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Molecular Modeling: Density Molecular Modeling: Density Functional TheoryFunctional Theory
C372Introduction to Cheminformatics II
Kelsey Forsythe
RecallRecall
Molecular Models
Empirical/Molecular Modeling Semi Empirical Ab Initio/DFT
Neglect ElectronsNeglect Core Electrons
Approximate/parameterize HF IntegralsFull Accounting of Electrons
Full Quantum MethodsFull Quantum Methods
Quantum Methods
Wavefunction Density Function
Hartree-Fock DFT
MP2, CI
Basis Set MethodsBasis Set Methods
NN44 dependence on # electrons dependence on # electrons Does not account for direct e-e Does not account for direct e-e
correlation (communication)correlation (communication) Perturbation theory (Moller-Plesset Perturbation theory (Moller-Plesset
methods)methods) Configuration interactionConfiguration interaction
Configuration Interaction Configuration Interaction (CI)(CI)
∑=
Φ+Φ=ΨN
i
HFii
HF aa1
00
unoccupied
occupied
Moller Plesset (MP)Moller Plesset (MP)
Hartree-Fock Hartree-Fock close to Full close to Full HamiltonianHamiltonian
VHH HFexact λ+= 0
Perturbation
DFTDFT
Replaces 3N spatial coordinate Replaces 3N spatial coordinate and N-spin coordinate wave and N-spin coordinate wave function with functionalfunction with functional Reduces # integrationsReduces # integrations Simplifies computations?Simplifies computations?
What is Density?What is Density?
Density provides us Density provides us information about information about how something(s) how something(s) is(are) is(are) distributed/spread distributed/spread about a given spaceabout a given space
For a chemical system For a chemical system the electron density the electron density tells us where the tells us where the electrons are likely to electrons are likely to exist (e.g. allyl)exist (e.g. allyl)
€
qr = n j *j
∑ a jr2
1111 ad∫ =Ψ τφ
What is Density?What is Density?
Allyl Cation: Allyl Cation:
ΨΨ∝ *ρ
What is Density?What is Density?
For a chemical system the For a chemical system the electron density tells us where electron density tells us where the electrons are likely to existthe electrons are likely to exist
Sum over all space gives total # Sum over all space gives total # electronselectrons
Nxdx
x
xdxdxddsxxxNx NN
=
=∞→
Ψ=
∫
∫ ∫
11
1
321
2
211
)(
0)(
...)...,(....)(
vv
v
vvvvvvv
ρ
ρ
ρ
Probability of finding any electron within dx1 while other electrons are elsewhere
∑ =i
iq 2Allyl cation
FunctionFunction
A function maps a set of numbers A function maps a set of numbers to another set of numbersto another set of numbers Ex. F(X)=XEx. F(X)=X
1234
1234
F(X)=Y
What’s a Functional?What’s a Functional?
A function of a functionA function of a function How does it differ from simple How does it differ from simple
function? function?
FunctionalFunctional
A function which maps a set of A function which maps a set of functions to a set of numbersfunctions to a set of numbers Ex. Ex. FF(A(X),B(X),C(X),….)=X(A(X),B(X),C(X),….)=X
A(X)B(X)C(X)D(X)
2013F1234
FunctionalFunctional
A function which maps a set of A function which maps a set of functions to a set of numbersfunctions to a set of numbers Ex. Energy is a functional of the Ex. Energy is a functional of the
wave functionwave function
€
< E >=Ψ*(
v r ) ˆ H Ψ(
v r )d
v r ∫
Ψ*(v r )Ψ(
v r )d
v r ∫
≡ average /expectation value of observable E
Goal?Goal?
Energy
Potential
Density
How now brown cow?
Energy From Density?Energy From Density?Classical ApproachClassical Approach
Nuclear-Electron InteractionNuclear-Electron Interaction
Electron-Electron InteractionElectron-Electron Interaction
€
Vne =Zk
v r −
v r k
∫k
nuclei
∑ ρ(v r )d
v r
Ve1e2=
1
2
ρ(v r 1)ρ(
v r 2)
v r 1 −
v r 2
dv r 1d
v r 2∫∫ Quantal Effects:
Exchange?Correlation?
Energy From Density?Energy From Density?
Electron-Electron InteractionElectron-Electron Interaction
);()(
2
1)()(
2
1
)()(
2
1
2121
21121
21
21
2121
21
21
21
∫∫∫∫
∫∫
−+
−=
++−
=
rdrdrr
rrhrrdrd
rrrr
V
nCorrelatioExchangerdrdrrrr
V
ee
ee
vvvv
vvvvv
vvvv
vvvvvv
ρρρ
ρρ
Exchange & Correlations
Hole function
Energy From Density?Energy From Density?
