Density Functional Theory Flashcards

1
Q

Why are ab-initio MO-based methods (HF, MCSCF, CISD, MP2, CCSD(T),…) are called wavefunction-based methods?

A

They compute energy as a functional of a wavefunction
E = f(Y(r))

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2
Q

Functional

A

Something that changes a function into a value

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3
Q

Function and operator

A

Function: value into a value
Operator: function into a function

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4
Q

Density functional theory

A

Incorporation of quantum mechanics into density-functional ideas

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5
Q

Why was it hoped that density based methods may be faster than wavefunction based methods?

A

Wavefunction base methods = function of 3N dimensions (N = number of electrons) so involve a lot of integrals. But for a stationary state of moving charged particles, E could be expressed as a functional of electron density which is only 3 dimensions (less integrals)

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6
Q

Hohnberg-Kohn existence theorem

A

For electronic systems, there exists a functional Ehk such that the Schrodinger equation becomes E = Ehk[p] where p(r) is the true electron density of stationary state

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7
Q

Hohnberg-Kohn variational theorem

A

For every approximate or trial density, if p(trial) is not equal to p(true), Ehk[p(trial)] is greater than or equal to than Etrue

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8
Q

Challenges of DFT theory

A

(1) How to generate good electron densities
(2) Ehk is unknown - how to approximate

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9
Q

How is problem (1) solved?

A

Kohn Sham MO’s are obtained with an SCF procedure but are variationally optimized to suit a different energy expression

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10
Q

Kohn-Sham SCF technique

A

p(trial) is built from Slater determinants of ‘N’ orbitals
The KS MO’s are obtained through an SCF procedure, but are variationally optimized to suit a different energy

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11
Q

Which term in Ehk is varied in DFT

A

The fourth term (exchange correlation functional)

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12
Q

Exchange correlation functionals

A

Usually taken as the sum of Ex[p] (exchange functional - Fermi correlation) and Ec[p] (correlation functional - Coulomb)

Require numerical integration

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13
Q

GGA DFT calculation comparison to HF

A

Slower than HF, but faster than MP2 and almost as accurate, thus cost effective for molecules 8-50 atoms, as well as solid state calculations

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14
Q

What forces to DFT methods do poorly for

A

London-dispersion forces and complexes

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15
Q

Geometry errors (DFT)
(mean average, Angstroms)

A

0.008 B2LYP
0.011 B3PW91

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16
Q

Dipole moment errors

A

u (MP2) ~ u (GGA)