Computational Materials Science:From Ground States to Excitations in Solids2.pptVIP

Computational Materials Science:From Ground States to Excitations in Solids2.ppt

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Computational Materials Science:From Ground States to Excitations in Solids2

Simple metal (Free electron like): Na Fermi surface of Na Simple metal (Free electron like): Al Fermi Surface of Al Density of States: Al More complicated metal: Cu Fermi Surface of Cu More complicated metal: MgB2 Electron-phonon coupling in MgB2 Fermi Surface of MgB2 Semi-metal: Graphene Semi-metal: Graphene Semiconductor: Si Semiconductor: Si Magnetism: BCC Fe (DFT-GGA) Magnetism: HCP Co (DFT-GGA) Magnetism: CCP Ni (DFT-GGA) Magnetic Properties * Computational Materials Science: From Ground States to Excitations in Solids Peihong Zhang Department of Physics, University at Buffalo, SUNY July 20, 2009 USTC 2009 Summer School Outline Materials properties from first-principles: a hard problem Earlier efforts Density functional theory Local Density Approximation Success of DFT: Examples “Failure” of DFT Beyond DFT: LDA+U Beyond DFT: Quasiparticle and optical excitations in solids Electron-phonon coupling and superconductivity Materials design from first-principles: realizing the dream Total Energy, Cohesive Energy 0.28 0.27 Pd 0.42 0.45 Rh 0.50 0.49 Mo 0.56 0.55 Nb Experiment DFT-LDA Metal Total energy of atoms (Ry.) Cohesive energy (Ry.) Comparison between the highest occupied Kohn-Sham orbital energy and the ionization energy (in Ry) (a) Morrison, et al., 1995 Ionization Energy Structural Properties: Molecules Structural properties of diborane 1.19 1.33 97o 122o EXP 1.19 1.33 97o 122o DFT-GGA 1.20 1.32 98o 121o DFT-LDA d2 (?) d1 (?) b a Diborne (3c-2e bond) Lattice constant (a.u.) LDA predicts lattice constants to within 2%. Bulk modulus (Mbar) LDA predicts bulk modulus to within a few percents. Structural Properties Lattice constant a3 a1 a2 Structure: BCC Brillouin Zone Ef Structure: CCP (FCC) Brillouin Zone EF Note that if we plot the Fermi surface of Al in the extended zone scheme, it will still look like a sphere! Energy (eV) occupied empty In contrast, DOS for a metal does not show a gap near the Fermi energy Structure: CCP Brillouin Zone Energy (eV) d-b

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