Point defects in uranium dioxide: Ab initio pseudopotential approach in the generalized gradient approximation

The stability of point defects in uranium dioxide is studied using an ab initio plane wave pseudopotential method in the generalized gradient approximation of the density functional theory. Uranium pseudopotentials are first tested in both the generalized gradient approximation and the local density approximation on metallic phases of uranium and on uranium dioxide. It is found that the generalized gradient approximation gives the best description of these materials. The energies of formation of point defects (single vacancies and interstitials, Frenkel pairs and Schottky defects) in UO2 are calculated. The values obtained lead to a reliable set of numerical data that are analyzed in the framework of the point defect model commonly used to assess defect concentrations in uranium dioxide as a function of the stoichiometry. The ability of the point defect model to accurately reproduce defect concentrations in uranium dioxide is discussed.

[1]  P. Söderlind First-principles elastic and structural properties of uranium metal , 2002 .

[2]  T. Arias,et al.  Iterative minimization techniques for ab initio total energy calculations: molecular dynamics and co , 1992 .

[3]  F. Murnaghan The Compressibility of Media under Extreme Pressures. , 1944, Proceedings of the National Academy of Sciences of the United States of America.

[4]  P. Hohenberg,et al.  Inhomogeneous Electron Gas , 1964 .

[5]  F. Jollet,et al.  Plane-wave pseudopotential study of point defects in uranium dioxide , 2001 .

[6]  Matthieu Verstraete,et al.  First-principles computation of material properties: the ABINIT software project , 2002 .

[7]  R. Konings,et al.  Thermochemical data for reactor materials and fission products: The ECN database , 1990 .

[8]  Burke,et al.  Generalized Gradient Approximation Made Simple. , 1996, Physical review letters.

[9]  Hamann Generalized norm-conserving pseudopotentials. , 1989, Physical review. B, Condensed matter.

[10]  H. Cynn,et al.  Phase diagram of uranium at high pressures and temperatures , 1998 .

[11]  B. Willis,et al.  A neutron diffraction study of anion clusters in nonstoichiometric uranium dioxide , 1990 .

[12]  W. Kohn,et al.  Self-Consistent Equations Including Exchange and Correlation Effects , 1965 .

[13]  H. Monkhorst,et al.  SPECIAL POINTS FOR BRILLOUIN-ZONE INTEGRATIONS , 1976 .

[14]  G. V. Chester,et al.  Solid State Physics , 2000 .

[15]  F. Jollet,et al.  Plane-wave pseudopotential study of the light actinides , 2002 .

[16]  李幼升,et al.  Ph , 1989 .

[17]  C. S. Barrett,et al.  Crystal Structure Variations in Alpha Uranium at Low Temperatures , 1963 .

[18]  C. Catlow,et al.  Point-defect calculations on UO2 , 1987 .

[19]  A. B. Lidiard Self-diffusion of uranium in UO2 , 1966 .

[20]  Martins,et al.  Efficient pseudopotentials for plane-wave calculations. , 1991, Physical review. B, Condensed matter.

[21]  A. Pasturel,et al.  Point defects in uranium dioxide , 1998 .

[22]  G. G. Stokes "J." , 1890, The New Yale Book of Quotations.

[23]  Hansjoachim Matzke,et al.  Atomic transport properties in UO2 and mixed oxides (U, Pu)O2 , 1987 .