Multistate metadynamics¶
The core functionality of the metafalcon
package is the multistate metadynamics implementation
(J. O. Lindner, M. I. S. Röhr, R. Mitrić, Phys. Rev. A 97 (5), 052502 (2018)). In this method,
the electronic Born-Oppenheimer two-state Hamiltonian is extended by an
off-diagonal potential
that is determined by an instance of the metadynamics method
and is therefore dependent on a set of collective variables (CVs).
Diagonalization yields the effective energy gap
which is used as a CV for the multistate metadynamics run.
In order to set up the simulation, run the GUI application and check the Do multistate metadynamics option in the metadynamics tab.
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The forms below that checkbox refer to the construction of , while the Gaussian height
in the upper part of the window is used for the Gaussians added to
.
is
the threshold that is used for the
-function to switch between
and
.
The Collective Variables tab also refers to the metadynamics in . Since the torsion
angle used in the previous example is an appropriate choice for the multistate
metadynamics, we don’t make any changes in this tab.
Run the simulation:
metaFALCON run
During the simulation, two files deltaE_meta.dat and deltaE_BO.dat are written that contain the
energy gaps and
.
The offdiagonal potential is handled just as a normal metadynamics instance, so the
input information about the latter is stored in another section of the meta-config.json file. It
is distinguished from the main metadynamics instance with the extension _multistate:
{
...
"metadynamics_multistate": {
"collective variables": [...],
"tau_g": ...,
...
},
...
}
This extension is needed later when referring to the multistate instance again, for example when
reconstructing :
metaFALCON reconstruct --extension multistate