When a local MP2 job (requested by the LOCAL_MP2 option for CORRELATION) is performed, the first new step after the SCF calculation is converged is to extract a minimal basis of polarized atomic orbitals (EPAOs) that spans the occupied space. There are three valid choices for this basis, controlled by the PAO_METHOD and EPAO_ITERATE keywords described below.
Non-iterated EPAOs: The initial guess EPAOs are the default for
local MP2 calculations, and are defined as follows. For each atom, the
covariant density matrix (SPS) is diagonalized, giving eigenvalues which
are approximate natural orbital occupancies, and eigenvectors which are
corresponding atomic orbitals. The eigenvectors with largest
populations are retained (where is the minimal basis dimension for
the current atom). This non-orthogonal minimal basis is symmetrically
orthogonalized, and then modified as discussed in
Int. J. Quantum Chem.
(2000), 76, pp. 169. to ensure that these functions rigorously span the occupied space of the full SCF calculation that has just been performed. These orbitals may be denoted as EPAO(0) to indicate that no iterations have been performed after the guess. In general, the quality of the local MP2 results obtained with this option is very similar to the EPAO option below, but it is much faster and fully robust. For the example of the torsional barrier calculations discussed above, 657 J. Chem. Phys.
(2000), 112, pp. 3592. the TRIM RMS deviations of 0.03 kcal/mol from full MP2 calculations are increased to only 0.04 kcal/mol when EPAO(0) orbitals are employed rather than EPAOs.
EPAOs: EPAOs are defined by minimizing a localization functional
as described in Ref.
Int. J. Quantum Chem.
(2000), 76, pp. 169. . These functions were designed to be suitable for local MP2 calculations, and have yielded excellent results in all tests performed so far. Unfortunately the functional is difficult to converge for large molecules, at least with the algorithms that have been developed to this stage. Therefore it is not the default, but is switched on by specifying a (large) value for EPAO_ITERATE, as discussed below.
PAO: If the SCF calculation is performed in terms of a molecule-optimized minimal basis, as described in Chapter 4, then the resulting PAO-SCF calculation can be corrected with either conventional or local MP2 for electron correlation. PAO-SCF calculations alter the SCF energy, and are therefore not the default. This can be enabled by specifying PAO_METHOD as PAO, in a job which also requests CORRELATION as LOCAL_MP2.
A local MP2 calculation (requested by the LOCAL_MP2 option for CORRELATION) consists of the following steps:
After the SCF is converged, a minimal basis of EPAOs are obtained.
The TRIM (and DIM) local MP2 energies are then evaluated (gradients are not yet available).
Details of the efficient implementation of the local MP2 method described above are reported in the recent thesis of Dr. Michael Lee. Here we simply summarize the capabilities of the program. The computational advantage associated with these local MP2 methods varies depending upon the size of molecule and the basis set. As a rough general estimate, TRIM MP2 calculations are feasible on molecule sizes about twice as large as those for which conventional MP2 calculations are feasible on a given computer, and this is their primary advantage. Our implementation is well suited for large basis set calculations. The AO basis two-electron integrals are evaluated four times. DIM MP2 calculations are performed as a by-product of TRIM MP2 but no separately optimized DIM algorithm has been implemented.
The resource requirements for local MP2 calculations are as follows:
Memory: The memory requirement for the integral transformation does not exceed , and is thresholded so that it asymptotically grows linearly with molecule size. Additional memory of approximately 32 is required to complete the local MP2 energy evaluation.
Disk: The disk space requirement is only about , but is not governed by a threshold. This is a very large reduction from the case of a full MP2 calculation, where, in the case of four integral evaluations, /4 disk space is required. As the local MP2 disk space requirement is not adjustable.
The evaluation of the local MP2 energy does not require any further customization. An adequate amount of MEM_STATIC (80 to 160 MB) should be specified to permit efficient AO basis two-electron integral evaluation, but all large scratch arrays are allocated from MEM_TOTAL.
$molecule 0 1 C C 1 1.32095 C 2 1.47845 1 121.19 O 3 1.18974 2 123.83 1 180.00 H 1 1.07686 2 121.50 3 0.00 H 1 1.07450 2 122.09 3 180.00 H 2 1.07549 1 122.34 3 180.00 H 3 1.09486 2 115.27 4 180.00 $end $rem METHOD local_mp2 BASIS 6-311g** $end @@@ $molecule 0 1 C C 1 1.31656 C 2 1.49838 1 123.44 O 3 1.18747 2 123.81 1 92.28 H 1 1.07631 2 122.03 3 -0.31 H 1 1.07484 2 121.43 3 180.28 H 2 1.07813 1 120.96 3 180.34 H 3 1.09387 2 115.87 4 179.07 $end $rem METHOD local_mp2 BASIS 6-311g** $end