[CP2K-user] IC-QMMM with single charge in front of a metal plane: open boundary corrections
Katharina Doblhoff-Dier
k.doblh... at lic.leidenuniv.nl
Wed Jun 24 13:23:48 UTC 2020
Dear CP2K community,
I am confused about the IC-QMMM method as implemented in CP2K. I am not
100% sure whether my question is related to my misunderstanding of the
method (as implemented) or on how to use it.
Originally, my confusion came from my not-understanding of the parameter
V_0 (i.e., EXT_POTENTIAL in the CP2K implementation): In periodic boundary
conditions, this parameter does not seem to make much sense to me:
Depending on the average potential in the quantum region, defining V_0 will
make the charge Q on the metal adapt in such a way that the average
potential in the cell is zero (I know that the latter is logic, but in view
of this, the physical meaning of V_0 becmes unclear to me):
[image: tmp1.png]
Alternatively, if a charge is put into the QM part (e.g. an H2+) and V0 is
adjusted such that the total charge Q on the metal is exaclty -1, a
spurious field will result over the cell (due to Ewald summation) and
again, V_0 does not have an obvious physical meaning.
[image: tmp2.png]
Considering that the periodic boundary conditions lead to lots of spurious
stuff, I then tried to go to MT boundary corrections or the IMPLICIT
poisson solver as implemented in CP2K. This gave me the following results
(note that I shifted the green and the blue curve by 0.4V for better
comparison)
red: IMPLICIT poissn solver with Neumann BC at z=0 and z=60 and
homogeneous Dirichlet BC at z=30
green: MT (Martyna-Tuckerman) poisson solver (shifted by 0.4V)
blue: normal Ewald summation (shifted by 0.4V)
[image: tmp3.png]
The corresponding V_0 (optimized such that Q=-1) were 1.11V for IMPLICIT
boundary conditions, 1.24V for MT boundary conditions and -0.37V for
periodic boundary conditions. While for periodic boundary conditions (blue
line) this can be seen to correspond to the potential in the metal part,
this is not the case for MT boundary conditions (green), where the
potential in the metal varies from about -0.4 to -0.5 (remember that I
shifted the curves by 0.4 volt) and for IMPLICIT boundary conditions.
Overall, to me, it looks as if the IC-QMMM method was ignoring the boundary
conditions and optimizing the charges for the periodic boundary conditions
and then keeping them fixed no matter what I set as POISSON_SOLVER. In the
MT boundary condition case (geen) we can thus see the influence of the
charges shieding the (spurious) field in periodic boundary conditions
(hence the slope in the metal part, which has the same slope as the average
field in the periodic solver).
Finally, I decided that, in principle, it should be possible to find an
energy minimum when Q_image=-Q_QM (as also shown in the original paper by
Siepmann and Sprik). With none of the boundary conditions could I find this
minimum correctly. However, here comes my non-understanding of Eq. 4 in the
paper by Golze, Iannuzzi, ..., and Hutter
(https://pubs-acs-org.ezproxy.leidenuniv.nl:2443/doi/10.1021/ct400698y)
into play: Here, the energy is written as:
[image: tmp4.png]
I would have thought this to be a grand canonical energy (grand canonical
only in the charges on the metal) expression, where the last term accounts
for the -N_i*mu_i term. Again, this does not seem physical to me if I think
of a capacitor (or a charge+image charge in a box that is periodic in x and
y, as I would then expect a correction for the charges in the QM region too
(unless the vacuum potential on the QM side is zero and open boundary
conditions are used, but likely this is wrong and this may be where my
entire confusion starts.
So summarizing, this boils down to a few questions:
1.) can the IC-QMMM method be combined with poisson solvers other than
periodic? If so, how? I simply set the poisson solver in the MM and the DFT
part.
2.) What do I need to do in order to find an energy minimum for
Q_image=-Q_QM?
3.) What is the meaning of V_0 and why is it substracted in the energy
expression.
Any physical insight is appreciated!
Thank you and best regards,
Katharina
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