4.4 Article

Adsorption and thermal chemistry of formic acid on clean and oxygen-predosed Cu(110) single-crystal surfaces revisited

Journal

SURFACE SCIENCE
Volume 646, Issue -, Pages 37-44

Publisher

ELSEVIER SCIENCE BV
DOI: 10.1016/j.susc.2015.06.007

Keywords

Formic acid; Copper single-crystal surface; Predosed oxygen; Thermal chemistry; X-ray photoelectron spectroscopy

Funding

  1. U.S. Department of Energy, Office of Science, Basic Energy Sciences, Materials Science Division [DE-SC0001839]
  2. U.S. Department of Energy (DOE) [DE-SC0001839] Funding Source: U.S. Department of Energy (DOE)

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The thermal chemistry of formic acid on clean and oxygen-predosed Cu(110) single-crystal surfaces was studied under ultrahigh-vacuum (UHV) conditions by temperature programmed desorption (TPD) and X-ray photoelectron spectroscopy (XPS). Key results reported in the past were confirmed, including the partial switchover from H-2 to H2O desorption upon oxygen addition on the surface and the development of a second decomposition regime at 420 K, in addition to the one observed at 460 K on the clean substrate. In addition, new observations were added, including the previously missed desorption of H-2 at 420 K and the existence of a normal kinetic isotope effect in both TPD peaks. Peak fitting of the XPS data afforded the identification of an asymmetric geometry for the formate intermediate, which was established to form by 200 K, and the presence of coadsorbed molecular formic acid up to the temperatures of decomposition, probably in a second layer and held by hydrogen bonding. Quantitative analysis of the TPD data indicated a one-to-one correspondence between the increase in oxygen coverage beyond theta(o) = 0.5 ML and a decrease in formic acid uptake that mainly manifests itself in a decrease in the decomposition seen in the 460 K TPD peak. All these observations were interpreted in terms of a simple decomposition mechanism involving hydrogen abstraction from adsorbed formate species, possibly aided by coadsorbed oxygen, and a change in reaction activation energy as a function of the structure of the oxygen overlayer, which reverts from a O-c(6 x 2) structure at high oxygen coverages to the O-(2 x 1) order seen at theta(o) = 0.5 ML. Published by Elsevier B.V.

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