Dear Juerg,
thanks for your answer. Whilst I am using an SCF convergence of 10e-6 as you suggest, I am not using the conjugate gradient OT minimizer but DIIS instead. Perhaps something to try out, I will give it a go. What I was wondering about is, if there is a possibility to control these sort of parameters for individual replicas.
The electronic structure will change quite a bit as one traverses along the profile between starting and last point, hence I wouldn't expect too much of a problem with the first point, but more towards the transition state. Anyways, I guess it is more reasonable to control the SCF globally for all points.
Another question I have in this context, is there a rule of thumb for how many intermediate structures for NEB should be provided? At the moment I am using a starting structure, a guess for the TS plus a final structure. With 8 replicas defined, the algorithm should interpolate between these. I was successful to localise
one transition state with this already, however, for other transition states things are more complicated. Also, in cases I observe rather strange energy profiles, in which the first (sometimes also the last) point lies higher in energy then the remaining points (see attachment). This is somewhat surprising, since the first point corresponds to an optimised structure (I am assuming that the first replica correlates with my first starting structure). Inspection of the
movie.xyz generated from the individual BAND files reassures me that I am looking at a reasonable trajectory. Is is worth waiting for this calculation to converge to some stationary point, or should I come up with a better setup in terms of structures?
Thanks for the advice
Tobias