We have explored the retention of hydrogen (H) in tungsten (W) by investigating its dissolution and aggregation in vacancy clusters (VCs) using a first-principles method and thermodynamic models. The solution… Click to show full abstract
We have explored the retention of hydrogen (H) in tungsten (W) by investigating its dissolution and aggregation in vacancy clusters (VCs) using a first-principles method and thermodynamic models. The solution energy of a single H in the VCs is in the range of -0.99 ~ -0.64 eV, much lower than that at a mono-vacancy (~ -0.37 eV) and interstitial site (~ 1.01 eV) in W. Such a remarkable discrepancy is rationalized on the electronic interaction of H with its neighboring W atoms, which varies from repulsion to attraction with H moving from perfect crystal to vacancy/VCs. Specifically, the solution/trapping energies of H in VCs can be well categorized by the coordination number of its neighboring W atoms, i.e. the lower the coordination number of W, the stronger is the H-W attraction and the lower is the H solution/trapping energy. Furthermore, taking the V_9^m cluster as an example, it is observed that the multiple H atoms form a multilayer nested cage configuration at VCs surface initially, and then the stable H2 molecules form in the center of VCs. Interestingly, the pre-existed H atoms in VCs inner surface has a shielding effect on the H-W interaction, decreasing the electron density of the central region of VCs and facilitating the formation of H2 molecules. Moreover, the desorption temperatures of H in VCs are also predicted based on the Polanyi-Wigner equation, which are in good agreement with the available thermal desorption spectroscopy experiments. Our calculations provide a good reference to understand the influence of VCs on the retention and evolution of H in W.
               
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