Pseudopotentials & TDDFT calculation

Slides:



Advertisements
Similar presentations
Take-home postcard. Basis set: Atomic orbitals s p d f SIESTA: Strictly localized (zero beyond cut-off radius)
Advertisements

Quantum Theory of Solids
Introduction to PAW method
First Principle Electronic Structure Calculation Prof. Kim Jai Sam ( ) Lab. 공학 ( ) Students : Lee Geun Sik,
Systematics for realistic proyects: from quick & dirty to converged calculations José M. Soler and Alberto García.
Introduction to the Theory of Pseudopotentials Patrick Briddon Materials Modelling Group EECE, University of Newcastle, UK.
Javier Junquera Code structure: calculation of matrix elements of H and S. Direct diagonalization José M. Soler = N  N N  1.
CHE Inorganic, Physical & Solid State Chemistry Advanced Quantum Chemistry: lecture 4 Rob Jackson LJ1.16,
PA4311 Quantum Theory of Solids Quantum Theory of Solids Mervyn Roy (S6) www2.le.ac.uk/departments/physics/people/mervynroy.
Norm-conserving pseudopotentials in electronic structure calculations Javier Junquera Alberto García.
The Projector Augmented Wave invented by P.E. Blochl, 1994 IBM Research Division, Zürich Research Laboratory Electronic Structure Course, UC Davis by Ryan.
Classical Model of Rigid Rotor
Modifying the Schrödinger Equation
Bondyakov A.S. Institute of Physics of ANAS, Azerbaijan JINR, Dubna.
Physics “Advanced Electronic Structure” Pseudopotentials Contents: 1. Plane Wave Representation 2. Solution for Weak Periodic Potential 3. Solution.
Lectures Introduction to computational modelling and statistics1 Potential models2 Density Functional.
Norm-conserving pseudopotentials and basis sets in electronic structure calculations Javier Junquera Universidad de Cantabria.
The Nuts and Bolts of First-Principles Simulation Durham, 6th-13th December : DFT Plane Wave Pseudopotential versus Other Approaches CASTEP Developers’
Javier Junquera Code structure: calculation of matrix elements of H and S. Direct diagonalization José M. Soler = N  N N  1.
Calculation of matrix elements José M. Soler Universidad Autónoma de Madrid.
R. Martin - Pseudopotentials1 African School on Electronic Structure Methods and Applications Lecture by Richard M. Martin Department of Physics and Materials.
Computational Solid State Physics 計算物性学特論 第6回
Norm Conserving Pseudopotentials and The Hartree Fock Method Eric Neuscamman Mechanical and Aerospace Engineering 715 May 7, 2007.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Some ideas for common input/output formats for the MS codes Keisuke Hatada Dipartimento di Fisica, Università Camerino.
PA4311 Quantum Theory of Solids Quantum Theory of Solids Mervyn Roy (S6) www2.le.ac.uk/departments/physics/people/mervynroy.
Electronic Bandstructures Information from Kittel’s book (Ch. 7) + many outside sources. Some lectures on energy bands will be based on those prepared.
Comp. Mat. Science School 2001 Lecture 21 Density Functional Theory for Electrons in Materials Richard M. Martin Bands in GaAs Prediction of Phase Diagram.
TBPW: A Modular Framework for Pedagogical Electronic Structure Codes Todd D. Beaudet, Dyutiman Das, Nichols A. Romero, William D. Mattson, Jeongnim Kim.
PA4311 Quantum Theory of Solids Quantum Theory of Solids Mervyn Roy (S6) www2.le.ac.uk/departments/physics/people/mervynroy.
The Tightbinding Bandstructure Theory
Physics “Advanced Electronic Structure” Lecture 1. Theoretical Background Contents: 1. Historical Overview. 2. Basic Equations for Interacting Electrons.
How to generate a mixed pseudopotential Objectives Generate a mixed pseudopotential to be used in the Virtual Crystal Approximation or in simulations at.
Bandstructures: Real materials. Due my interests & knowledge, we’ll mostly focus on bands in semiconductors. But, much of what we say will be equally valid.
