Module 1: DFT Flashcards

1
Q

Main Challenges for DFT

A
  • dispersion forces
    • due to long-range correlations between zero-point fluctuations of dipole moments
    • (semi-)local functionals cannot capture this long-range interactions
  • overbinding
    • usually leads to higher energies, shorter bond lengths, etc.
  • self-interaction
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2
Q

Dispersion Correction

A
  • correct for dispersion by adding dispersion energy to Kohn-Sham energy
  • different methods
    • DFTD3
    • TS-vdW
    • vdW-DF
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3
Q

Dispersion Energy

A
  • Dispersion energy determined by dispersion coefficients Cx and separation distance rx
    • C6 ≡ vdW/London dispersion
    • calculated analytically using Casimir-Polder formula
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4
Q

DFTD3

A
  • uses C6, C8 terms to calculate dispersion energy
  • use AmHn/BkHl referece hydrides to compute molecular polarizabilities α() and subtract contribution due to H2 component
    • Requires TDDFT calculations
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5
Q

TS-vdW

A
  • semi-empirical
  • Calculate effective C6,AB using geometric-like mixing of effective same-species C6,ii weighted by static polarizabilities
  • Effective C6,ii modified by Hirschfield colume partitioning function
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6
Q

Local Density Approximation

(Overview)

A
  • uses per electron exchange-correlation energy of homogeneous electron gas
    • exchange known analytically
    • correlation known analytically or numerically exact
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7
Q

Local Density Approximation

(Good Performance)

A
  • structural, elastic, and vibrational properties
  • material science
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8
Q

Local Density Approximation

(Bad Performance)

A
  • overbinds → binding energies too high
  • underestimates lattice constants
  • unreliable activation energies for chemical reactions
  • energetics of magnetic materials
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9
Q

Generalized Gradient Approximation

(Overview)

A
  • enhancement factor Fxc over LDA
    • contains next term in derivative expansion of density
  • no universal form
    • e.g. PBE (Perdew-Burke-Ernzerhof)
  • more repulsive core-valence xc → increase in bulk lattice contants
  • reduced valence effects → decrease in cohesive energies
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10
Q

Generalized Gradient Approximation

(Good Performance)

A
  • atomic and molecular total energies improved
  • corrects LDA overbinding
  • improved activation energies (still too low, though)
  • more relaistic magnetic solids
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11
Q

Generalized Gradient Approximation

(Bad Performance)

A
  • softened bonds → increase lattice constants
  • dispersion not included
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12
Q

Exchange Correlation Exact Definition

A
  • Coulomb interaction between electron at r and value of xc-hole nxc(r,r’) at r
    • nxc not known exactly
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13
Q

Hybrid Functionals

A

e.g. B3LYP

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14
Q

vdW-DF

A
  • adds non-local term with kernal function
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15
Q

TDDFT

A
  • uses Runge-Gross Theorem for quantum mechanical action to define xc energy
  • requires new functionals that include (non-)locality in space and time
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