Kinetic EnergyKinetic Energy Thomas-Fermi’s uniform metallic Thomas-Fermi’s uniform metallic
electron gaselectron gas
€
Te ≈ Tueg =3
10(3π 2)2 / 3 ρ 5 / 3(
v r )d
v r ∫
Hohenberg-KohnHohenberg-Kohn
Existence TheoremExistence Theorem
Variational TheoremVariational Theorem
BUTBUT Don’t know how to guess density formDon’t know how to guess density form Don’t want to have to calculate wavefunctionDon’t want to have to calculate wavefunction
exactguessguessguess EE
E
≥∴Ψ→
→
ρ
ρ
Energy Functional Existence Energy Functional Existence (Hohenberg-Kohn (1965))(Hohenberg-Kohn (1965))
For a given system of non-For a given system of non-interacting electron in the interacting electron in the presence of an external field presence of an external field (nuclei) there exists:(nuclei) there exists:[ ]
[ ] [ ] rdrFrdrVrE
ts
rdVTrF
ne
vvvvv
vv
)()()(
..
)̂ˆ()( *
ρρρ
ρ
+=
Ψ+Ψ≡
∫
∫
What is this?
Functional Form?Functional Form?
For a given system of non-For a given system of non-interacting electrons in the interacting electrons in the presence of an external field presence of an external field (nuclei):(nuclei):
€
F ρ(v r )[ ] ≡ Ψ*∫ ( ˆ T + ˆ V )Ψd
v r
≡ (Fkinetic + Fpotential )
What is this?
Kohn-Sham Self Consistent Kohn-Sham Self Consistent field Methodologyfield Methodology
For a given system of non-For a given system of non-interacting electrons in the interacting electrons in the presence of an external field presence of an external field assume they have a density of assume they have a density of some some realreal system or system or replaced by replaced by
∑=
→
−
iii
realreal
realeractingnon
rcr )()(
int
φχ
χρ
ρρ
HF-like
Functional Form?Functional Form?
HF-like?HF-like?
ni=non-ni=non-interactinginteracting
€
F ρ(v r )[ ] ≡ Ψ*∫ ( ˆ T + ˆ V )Ψd
v r
≡ (Fkinetic
?1 2 3 + Fcoulomb
Poisson1 2 3 + Fexchange + Fcorrelation
?1 2 4 4 4 3 4 4 4
)
Fkinetic = Tni + ΔT
F? ρ(v r )[ ] ≡ DFT input
What is this?
DFT ProcedureDFT Procedure Guess electron densityGuess electron density Choose basisChoose basis Calculate KS-integrals for TCalculate KS-integrals for Tnini and V and Vnene using basis using basis Calculate remaining integrals usingCalculate remaining integrals using Solve matrix equations (just as in HF-SCF) Solve matrix equations (just as in HF-SCF) Calculate new electron density ( )Calculate new electron density ( ) Repeat to error tolerance until difference betweenRepeat to error tolerance until difference between minimizedminimized
0ρ
0ρ
newρ
€
ρ0 and ρ new
DFT Challenge( )DFT Challenge( ) Determining the Determining the
form of the form of the exchange-correlation exchange-correlation functionalfunctional LDA-Local Density LDA-Local Density
ApproximationApproximation Uniform electron gasUniform electron gas
Becke Exchange Becke Exchange Correction (1988)Correction (1988) Asymptotic correctionAsymptotic correction
Lee-Yang-Parr(1988)Lee-Yang-Parr(1988) Correlation correctionCorrelation correction
0ρ
321 )(3/1 ρρ FCFF correx +=+
QM-MC simulationsCeperly and Alder(1980)
DFT-SummaDFT-Summa
Exact (by construction)!Exact (by construction)! Includes CorrelationIncludes Correlation Includes ExchangeIncludes Exchange
Approximate (by application)Approximate (by application)
NOT variational as a result (E<ENOT variational as a result (E<Eexactexact))
€
F ρ(v r )[ ] ≡ Ψ*∫ ( ˆ T + ˆ V )Ψd
v r
F ρ(v r )[ ] ≡ DFT input ≡ unknown
DFT-SummaDFT-Summa
Does not describe:Does not describe: Dispersion Forces (due to LDA)Dispersion Forces (due to LDA) DynamicsDynamics
No phasesNo phases Transition probabilitiesTransition probabilities No resonance and interference Includes No resonance and interference Includes
ExchangeExchange
ScalingScaling
€
N 3 vs N 4 (ab initio)