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The CC2 ground-state energy
is--similarly to other coupled-cluster energies--obtained
from the expression
ECC |
= 〈HF| H| CC〉 = 〈HF| H exp(T)| HF〉 , |
(9.1) |
|
= ESCF +  tabij + taitbj![$\displaystyle \Big]$](img137.png) 2(ia| jb) - (ja| ib) , |
(9.2) |
where the cluster operator T is expanded as
T = T1 + T2 with
T1 |
= taiτai |
(9.3) |
T2 |
=  taibjτaibj |
(9.4) |
(for a closed-shell case; in an open-shell case an additional spin
summation has to be included).
The cluster amplitudes tai and taibj are obtained as solution
of the CC2 cluster equations [101]:
Ωμ1 |
= 〈μ1| + [ , T2]| HF〉 = 0 , |
(9.5) |
Ωμ2 |
= 〈μ2| + [F, T2]| HF〉 = 0 , |
(9.6) |
with

= exp(-
T1)
H exp(
T1),
where μ1 and μ2 denote, respectively, the sets
of all singly and doubly excited determinants.
The residual of the cluster equations
Ω(tai, taibj) is the
so-called vector function.
The recommended reference for the CC2 model is ref. [101],
the implementation with the resolution-of-the-identity approximation, RI-CC2,
was first described in ref. [10].
Subsections
Next: Advantages of the RI
Up: Second-Order Approximate Coupled-Cluster (CC2)
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