Electric field which acts on core C due to the valence electrons and the other cores. Where is a cutoff function for the electric field inside the core.
Physics “Advanced Electronic Structure”
9/30/2015PHY 752 Fall Lecture 161 PHY 752 Solid State Physics 11-11:50 AM MWF Olin 103 Plan for Lecture 16: Reading: Chapter 5 in GGGPP Ingredients.
Harmonic Oscillator (harmosc1.mpg) The wave function at t = 0 has the form  (x,0) = A exp[-x 2 /10 2 ] V(x) = ½ (x/50) 2 & starting v = 0 Which direction.
How to generate a pseudopotential with the semicore in the valence Objectives Check whether semicore states should be explicitly included in the valence.
Start. Technische Universität Dresden Physikalische Chemie Gotthard Seifert Tight-binding Density Functional Theory DFTB an approximate Kohn-Sham DFT.
Biswajit Santra Fritz Haber Institute of the Max Planck Society MONET.
Spin-Orbit Coupling. Spin-Orbit Coupling First Some General Comments An Important (in some cases) effect we’ve left out! We’ll discuss it mainly for terminology.
Advanced methods of molecular dynamics 1.Monte Carlo methods 2.Free energy calculations 3.Ab initio molecular dynamics 4.Quantum molecular dynamics 5.Trajectory.
2/25/2015PHY 752 Spring Lecture 181 PHY 752 Solid State Physics 11-11:50 AM MWF Olin 107 Plan for Lecture 18: Reading: Chapter 10 in MPM Ingredients.
2/18/2015PHY 752 Spring Lecture 151 PHY 752 Solid State Physics 11-11:50 AM MWF Olin 107 Plan for Lecture 15: Reading: Chapter 10 in MPM Numerical.
PA4311 Quantum Theory of Solids Quantum Theory of Solids Mervyn Roy (S6) www2.le.ac.uk/departments/physics/people/mervynroy.
The Pseudopotential Method Builds on all of this..
Computational Physics (Lecture 23) PHY4370. Mermin finite temperature and ensemble density functional theory The theorems of Hohenberg and Kohn for the.
2/23/2015PHY 752 Spring Lecture 171 PHY 752 Solid State Physics 11-11:50 AM MWF Olin 107 Plan for Lecture 17: Reading: Chapter 10 in MPM Ingredients.
A Personal History of the ABINIT Project
Isolated Si atoms.
BY SELLAVEL E (CA15M006) Guided By Prof.B.Viswanathan
Testing Atomic Structure using Atom Interferometry
Potential - density pairs (continued)
Solve: 1. 4<
The Pseudopotential Method Builds on all of this. See YC, Ch
Coulomb repulsion and Slater Integrals
Electronic Structure and First Principles Theory
Dirac Line Nodes in Inversion Symmetric Crystals C. L. Kane & A. M
The Pseudopotential Method Builds on all of this.
Reciprocal lattice Real space lattice.
Physical Chemistry Week 12
Shells and Valence Electrons
Scalar theory of diffraction
Scalar theory of diffraction
Unit 3 Review (Calculator)
How to test a norm-conserving pseudopotential
Calculate 9 x 81 = x 3 3 x 3 x 3 x 3 3 x 3 x 3 x 3 x 3 x 3 x =
The following slides show you how to treat the Coulomb interaction in a many particle Hamiltonian. As the Coulomb interaction diverges for the case where.
Presentation transcript:

Pseudopotentials & TDDFT calculation UNIST Dongbin Shin

Why pseudopotentials? To minimize the size of plane wave basis : valence state are smoother than core state, pseudized valence wave function are nodeless To reduce number of electron in system

Generating Pseudopotential

Norm-conserving pseudopotentials

Pseudopotential - Local Part

Separable Kleinman-Bylander form for NLpp

Separable Kleinman-Bylander form for NLpp

Ultrasoft pseudopotentials

ylmr2.f90 Spherical harmonics

Initial pseudopotential init_us_1.f90 Initial pseudopotential

init_us_2.f90 Beta term in G space

realus.f90 Beta term in real space

Solve nonlocal potentials add_vuspsi.f90 Solve nonlocal potentials

Suzuki-Trotter type split-operator

TD-DFT pseudopotential theory