Optical Properties of Solids Claudia Ambrosch-Draxl Chair of Atomistic Modelling and Design of Materials University Leoben, Austria Basics light scattering dielectric tensor in the RPA sumrules symmetry the band gap problem Program program flow inputs outputs Examples convergence results Outlook applications beyond linear optics beyond RPA Optics in WIEN2k Outline Basics light scattering dielectric tensor in the RPA sumrules symmetry the band gap problem Program program flow inputs outputs Examples convergence results Outlook applications beyond linear optics beyond RPA Optics in WIEN2k Outline Dielectric function Optical absorption Optical gap Exciton binding energy Photoemission spectra Core level spectra Raman scattering Compton scattering Positron annihilation NMR spectra Electron spectroscopy Light emitting diodes Lasers Solar cells Displays Computer screens Smart windows Light bulbs CDs & DVDs understand physics characterize materials tailor special properties Excited States Properties & Applications Light – Matter Interaction Polarizability: Linear approximation: susceptibility χ conductivity σ Fourier transform: ∋ dielectric tensor Optical Properties Response to external electric field E The Dielectric Tensor Bloch electrons: Interband contribution: intraband interband independent particle approximation, random phase approximation (RPA) Optical Properties Free electrons: Lindhard formula Light Scattering hω E S interband transition ck EF hω intraband transition vk wave vector Optical Properties Energy band structure Optical "Constants" Optical conductivity: Complex refractive index: Reflectivity: Absorption coefficient: Loss function: Kramers-Kronig relations Optical Properties Complex dielectric tensor: Intraband Contributions Dielectric Tensor: Drude-like terms Plasma frequency: Metals Optical conductivity: Optical Properties Sumrules Symmetry monoclinic (α,β=90°) orthorhombic tetragonal, hexagonal cubic Dielectric Tensor triclinic Magneto-optics without magnetic field, spin-orbit coupling: cubic with magnetic field H װz, spin-orbit coupling: tetragonal KK KK Example: Ni KK Be careful .... Wavefunction vs. Density Hartree-Fock: Koopman's theorem DFT: Lagrange parameters Janak's theorem auxiliary functions Excited States ionization energies Approximations used: Ground state: Local Density Approximation (LDA) Generalized Gradient Approximation (GGA) Excited state: Interpretation within one-particle picture Interpretation of excited states in terms of ground state properties Electron-hole interaction ignored (RPA) Where do possible errors come from? How to treat excited states ab initio? Excited State Properties Open Questions The Band Gap Problem Ionization energy Electro-affinity Band gap shift of conduction bands: scissors operator many-body perturbation theory: GW approach Basics Program Examples Outlook light scattering dielectric tensor in the RPA sumrules symmetry the band gap problem program flow inputs outputs convergence results applications beyond linear optics beyond RPA Optics in WIEN2k Outline Program Flow converged potential kgen dense mesh lapw1 eigenstates lapw2 Fermi distribution optic momentum matrix elements joint dielectrix tensor components kram Re ε Im ε optical coefficients broadening scissors operator Optics in WIEN2k SCF cycle al.inop 2000 1 -5.0 2.2 1 1 OFF "optic" number of k-points, first k-point Emin, Emax: energy window for matrix elements number of cases (see choices below) Re <x><x> unsymmetrized matrix elements written to file? 800 1 -5.0 5.0 3 1 3 7 OFF number of k-points, first k-point Emin, Emax: energy window for matrix elements number of cases (see choices below) Choices: Re <x><x> 1......Re <x><x> Re <z><z> 2......Re <y><y> Im <x><y> 3......Re <z><z> 4......Re <x><y> 5......Re <x><z> 6......Re <y><z> 7......Im <x><y> 8......Im <x><z> 9......Im <y><z> Inputs ni.inop (magneto-optics) "joint" al.injoint lower and upper band index Emin, dE, Emax [Ry] output units eV / Ry switch number of columns to be considered broadening for Drude model choose gamma for each case! SWITCH 0...JOINT DOS 1...JOINT DOS 2...DOS 3...DOS 4...Im(EPSILON) 5...Im(EPSILON) 6...INTRABAND 7...INTRABAND for each band combination sum over all band combinations for each band sum over all bands total for each band combination contributions contributions including band analysis Inputs 1 18 0.000 0.001 1.000 eV 4 1 0.1 0.2 "kram" al.inkram broadening gamma energy shift (scissors operator) add intraband contributions 1/0 plasma frequency gamma(s) for intraband part 0.1 0.0 1 12.6 0.2 as number of colums as number of colums 70 Silicon Dielectric function 60 Imε 50 40 si.inkram Reε 30 20 10 0 -10 Γ=0.05eV -20 0 1 2 3 Energy [eV] 4 5 6 0.05 broadening gamma 1.00 energy shift (scissors operator) 0 .... Inputs 80 optic case.symmat case.mommat momentum matrix elements, symmetrized analysis, NLO joint Im ε SWITCH 4 kram case.epsilon case.sigmak case.refraction case.absorp case.eloss complex dielectric tensor optical conductivity refractive index absorption coefficient loss function Outputs case.joint Basics light scattering dielectric tensor in the RPA sumrules symmetry the band gap problem Program program flow inputs outputs Examples convergence results Outlook applications beyond linear optics beyond RPA Optics in WIEN2k Outline Results .... Convergence Interband Im ε 150 125 100 75 165k 286k 560k 1240k 2456k 3645k 4735k 12.8 12.7 12.6 12.5 12.4 12.3 12.2 12.1 12.0 ωp 0 1000 2000 3000 4000 5000 k-points in IBZ 50 25 0 0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 Energy [eV] Example: Al 175 Sumrules 5 165 k-points 4735 k-points Experiment 3 Example: Al Neff [electrons] 4 2 1 0 0 10 20 30 40 50 60 70 80 90 100 Energy [eV] Loss Function 120 80 intraband 60 40 total 20 0 Example: Al Loss function 100 interband 0 5 10 Energy [eV] 15 20 Example: Platinum Theory - Experiment K. Glantschnig, and C. Ambrosch-Draxl, (preprint). C. Ambrosch-Draxl and J. O. Sofo Comp. Phys. Commun., in print