Ground State Properties, Gradients and Geometries

L^{ur CC2}(t,, β) |
= | 〈HF| H| CC〉 + 〈μ_{1}| + [, T_{2}]| HF〉 |
(9.12) |

+ 〈μ_{2}| + [F_{0} + β, T_{2}]| HF〉 |

with

〈V〉^{ur CC2} |
= | ℜ = D^{ur}_{pq} V_{pq} , |
(9.13) |

= | ℜ〈HF|| HF〉 + 〈μ_{1}| + [V, T_{2}]| HF〉 |
(9.14) | |

+ 〈μ_{2}|[, T_{2}]| HF〉 , |

where ℜ indicates that the real part is taken.

L^{rel CC2}(t,) |
= | 〈HF| H| CC〉 + 〈μ_{1}| + [, T_{2}]| HF〉 |
(9.15) |

+ 〈μ_{2}| + [F, T_{2}]| HF〉 + F_{μ0} , |

where

〈V〉^{rel CC2} |
= | ℜ〈HF|| HF〉 + 〈μ_{1}| + [V, T_{2}]| HF〉 |
(9.16) |

+ 〈μ_{2}|[V, T_{2}]| HF〉 + V_{μ0} , |
|||

= | D^{rel}_{pq} V_{pq} . |
(9.17) |

The calculation of one-electron first-order properties requires that in addition to the cluster equations also the linear equations for the Lagrangian multipliers are solved, which requires similar resources (CPU, disk space, and memory) as the calculation of a single excitation energy. For orbital-relaxed properties also a CPHF-like linear equation for the Lagrangian multipliers needs to be solved and the two-electron density has to be build, since it is needed to set up the inhomogeneity (right-hand side). The calculation of relaxed properties is therefore somewhat more expensive--the operation count for solving the so-called Z-vector equations is similar to what is needed for an SCF calculation--and requires also more disk space to keep intermediates for the two-electron density--about

The calculation of the gradient implies the calculation of the same variational densities as needed for relaxed one-electron properties and the solution of the same equations. The construction of the gradient contributions from the densities and derivative integrals takes about the same CPU time as 3-4 SCF iterations and only minor extra disk space. For details of the implementation of CC2 relaxed first-order properties and gradients and a discussion of applicability and trends of CC2 ground-state equilibrium geometries see ref. [13]. The following is in example input for a MP2 and CC2 single point calculation of first-order properties and gradients:

$ricc2 mp2 cc2 $response static relaxed operators=diplen,qudlen gradientA different input is required for geometry optimizations: in this case the model for which the geometry should be optimized must be specified in the data group

`$ricc2`

by the keyword `geoopt`

:
$ricc2 mp2 cc2 geoopt model=cc2

For CC2 calculations, the single-substitution part of
the Lagrangian multipliers
are saved in the file
`CCL0--1--1---0`

and can be kept for a restart (for MP2 and
CCS, the single-substitution part
vanishes).

For MP2 only relaxed first-order properties and gradients are implemented (unrelaxed MP2 properties are defined differently than in CC response theory and are not implemented). For MP2, only the CPHF-like Z-vector equations for need to be solved, no equations have to be solved for the Lagrangian multipliers . CPU time and disk space requirements are thus somewhat smaller than for CC2 properties or gradients.

For SCF/CIS/CCS it is recommended to use the modules
`grad` and `rdgrad` for the calculation of,
ground state gradients and first-order properties.