Polymerization and decomposition ofC60on Pt(111) surfaces

X射线光电子能谱 俄歇电子能谱 低能电子衍射 退火(玻璃) 结晶学 电子光谱学 分析化学(期刊) 单层 材料科学 物理 原子物理学 电子衍射 化学 核磁共振 衍射 纳米技术 热力学 光学 色谱法 核物理学
作者
Nathan S. Swami,Hong He,Bruce E. Koel
出处
期刊:Physical review [American Physical Society]
卷期号:59 (12): 8283-8291 被引量:44
标识
DOI:10.1103/physrevb.59.8283
摘要

The interaction of ${\mathrm{C}}_{60}$ with Pt(111) was investigated at submonolayer, monolayer, and multilayer coverages by Auger electron spectroscopy, x-ray photoelectron spectroscopy (XPS), UV photoelectron spectroscopy (UPS), high-resolution electron-energy-loss spectroscopy (HREELS), and low-energy electron diffraction studies. The Pt(111) surface strongly affects the thermal decomposition of ${\mathrm{C}}_{60}.$ At submonolayer coverages, ${\mathrm{C}}_{60}$ is polymerized on Pt(111) at $T>~300\mathrm{K}$ as was evident from UPS spectra that show a 0.4--0.5 eV shift towards ${E}_{F}$ for the VB features, in comparison to that of multilayer ${\mathrm{C}}_{60}$ films on Pt(111). The polymerization was most clearly evident in HREELS for ${\mathrm{C}}_{60}$ films on Pt(111) annealed to 700 K in the presence of O adatoms or Sn, as seen by the rise in intensity of the ${A}_{g}(2)$ derived mode at 1460 ${\mathrm{cm}}^{\mathrm{\ensuremath{-}}1}$. As a result, annealing multilayer ${\mathrm{C}}_{60}$ films on Pt(111) to $T>~600\mathrm{K}$ leads to a ${\mathrm{C}}_{60}$ adlayer that is quite different from 1 ML ${\mathrm{C}}_{60}/\mathrm{P}\mathrm{t}(111).$ On annealing ${\mathrm{C}}_{60}$ films on Pt(111) to 900 K, graphite domains appear on the surface and complete fragmentation occurs at 1050 K. HREELS, XPS, and UPS results comparing the ${\mathrm{C}}_{60}$ monolayer to the multilayer were used to study charge-transfer interactions between ${\mathrm{C}}_{60}$ and Pt(111). For 1 ML ${\mathrm{C}}_{60}/\mathrm{P}\mathrm{t}(111)$ at 300 K, UPS spectra show that the ${\mathrm{C}}_{60}$ valence-band features are shifted by about 0.4--0.5 eV towards ${E}_{F},$ while XPS studies show that the $\mathrm{C}(1s)$ core level is shifted by 0.4 eV to a lower binding energy and HREELS studies show that the ${T}_{1u}(1)$ mode is shifted down by 20 ${\mathrm{cm}}^{\mathrm{\ensuremath{-}}1}$ in comparison to multilayer coverages of ${\mathrm{C}}_{60}$ on Pt(111). Based on these shifts it was concluded that charge transfer of two electrons occurs from Pt(111) to monolayer ${\mathrm{C}}_{60}$ upon chemisorption. These charge-transfer interactions contribute to strong binding of the ${\mathrm{C}}_{60}$ monolayer and a low mobility for ${\mathrm{C}}_{60}$ molecules on the Pt(111) surface, which results in the growth of a disordered ${\mathrm{C}}_{60}$ film on Pt(111) at room temperature. Increased mobility of ${\mathrm{C}}_{60}$-derived species on the surface at 900 K results in the growth of an ordered film with a hexagonal structure.
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