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17 THE DENSITY FUNCTIONAL PROGRAM 114<br />

17.4 Density Functionals<br />

In the following, ρ α and ρ β are the α and β spin densities; the total spin density is ρ;<br />

The gradients of the density enter through<br />

σ αα = ∇ρ α · ∇ρ α ,σ ββ = ∇ρ β · ∇ρ β ,σ αβ = σ βα = ∇ρ α · ∇ρ β ,σ = σ αα + σ ββ + 2σ αβ (5).<br />

χ α =<br />

√<br />

σαα<br />

ρ 4/3 α<br />

, χ β =<br />

√ σββ<br />

ρ 4/3<br />

β<br />

. (6)<br />

υ α = ∇ 2 ρ α ,υ β = ∇ 2 ρ β ,υ = υ α + υ β . (7)<br />

Additionally, the kinetic energy density for a set of (Kohn-Sham) orbitals generating the density<br />

can be introduced through<br />

τ α =<br />

α<br />

∑<br />

i<br />

|∇φ i | 2 ,τ β =<br />

β<br />

∑<br />

i<br />

|∇φ i | 2 ,τ = τ α + τ β . (8)<br />

All of the available functionals are of the general form<br />

F [ρ s ,ρ ¯s ,σ ss ,σ ¯s ¯s ,σ s ¯s ,τ s ,τ ¯s ,υ s ,υ ¯s ] =<br />

∫<br />

d 3 rK (ρ s ,ρ ¯s ,σ ss ,σ ¯s ¯s ,σ s ¯s ,τ s ,τ ¯s ,υ s ,υ ¯s ) (9)<br />

where ¯s is the conjugate spin to s.<br />

Below is a list of keywords for the functionals supported by <strong>MOLPRO</strong>. Additionally there are<br />

a list of alias keywords deatailed in the next section for various combinations of the primary<br />

functionals listed below.<br />

PBEC<br />

PW86<br />

B95<br />

TH4<br />

TH2<br />

ECERF<br />

PBE Correlation Functional<br />

doi:10.1103/PhysRevLett.77.3865<br />

.. GGA Exchange Functional.<br />

doi:10.1103/PhysRevB.33.8800<br />

Becke 1995 Correlation Functional.<br />

tau dependent Dynamical correlation functional.<br />

doi:10.1063/1.470829<br />

.. Density an gradient dependent first and second row exchangecorrelation<br />

functional.<br />

doi:TH3/4<br />

.. Density and gradient dependent first row exchange-correlation<br />

functional.<br />

doi:10.1021/jp980259s<br />

Short-range LDA correlation functional. Local-density approximation<br />

of correlation energy<br />

for short-range interelectronic interaction erf(µr 21 )/r 12 ,<br />

S. Paziani, S. Moroni, P. Gori-Giorgi, and G. B. Bachelet, Phys.<br />

Rev. B 73, 155111 (2006).<br />

(<br />

[φ 2 (ζ )] 3 √ ) µ rs<br />

Q<br />

εc<br />

SR (r s ,ζ , µ) = εc PW92<br />

φ 2<br />

+ a<br />

(ζ ) 1 µ 3 + a 2 µ 4 + a 3 µ 5 + a 4 µ<br />

(r s ,ζ )−<br />

(1 + b 2 0 µ2 ) 4

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