Auxiliary basis sets for grid-free density functional theory

Density functional theory (DFT) has gained popularity because it can frequently give accurate energies and geometries. The evaluation of DFT integrals in a fully analytical manner is generally impossible; thus, most implementations use numerical quadrature over grid points. The grid-free approaches were developed as a viable alternative based upon the resolution of the identity (RI). Of particular concern is the convergence of the RI with respect to basis set in the grid-free approach. Conventional atomic basis sets are inadequate for fitting the RI, particularly for gradient corrected functionals [J. Chem. Phys. 108, 9959 (1998)]. The focus of this work is on implementation of and selection of auxiliary basis sets. Auxiliary basis sets of varying sizes are studied and those with sufficient flexibility are found to adequately represent the RI.

[1]  M. Rasolt Exchange and correlation energy in a nonuniform fermion fluid. , 1986, Physical review. B, Condensed matter.

[2]  Joel D. Kress,et al.  Rational function representation for accurate exchange energy functionals , 1987 .

[3]  J. Almlöf,et al.  A GRID-FREE DFT IMPLEMENTATION OF NON-LOCAL FUNCTIONALS AND ANALYTICAL ENERGY DERIVATIVES , 1996 .

[4]  B. A. Hess,et al.  Toward the variational treatment of spin‐orbit and other relativistic effects for heavy atoms and molecules , 1986 .

[5]  Parr,et al.  Local exchange-correlation functional: Numerical test for atoms and ions. , 1992, Physical review. A, Atomic, molecular, and optical physics.

[6]  T. G. Wright Geometric structure of Ar⋅NO+: Revisited. A failure of density functional theory , 1996 .

[7]  Axel D. Becke,et al.  Density‐functional thermochemistry. IV. A new dynamical correlation functional and implications for exact‐exchange mixing , 1996 .

[8]  D. Langreth,et al.  Beyond the local-density approximation in calculations of ground-state electronic properties , 1983 .

[9]  Michael W. Schmidt,et al.  Effective convergence to complete orbital bases and to the atomic Hartree–Fock limit through systematic sequences of Gaussian primitives , 1979 .

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

[11]  S. H. Vosko,et al.  Accurate spin-dependent electron liquid correlation energies for local spin density calculations: a critical analysis , 1980 .

[12]  Michael J. Frisch,et al.  The performance of the Becke-Lee-Yang-Parr (B-LYP) density functional theory with various basis sets , 1992 .

[13]  G. Merrill,et al.  FLUORIDE-INDUCED ELIMINATION OF ETHYL FLUORIDE. THE IMPORTANCE OF HIGH-LEVEL OPTIMIZATIONS IN AB INITIO AND DFT STUDIES , 1995 .

[14]  Thom H. Dunning,et al.  Gaussian basis sets for use in correlated molecular calculations. V. Core-valence basis sets for boron through neon , 1995 .

[15]  Benny G. Johnson,et al.  The performance of a family of density functional methods , 1993 .

[16]  Cook,et al.  Grid-free density-functional technique with analytical energy gradients. , 1995, Physical review. A, Atomic, molecular, and optical physics.

[17]  J. Stephen Binkley,et al.  Self‐consistent molecular orbital methods. XIX. Split‐valence Gaussian‐type basis sets for beryllium , 1977 .

[18]  Brett I. Dunlap Geometry optimization using local density functional methods , 1986 .

[19]  A. Becke,et al.  Density-functional exchange-energy approximation with correct asymptotic behavior. , 1988, Physical review. A, General physics.

[20]  B. Alder,et al.  THE GROUND STATE OF THE ELECTRON GAS BY A STOCHASTIC METHOD , 2010 .

[21]  K. Burke,et al.  Rationale for mixing exact exchange with density functional approximations , 1996 .

[22]  P. Pyykkö,et al.  Two-dimensional, fully numerical molecular calculations , 1985 .

[23]  Horst M. Sulzbach,et al.  Exploring the boundary between aromatic and olefinic character: Bad news for second-order perturbation theory and density functional schemes , 1996 .

[24]  Mark S. Gordon,et al.  General atomic and molecular electronic structure system , 1993, J. Comput. Chem..

[25]  Trevor J. Sears,et al.  Far infrared laser magnetic resonance of singlet methylene: Singlet–triplet perturbations, singlet–triplet transitions, and the singlet–triplet splittinga) , 1983 .

[26]  Jan Almlöf,et al.  Density functionals without meshes and grids , 1993 .

[27]  David E. Bernholdt,et al.  Fitting basis sets for the RI-MP2 approximate second-order many-body perturbation theory method , 1998 .

[28]  R. C. Weast CRC Handbook of Chemistry and Physics , 1973 .

[29]  M. Gordon,et al.  Evaluation of gradient corrections in grid-free density functional theory , 1999 .

[30]  Katrina S. Werpetinski,et al.  A NEW GRID-FREE DENSITY-FUNCTIONAL TECHNIQUE : APPLICATION TO THE TORSIONAL ENERGY SURFACES OF ETHANE, HYDRAZINE, AND HYDROGEN PEROXIDE , 1997 .

[31]  J. Almlöf,et al.  Integral approximations for LCAO-SCF calculations , 1993 .

[32]  W. C. Lineberger,et al.  Methylene: A study of the X̃ 3B1 and ã 1A1 states by photoelectron spectroscopy of CH−2 and CD−2 , 1985 .

[33]  J. C. Slater Statistical Exchange-Correlation in the Self-Consistent Field , 1972 .

[34]  G. Herzberg,et al.  Constants of diatomic molecules , 1979 .