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CO Adsorption on Pd(100) Revisited by Sum Frequency Generation: Evidence for Two Adsorption Sites in the Compression Stage

机译:总和频率产生再探讨Pd(100)上的CO吸附:压缩阶段两个吸附位的证据

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Sum frequency generation (SFG) and low-energy electron diffraction (LEED) have been used to revisit CO adsorption on Pd(100) from very low coverages up to saturation at 300 K. Below 0.5 ML, variations of SFG frequency and intensity with coverage are consistent with IRAS results from the literature. Novel observations are done above 0.5 ML, where the CO adlayer compression takes place. The existing compression model postulates the coexistence of compressed and uncompressed CO. We observe two bands in the spectral region of bridge sites and assign them to compressed and uncompressed CO. Both types of CO behave very differently: the molecular hyperpolarizability at compressed sites is smaller by a factor of 2 than at uncompressed sites. The frequency of uncompressed CO red-shifts during compression as the partial coverage decreases, while that of compressed CO continues to blue-shift as coverage increases. In the time domain, the coexistence of compressed and uncompressed sites results in oscillations in the decay of SFG intensity. A strong decrease from 690 to 222 fs of the phase relaxation time of uncompressed CO is observed during compression, indicating a stronger coupling to the substrate. These results are complemented by calculations of dipole-dipole interactions and DFT VASP calculations. While continuing blue-shift of compressed sites reflects a combination of increasing dipolar coupling and chemisorption change with coverage like below 0.5 ML, the very large red-shift amplitude of uncompressed CO indicates a large chemical contribution opposite to compressed CO. DFT VASP calculations allow us to follow the surface structure evolution from 0.5 to 0.67 ML and CO frequency changes with coverage. Pd atoms below compressed CO rows are pushed up, and compressed CO is tilted by 8- 9° with respect to the surface normal. A frequency split between compressed and uncompressed CO is found in agreement with experimental data. These results suggest that while compressed CO is less strongly bonded as compression proceeds the remaining uncompressed CO is more strongly bonded.
机译:总频率生成(SFG)和低能电子衍射(LEED)已用于重新覆盖CO在Pd(100)上的吸附,从极低的覆盖率到300 K饱和。0.5ML以下,SFG频率和强度随覆盖率而变化与文献中的IRAS结果一致。在0.5 ML以上进行了新的观察,发生了CO吸附层压缩。现有的压缩模型假定压缩和未压缩的CO共存。我们在桥位的光谱区域中观察到两个谱带,并将它们分配给压缩和未压缩的CO。两种类型的CO的行为都非常不同:压缩位处的分子超极化性较小是未压缩位置的2倍。随着部分覆盖率的降低,未压缩的CO的频率在压缩过程中发生红移,而随着覆盖率的增加,未压缩的CO的频率继续发生蓝移。在时域中,压缩和未压缩位置的共存会导致SFG强度衰减的振荡。在压缩过程中观察到未压缩CO的相弛豫时间从690 fs大幅降低到222 fs,这表明与基底的耦合更强。这些结果通过偶极-偶极相互作用的计算和DFT VASP计算得到补充。尽管压缩位点的持续蓝移反映了偶极耦合和化学吸附变化的结合,覆盖率低于0.5 ML,但未压缩CO的非常大的红移幅度表明与压缩CO相反的化学贡献很大。DFTVASP计算使我们能够遵循从0.5到0.67 ML的表面结构演变,CO频率随覆盖范围而变化。压缩的CO行下方的Pd原子被向上推,压缩的CO相对于表面法线倾斜8-9°。与实验数据一致,发现压缩和未压缩CO之间的频率分配。这些结果表明,当压缩进行时,压缩的CO结合力较弱,其余未压缩的CO结合力更强。

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