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![Page 1: Introduction to density functional theory - YAMBO · PDF fileIntroduction to DFT - Myrta Grüning Introduction to density functional theory What is density functional theory How does](https://reader037.vdocument.in/reader037/viewer/2022102920/5aadb6287f8b9a8f498e9b4e/html5/thumbnails/1.jpg)
Introduction to DFT - Myrta Grüning
Introduction to density functional theory
What is density functional theory
How does it work in practice
How does DFT fit in this workshop
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Introduction to DFT - Myrta Grüning
Challenge of electronic structure problem
Goal: determine material properties directly from fundamental equations
Challenge: develop efficient andaccurate methods to achieve that goal
# electronsCO
ST
Exponential
wall
any observable:
From
degrees of freedom: Note: only electronic degrees of freedom; Born-Oppeheimer approximation
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Introduction to DFT - Myrta Grüning
Use simpler quantities than wavefunction
reduce # degree of freedom by averaging out information I do not need
e.g. density matrices
: all info's about the system: do I really need that?!?
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Introduction to DFT - Myrta Grüning
Examples of density matrices
diagonal two-particle density matrix
electron density
one-particle density matrix
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Introduction to DFT - Myrta Grüning
Examples of density matrices
diagonal two-particle density matrix
one-particle density matrix
electron density
NOTE:
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Introduction to DFT - Myrta Grüning
The simplest of them all: density
electron density: just 3 degrees of freedom!
Which information is contained in the density
Can we use the density to calculate materials properties
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Introduction to DFT - Myrta Grüning
Which information does the density contain?
cusps: nuclear positions & charges
Space integration: total number of electrons
Number of electrons, nuclear position/charges uniquely define the Hamiltonian(*)
Once the Hamiltonian is known, we can in principle SOLVE IT!
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Introduction to DFT - Myrta Grüning
Which information does the density contain?
Formal proof: H-K theorem (reductio ad absurdum)
one-to-one correspondence:
ground state unique, universal functional of the density:
any ground state observable is a density functional:
Hohenberg-Kohn (1964)
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Introduction to DFT - Myrta Grüning
Can we use the density for calculations?
one-to-one correspondence + Ritz variational principle:
Ground state energy is a density functional:
With this minimum principle we can develop a computational method to calculate GS properties of a system
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Introduction to DFT - Myrta Grüning
What is density-functional theory?
based on the Hohenberg-Kohn theorem
Electronic structure approach whose key quantity is the density
to calculate GS properties of a system
(ensures that many-particle system in its GS is fully characterized by its GS density)
minimizes
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Introduction to DFT - Myrta Grüning
Rewrite the total energy as functional of n...
Challenge:Fit many-particle intricacies in such simple object as the density
We need:
We have:
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Introduction to DFT - Myrta Grüning
Critical approximation is the kinetic energy Thomas-Fermi (1927)
i.e.: separate always lower energy than
Problems: at best qualitative, no chemical bonding -Achievements: qualitative trends for atoms +
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Introduction to DFT - Myrta Grüning
Get large part of T via non-interacting systemKohn-Sham (1965)
Physical system (N-body problem)
Kohn-Sham system (N X 1-body problems)
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Introduction to DFT - Myrta Grüning
Kohn-Sham equationsKohn-Sham (1965)
Defining the exchange-correlation energy functional
+ applying Hohenberg-Kohn II ( minimize E) for both systems:
{
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Introduction to DFT - Myrta Grüning
How do we approximate the xc functional
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Introduction to DFT - Myrta Grüning
How to solve the KS equations in practice
{Nonlinear, integro-differential equations
1. solution through self-consistency2. basis set expansion to get an algebraic problem
{ }
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Introduction to DFT - Myrta Grüning
Solution through self-consistency
GUESSDENSITY
CALCULATEKS POTENTIAL
SOLVE KSEQUATIONS
CALCULATEENERGY/NEW DENSITY
CHECKCRITERIA
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Introduction to DFT - Myrta Grüning
Basis set expansion to get algebraic problem
Expansion in a convenient basis set
Hamiltonian (overlap) matrix elements
Solve (generalized) eigenproblem
Possible choices:Localized basis sets
e.g.: Gaussians, Slater
Delocalized basis setsPlane-waves
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Introduction to DFT - Myrta Grüning
Periodic crystals are described in terms of:
Crystal Unit cellPrimitive Lattice vectors
Basis
Reciprocal lattice vectors:
Direct, real space
1st Brillouin zone:
Fourier trasformReciprocal, momentum, k-space
Translations
Primitive reciprocalLattice vectors
translation respresented by
with
with
Wigner-Seitz primitive cell in k-space
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Introduction to DFT - Myrta Grüning
Eigenvalue/functions of electrons in a crystal
Eigenfunctions have symmetry of the systemBloch functions
Band structure
with
with k varying over the whole Brillouin zone(# k in 1BZ = # unit cells)
k
E(k)
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Introduction to DFT - Myrta Grüning
Planewave basis set
pseudopotential!
