4.3 Article

First-principles investigation of CuO decomposition and its transformation into Cu2O

期刊

PHYSICAL REVIEW MATERIALS
卷 6, 期 9, 页码 -

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AMER PHYSICAL SOC
DOI: 10.1103/PhysRevMaterials.6.096001

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  1. European Research Council (H2020 Excellent Science) Researcher Award [832889-PyroSafe]

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This paper reports on the mechanisms of CuO decomposition and its phase transformation into Cu2O. The results show that CuO decomposition starts at defects/interfaces/surfaces, with CuO(001) surface having a lower activation energy for oxygen vacancy formation. The release of oxygen upon decomposition is driven by the migration of vacancies close to the surface and towards the bulk. The phase transformation from CuO to Cu2O occurs in two steps, with a structural modification from monoclinic to orthorhombic followed by a barrierless transition to the cubic phase.
This paper reports on the mechanisms of CuO decomposition and its associated phase transformation into Cu2O, as a fundamental step of thermite materials reaction, where CuO serves as the oxidizer. The Frenkel pair defects in perfect bulk CuO show extremely high formation energy (>4 eV) indicating that its decom-position initiates at defects/interfaces/surfaces, the latter being sensitive to surface orientation. In contrast to a variety of CuO surfaces [(111), (110), (101 over bar )] exhibiting three-fold coordinated oxygen atoms, results show that oxygen vacancy formation requires higher disordered surfaces, such as the CuO(001), on which the vacancy formation activation energy is reduced to 1.31 eV. This leads to the exothermic formation of a chemisorbed O-O peroxy-bridge complex at the surface (-1.25 eV adsorption) that thermodynamically moderates the backreaction (vacancy annihilation). Further desorption of molecular oxygen necessitates an activation of 1.53 eV, compatible with CuO decomposition observed experimentally at 600 K (similar to second process duration). As a driving mechanism of oxygen release upon decomposition, migrations of the vacancy close to the surface and towards the bulk are determined for a number of crystalline directions and surface orientations and show considerable anisotropy, with two preferential directions: [110] and [001] with 1.35 and 1.77 eV activation, lowered to 1.08 and 1.03 eV activation when approaching the (111) and (001) surfaces, respectively. Finally, the CuO to Cu2O phase transformation follows a two-step process: a first structural modification from monoclinic to orthorhombic takes place when CuO has lost 12.5% of its oxygen atoms, followed by a barrierless transition to the cubic phase when 44-48% of the oxygen atoms have been removed, i.e., very close to stoichiometric Cu2O.

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