Resgrg:comp-photo-version control-codes
This page explains the local modifications made to the Gaussian code by the group. Hopefully it'll also explain how to use them as well.
The codes
Shaopeng
This is a replacement for the existing matrix element generator (hereafter known as the Klene code)
that is used for large (number of orbitals > 8)
CASSCF calculations. If your job shows SME calculated on fly
then it's using this path.
The Shaopeng code computes the same matrix elements but does it faster, and in a way that allows certain compiler optimisations to be used. The result should be an approximate 4X speedup, depending on the job and the architecture that you're running on. This speedup comes at a cost of memory. The algorithm is much more demanding of memory and this extra demand scales with the number of processors.
How to use it: by default l510 will make a decision on whether to use the Klene code path or the Shaopeng based on the problem size and the amount of memory and processors allocated. You can force one code path over the other with the IOP(5/139=x) where:
Iop(5/139) | Effect |
---|---|
0 | Default, choose code path automatically |
1 | Force Klene code path |
2 | Force Shaopeng code path |
Seamfollowing
Dunno
ONIOM Freq
Shows contributions of sub-calculations to the ONIOM frequency according to the formula:
The sub-calculation terms are obtained from the diagonal elements after transformation of the sub-Hessians with the ONIOM normal modes. This gives the curvature of each sub-calculation PES with respect to the ONIOM mode so we can see how the ONIOM PES is determined i.e. if a transition state located using ONIOM has an imaginary mode comprised of three real sub-components, then the transition state is a result of the extrapolation and is not consistent with the underlying calculations. This result suggests caution should be used as the stationary point may be spurious.
The ONIOM frequency analysis is called using IOp(7/123=1):
IOp(123) ... Print partitioning of ONIOM vibrational frequencies into contributions from individual sub-calculations. see Vreven et al. JCTC, 2012, DOI: 10.1021/ct300612m 0 ... Don't do ONIOM frequency analysis 1 ... Do ONIOM frequency analysis
Example output:
Mode Low-Real Low-Model High-Model Total 1 2181.3672 433.6860 231.1949 2150.2862 2 4029.7184 2543.4278 2310.9318 3887.1598 3 4317.3046 869.1994 789.5792 4301.9818