The NWChem Electrostatic Potential (ESP) module derives partial atomic charges that fit the quantum mechanical electrostatic potential on selected grid points.
The ESP module is specified by the NWChem task directive
task esp
The input for the module is taken from the ESP input block
ESP
...
END
The grid points for which the quantum mechanical electrostatic potential is evaluated and used in the fitting procedure of the partial atomic charges all lie outside the van der Waals radius of the atoms and within a cutoff distance from the atomic centers. The following input parameters determine the selection of grid points.
- If a grid file is found, the grid will be read from that file. If no grid file is found, or the keyword
recalculate
is given, the grid and the electrostatic potential is recalculated.
- The extent of the grid is determined by the
range
keyword
range <real rcut>
where rcut
is the maximum distance in nm between a grid point and any of the atomic centers.
When omitted, a default value for rcut of 0.3 nm is used.
- The grid spacing is specified by the
spacing
keyword
spacing <real spac>
where spac
is the grid spacing in nm for the regularly spaced grid points.
If not specified, a default spacing of 0.05 nm is used.
- The van der Waals
radius
of an element can be specified by
radius <integer iatnum> <real atrad>
where iatnum is the atomic number for which a van der Waals radius of atrad in nm will be used in the grid point determination.
Default values will be used for atoms not specified.
- The
probe
radius in nm determining the envelope around the molecule is specified by
probe <real probe default 0.07>
- The distance between atomic center and probe center can be
multiplied by a constant
factor
specified by
factor <real factor default 1.0>
All grid points are discarded that lie within a distance factor*(radius(i)+probe)
from any atom i.
- Schwarz screening is applied using
screen [<real scrtol default 1.0D-5>]
Additional constraints to the partial atomic charges can be imposed during the fitting procedure.
- The net charge of a subset of atoms can be constrained using
constrain <real charge {<integer iatom>}
where charge
is the net charge of the set of atoms {iatom}
. A negative atom number iatom can be
used to specify that the partial charge of that atom is substracted in the sum for the set.
- The net charge of a sequence of atoms can be constrained using
constrain <real charge> <integer iatom> through <integer jatom>
where charge is the net charge of the set of atoms {[iatom:jatom]}
.
- A group of atoms can be constrained to have the same charge with
constrain equal {<integer iatom>}
- The individual charge of a group of atoms can be constrained to be equal to those of a second group of atoms with
constrain group <integer iatom> <integer jatom> to <integer katom> <integer latom>
resulting in the same charge for atoms iatom and katom, for atoms iatom+1 and k atom+1, ... for atoms jatom and latom.
- A special constraint
constrain xhn <integer iatom> {<integer jatom>}
can be used to constrain the set {iatom,{jatom}}
to zero charge, and constrain all atoms in {jatom}
to have the same charge. This can be used, for example, to restrain a methyl group to zero charge,
and have all hydrogen carrying identical charges.
Restraints can be applied to each partial charge using the RESP charge fitting procedure.
- The directive for charge restraining is
restrain [hfree] (harmonic [<real scale>] | \
hyperbolic [<real scale> [<real tight>]] \
[maxiter <integer maxit>] [tolerance <real toler>])
Here hfree
can be specified to exclude hydrogen atoms from the
restraining procedure. Variable scale
is the strength of the restraint
potential, with a default of 0.005 au for the harmonic
restraint and a
default value of 0.001 au for the hyperbolic
restraint. For the
hyperbolic restraints the tightness tight
can be specified to change the
default value of 0.1 e. The iteration count that needs to be carried out
for the hyperbolic restraint is determined by the maximum number of
allowed iterations maxiter
, with a default value of 25, and the
tolerance
in the convergence of the partial charges toler
, with a
default of 0.001 e.