Gaussian basis density functional theory for systems periodic in two or three dimensions: Energy and forces

We describe a formulation of electronic density functional theory using localized Gaussian basis functions for systems periodic in three dimensions (bulk crystals) or two dimensions (crystal slabs terminated by surfaces). Our approach generalizes many features of molecular density functional methods to periodic systems, including the use of an auxiliary Gaussian basis set to represent the charge density, and analytic gradients with respect to nuclear coordinates. Existing quantum chemistry routines for analytic and numerical integration over basis functions can be adapted to our scheme with only slight modifications, as can existing extended Gaussian basis sets. Such basis sets permit accurate calculations with far fewer basis functions (and hence much smaller matrices to diagonalize) than plane‐wave based methods, especially in surface calculations, where in our approach the slab does not have to repeat periodically normal to the surface. Realistic treatment of molecule–surface interactions is facilitate...

[1]  Steven G. Louie,et al.  First-principles linear combination of atomic orbitals method for the cohesive and structural properties of solids: Application to diamond , 1984 .

[2]  Krueger,et al.  First-principles calculation of the electronic structure of the wurtzite semiconductors ZnO and ZnS. , 1993, Physical review. B, Condensed matter.

[3]  A. Becke Density-functional thermochemistry. III. The role of exact exchange , 1993 .

[4]  Alex Zunger,et al.  Self-consistent numerical-basis-set linear-combination-of-atomic-orbitals model for the study of solids in the local density formalism , 1977 .

[5]  Ronald H. Felton,et al.  A new computational approach to Slater’s SCF–Xα equation , 1975 .

[6]  R. Dovesi,et al.  Ab initio Hartree-Fock treatment of ionic and semi-ionic compounds: state of the art , 1992, Philosophical Transactions of the Royal Society of London. Series A: Physical and Engineering Sciences.

[7]  Harris Simplified method for calculating the energy of weakly interacting fragments. , 1985, Physical review. B, Condensed matter.

[8]  O. Madelung Semiconductors : group IV elements and III-V compounds , 1991 .

[9]  Andrew Komornicki,et al.  Molecular gradients and hessians implemented in density functional theory , 1993 .

[10]  Hamann Band structure in adaptive curvilinear coordinates. , 1995, Physical review. B, Condensed matter.

[11]  J. Callaway,et al.  Total energy of metallic lithium , 1983 .

[12]  D. Hamann,et al.  Norm-Conserving Pseudopotentials , 1979 .

[13]  Chen,et al.  Dual-space approach for density-functional calculations of two- and three-dimensional crystals using Gaussian basis functions. , 1995, Physical review. B, Condensed matter.

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

[15]  Sharon Hammes-Schiffer,et al.  A new formulation of the Hartree-Fock-Roothaan method for electronic structure calculations on crystals , 1994 .

[16]  J. Boettger Equation of state calculations using the LCGTO-FF method: Equilibrium properties of hcp beryllium † , 1995 .

[17]  J. Boettger,et al.  Total energy and pressure in the Gaussian-orbitals technique. I. Methodology with application to the high-pressure equation of state of neon , 1984 .

[18]  A. Zunger,et al.  New approach for solving the density-functional self-consistent-field problem , 1982 .

[19]  P. P. Ewald Die Berechnung optischer und elektrostatischer Gitterpotentiale , 1921 .

[20]  M. Mehl,et al.  Linearized augmented plane wave electronic structure calculations for MgO and CaO , 1988 .

[21]  Boettger,et al.  High-precision calculation of crystallographic phase-transition pressures for aluminum. , 1995, Physical review. B, Condensed matter.

[22]  R. O. Jones,et al.  The density functional formalism, its applications and prospects , 1989 .

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

[24]  J. Mintmire,et al.  Local-density-functional methods in two-dimensionally periodic systems. Hydrogen and beryllium monolayers , 1982 .

[25]  Erich Wimmer,et al.  Full-potential self-consistent linearized-augmented-plane-wave method for calculating the electronic structure of molecules and surfaces: O 2 molecule , 1981 .

[26]  M. Yin,et al.  Ground-state properties of diamond , 1981 .

[27]  John R. Sabin,et al.  On some approximations in applications of Xα theory , 1979 .

[28]  Eugene P. Wigner,et al.  Effects of the Electron Interaction on the Energy Levels of Electrons in Metals , 1938 .

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

[30]  C. S. Wang,et al.  Self-Consistent Calculation of Energy Bands in Ferromagnetic Nickel , 1973 .

[31]  Car,et al.  Unified approach for molecular dynamics and density-functional theory. , 1985, Physical review letters.

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

[33]  Kee-Joo Chang,et al.  HIGH-PRESSURE BEHAVIOR OF MGO - STRUCTURAL AND ELECTRONIC-PROPERTIES , 1984 .

[34]  R. Dovesi,et al.  On the electrostatic potential in crystalline systems where the charge density is expanded in Gaussian functions , 1992 .

[35]  E. Lafon,et al.  Application of the Method of Tight Binding to the Calculation of the Energy Band Structures of Diamond, Silicon, and Sodium Crystals , 1971 .