The box is assumed to be orthorhombic, i.e. all angles have to be
90
. With the additional options SURFACE or
POLYMER periodic boundary conditions in only one or two
dimensions, respectively, are decoupled.
Available Poisson solvers are: {HOCKNEY,TUCKERMAN,MORTENSEN}
All methods require that the charge density is zero at the border of the box. For normal systems this means that about a minimum of 3 Angstrom space between the outmost atoms and the box is required. However, for some systems (e.g. with negative CHARGE) and for high accuracy calculations this may not be enough. Some a list of additional requirements of the individual methods follows below.
The ISOLATED MOLECULE keyword has only an effect on the calculation of the degrees of freedom (3N-6 vs. 3N-3 for periodic systems) and thus the calculation of the instantaneous temperature.
CENTER MOLECULE ON/OFF: The main purpose of this is to
center the molecule (center of mass) in the box. This is needed for the
HOCKNEY Poisson solver. This solver gives wrong results if the charge
density is not centered in the computational box. All other solvers
behave like the periodic counterpart, i.e. the relative position of the
charge density and the box are not important. Further requirements:
HOCKNEY Method:
TUCKERMAN Method:
MORTENSEN Method:
Finally, for many systems using a large enough cell and periodic boundary conditions is also an option. In general, the computed properties of molecules should be independent of the scheme used (either pbc or isolated box) except in difficult cases such as charged molecules, where the calculation in an isolated box is recommended. The PBC calculation is always cheaper for a box of the same size, so for a neutral molecule such as water molecule you would save time and memory by not using SYMMETRY 0.