Hey Christoph,
"> I guess if you would have an infinitely long trajectory and hence
> infinitely long blocks the ends should go to 0.
> We implemented this after https://doi.org/10.1007/978-94-010-0173-1_7,
> so you can have a look at that as well. "
I agree, but only in a scenario where the potential form of choice (pairwise for example) is indeed such that allows you to reproduce the forces. Maybe some systems require multi-body terms or some things like that.
In any case, sorry, because my sentence "
I mean, how do they the value of (F_il,model - Fil,ref)^2, which should ideally be 0, at each point?" was not well written. it should be "I mean, how do these errors relate to the value of (F_il,model - Fil,ref)^2, (...), at each point?"
What I mean is: if you have for example more than one superatom type, you will have minimum 3 pairwise potentials: 1-1, 1-2, 2-2. Each of them will be a separate .force output file and have its own reported "error". But if you look at force-matching's formalism as develop by Voth (which is the one implemented in VOTCA), they work with equations for the global, total force acting on each atom i. So in fact I was curious to know what are these individual errors of 1-1, 1-2 and 2-2 (i.e., how are they calculated by VOTCA?).
"> The paper is from 2009, let me see if I can still find it. Please send
> me your github username in an email."
I sent you an email :)
If I somehow emailed the wrong Christoph Junghans and you didnt receive anything, you can feel free to email me instead:
cecilia.sar...@umontpellier.fr