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Correction: A unified study for water adsorption on metals: meaningful models from structural motifs

Guillem Revilla-López * and Núria López *
Institute of Chemical Research of Catalonia, ICIQ, Av. Països Catalans 16, 43007 Tarragona, Spain. E-mail: nlopez@iciq.es

Received 2nd September 2014 , Accepted 2nd September 2014

First published on 11th September 2014


Abstract

Correction for ‘A unified study for water adsorption on metals: meaningful models from structural motifs’ by Guillem Revilla-López et al., Phys. Chem. Chem. Phys., 2014, 16, 18933–18940.


Authors noticed erroneous values in Table 2 that should be the result of applying the formula: γads (eV Å−2) = Eads/A where Eads are the total adsorption energies for each motif, and A the surface area where the motif was calculated.

Consequently the first paragraph of section 3.1, “Strain effects on DFT adsorption energies” from line 47 on page 18935 to line 8 on page 18936, should read:

The DFT-D2 adsorption energies for different sets of training structures under ±4% dXY deformation are presented in Table 1 in eV per H2O. Table 2 reports the same energies per surface area unit, Å−2, to better understand the experimental results. The direct comparison between data in Tables 1 and 2 indicates that the adsorption energies and surface energies follow a similar pattern. In both cases sqrt(37), 0.7 ML, shows the lowest energy. In contrast, ice-like bilayer, 0.67 ML, and Rosette, 0.5 ML, swap their position in the ranking with the latter being the least stable. Yet, in Ru(0001) dissociated ice-like bilayer has the lowest adsorption energy, γads, followed by the other three in the same ordering.

Table 2 DFT-D2 calculated adsorption energies for H-down ice-like, sqrt(37) and Rosette structures on Pd, Pt and Ru. All energies are in eV Å−2. All dXY are in plane deformations (in %) with respect to the unstrained metal slab
d XY Pd(111) Pt(111) Ru(0001)
Ice-like sqrt(37) Rosette Ice-like sqrt(37) Rosette Ice-like Ice-like diss. sqrt(37) Rosette
4 −0.059 −0.071 −0.048 −0.057 −0.068 −0.047 −0.061 −0.099 −0.083 −0.059
2 −0.061 −0.072 −0.048 −0.058 −0.070 −0.047 −0.064 −0.099 −0.082 −0.059
0 −0.063 −0.073 −0.049 −0.060 −0.071 −0.047 −0.064 −0.092 −0.082 −0.058
−2 −0.064 −0.074 −0.050 −0.061 −0.072 −0.047 −0.064 −0.084 −0.083 −0.057
−4 −0.065 −0.075 −0.049 −0.063 −0.073 −0.047 −0.066 −0.075 −0.083 −0.056


The Royal Society of Chemistry apologises for these errors and any consequent inconvenience to authors and readers.


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