sanya
sanya@photonics.ru
My experience in the study of E/Z photoisomerization says that minimal basis set is never sufficient, especially for conical intersections. At conical intersections, the shape of the molecule is severely distorted, and the basis set should be sufficiently flexible to allow for these distortions; otherwise, you can miss the necessary stationary point or conical intersection.
For example, a comprehensive CASSCF/XMCQDPT study of photoisomerization of stilbene was performed by Alex (http://pubs.acs.org/doi/abs/10.1021/ct400647w). The authors use cc-pVTZ basis set. For qualitative results, double-zeta basis set with polarization functions is OK.
Now, your inputs. For active space (8 electrons, 8 orbitals), CISTEP=ALDET in $mcscf and DISTCI= If you use a multicore computer, set: $smp load=0 call64=.t. smppar=.t. $end For cluster add this line (actually, I do not remove this line in single-node calculations, it does no harm): $p2p p2p=.t. dlb=.t. $end (you can add mixed=.t. if the nodes of your cluster differ from each other) This line is mandatory: $trans mptran=2 dirtrf=.t. aoints=dist altpar=.t. mode=112 $end This line speeds up CASCI step: $ciinp castrf=.t. $end This line is for CISTEP=GUGA if you prefer to use it: $gugem pack2=.t. $end For CASSCF (that is, _complete_ rather than _restricted_ active space SCF) calculations, _remove_ fors=0 and IEXCIT key. You need _all_ excitations within the given active space. The default is fors=1 (aka CAS). With these keys, you'll be surprised how fast CASSCF can be.
Fri Apr 24 '15 3:48am
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