2019
DOI: 10.1088/1741-4326/ab33e7
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Surface coverage dependent mechanisms for the absorption and desorption of hydrogen from the W(1 1 0) and W(1 0 0) surfaces: a density functional theory investigation

Abstract: Surface coverage dependent mechanisms for the absorption and desorption of hydrogen from the W(110) and W(100) surfaces: a DFT investigation.

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Cited by 25 publications
(58 citation statements)
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“…Using this method, we determine the dependence of the desorption energy E D and the absorption energy (the surface into the bulk) E A on hydrogen coverage. For both energies the dependence is similar: they increase as coverage decreases which is in agreement with DFT calculations [17,18].…”
Section: Discussionsupporting
confidence: 88%
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“…Using this method, we determine the dependence of the desorption energy E D and the absorption energy (the surface into the bulk) E A on hydrogen coverage. For both energies the dependence is similar: they increase as coverage decreases which is in agreement with DFT calculations [17,18].…”
Section: Discussionsupporting
confidence: 88%
“…Sub-surface Bulk ≈ 0.60−0.50 eV; this might appear large as compared to DFT results [18] in which E off−set S does not exceed 0.12 eV on well oriented surfaces. The discrepancy could be explained by the fact that in the present work, we model highly damaged surfaces, which might explain a larger value of E off−set…”
Section: Surfacementioning
confidence: 56%
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“…As in our previous studies of the interactions of hydrogen with tungsten surfaces 17,18 , herein we use a similar periodic plane-wave DFT model as implemented in Quantum Espresso package 19 .…”
Section: Density Functional Theory Surface Model and Numerical Parame...mentioning
confidence: 99%
“…More precisely, Bergstrom et al, 35 and Nojima et al 24 established two diffusion paths for hydrogen on the W(110) plane: one along the TF-LB-TF adsorptions sites with related activation barrier of 0.30 eV, and another one along the TF-SB-TF path with an activation barrier of 0.07 eV. In the z-direction, the activation barrier for desorption is much higher at around 0.8eV 17 . As a result, the propensity of hydrogen to move almost freely in 1D only along the TF-SB-TF path of W(110) would be established.…”
Section: -W(110) Surfacementioning
confidence: 99%