Expand:with
Diagonalize:
Matrix elements:
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Introduction to DFT - Myrta Grüning
You need to "converge" wrt these parameters
a. energy cutoff used to define the size of the planewave basis set
I need to evaluate integrals of the type(e.g. for the charge density)
numerically on a discrete (uniform) grid as:
b. number & density of k points used to sample k-space
You need to "converge" wrt these parameters
with
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Introduction to DFT - Myrta Grüning
DFT with PWs in practice:
System:
Hamiltonian: (physical approx.)
Numerical approx:
Physical quantities
1-particle quantities
GUESSDENSITY
CALCULATEKS POTENTIAL
SOLVE KSEQUATIONS
CALCULATEENERGY/NEW DENSITY
CHECKCRITERIA
Solve KS equations
IN: OUT:
RUN:
xc-approximation(relativistic effects)
unit celllattice vectorsbasis
energy cut-offk-points gridpseudopotentialsSCF procedure/threshold
density and related quantitiestotal energy and componentsany GS observable (in principle)
Kohn-Sham 1-p wavefunctionsKohn-Sham 1-p energies
Energ
y (
eV
)
L LZ A D A
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Introduction to DFT - Myrta Grüning
Connection KS and physical quantities?
Energ
y (
eV
)
L LZ A D A
10
0
5
10
15
0 5 15
LD
A B
an
d G
ap
(eV
)
Experimental Band Gap (eV)
Bandgap problem:
"looks like"experimental
results
but bandgapsystematically
too small
Is it just a xc problem?
NO:
v
c
ε
ε−A
−IKS bandgap Energy gap
Δ
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Introduction to DFT - Myrta Grüning
Starting point for excitations in MB system
n-particle propagator =
n-particle propagator in the independent particle system
+Term that brings in
correlation
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Introduction to DFT - Myrta Grüning
Choices for 1-particle wavefunction/energy
1-p model:independent
particlesHartree
independentfermions
independentparticles in
effective potential
Hartree-Fock
Kohn-Sham
partially interactingparticles in
effective potential
generalizedKohn-Sham
cost:approach:
N3
N3
N4
N4
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Introduction to DFT - Myrta Grüning
References&material&further reading
A Chemist’s Guide to Density Functional Theory. Second EditionWolfram Koch, Max C. Holthausen (2001) Wiley-VCH Verlag GmbH
A Primer in Density Functional TheoryEds. C. Fiolhais F. Nogueira M. Marques (2003) Springer-Verlag Berlin Heidelberg
Density Functional Theory - An Advanced CourseEberhard Engel · Reiner M. Dreizler (2001) Springer-Verlag Berlin Heidelberg
Kohn-Sham potentials in density functional theoryPh.D thesis - Robert van Leeuwen
Electronic Structure of Matter – Wave Functions and Density FunctionalsW. Kohn - Nobel Lecture, January 28, 1999