力学以及不同氧化物相的热力学稳定性范围来讨论膜的生长。 [S0163-1829(99)11007-5]。 [参考:56]

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