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Hydrogen adsorption and desorption at the Pt(110)-(1 x2) surface: experimental and theoretical study

机译:氢在Pt(110)-(1 x2)表面的吸附和解吸:实验和理论研究

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The interaction of hydrogen with the Pt(110)-(1x2) surface is studied using temperature programmed desorption (TPD) measurements and density functional theory (DFT) calculations. The ridges in this surface resemble edges between micro-facets of Pt nano-partide catalysts used for hydrogen evolution (HER) and hydrogen oxidation reactions (HOR). The binding energy and activation energy for desorption are found to depend strongly on hydrogen coverage. At low coverage, the strongest binding sites are found to be the low coordination bridge sites at the edge and this is shown to agree well with the He-atom interaction and work function change which have been reported previously. At higher hydrogen coverage, the higher coordination sites on the micro-facet and in the trough get populated. The simulated TPD spectra based on the DFT results are in close agreement with our experimental spectra and provide microscopic interpretation of the three measured peaks. The lowest temperature peak obtained from the surface with highest hydrogen coverage does not correspond to desorption directly from the weakest binding sites, the trough sites, but is due to desorption from the ridge sites, followed by subsequent, thermally activated rearrangement of the H-adatoms. The reason is low catalytic activity of the Pt-atoms at the trough sites and large reduction in the binding energy at the ridge sites at high coverage. The intermediate temperature peak corresponds to desorption from the micro-facet. The highest temperature peak again corresponds to desorption from the ridge sites, giving rise to a re-entrant mechanism for the thermal desorption.
机译:使用程序升温脱附(TPD)测量和密度泛函理论(DFT)计算研究了氢与Pt(110)-(1x2)表面的相互作用。该表面中的凸脊类似于用于析氢(HER)和氢氧化反应(HOR)的Pt纳米粒子催化剂的微刻面之间的边缘。发现用于解吸的结合能和活化能在很大程度上取决于氢的覆盖率。在低覆盖率下,发现最强的结合位点是边缘处的低配位桥位点,这表明与先前报道的He-原子相互作用和功函数变化非常吻合。在较高的氢覆盖范围内,在微刻面和波谷中的较高配位位点被填充。基于DFT结果的模拟TPD光谱与我们的实验光谱非常吻合,并提供了三个实测峰的微观解释。从具有最高氢覆盖率的表面获得的最低温度峰并不对应于直接从最弱的结合位点即槽位点解吸,而是由于从脊位点解吸,随后是H原子的热活化重排。原因是在高覆盖率下,Pt原子在谷点处的催化活性低,并且在脊位处的结合能大大降低。中间温度峰对应于从微面解吸。最高的温度峰值再次对应于从脊位置解吸,从而引起了热解吸的折返机制。

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