small documentation fixes to fix typos and formatting issues
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@ -111,26 +111,26 @@ Coefficients parameterized by "(Fox)"_#Fox are assigned for each
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atom type designating the chemical symbol and charge of each atom
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type. Valid chemical symbols for compute saed are:
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H: He: Li: Be: B:
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C: N: O: F: Ne:
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Na: Mg: Al: Si: P:
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S: Cl: Ar: K: Ca:
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Sc: Ti: V: Cr: Mn:
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Fe: Co: Ni: Cu: Zn:
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Ga: Ge: As: Se: Br:
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Kr: Rb: Sr: Y: Zr:
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Nb: Mo: Tc: Ru: Rh:
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Pd: Ag: Cd: In: Sn:
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Sb: Te: I: Xe: Cs:
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Ba: La: Ce: Pr: Nd:
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Pm: Sm: Eu: Gd: Tb:
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Dy: Ho: Er: Tm: Yb:
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Lu: Hf: Ta: W: Re:
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Os: Ir: Pt: Au: Hg:
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Tl: Pb: Bi: Po: At:
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Rn: Fr: Ra: Ac: Th:
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Pa: U: Np: Pu: Am:
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Cm: Bk: Cf:tb(c=5,s=:)
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H: He: Li: Be: B:
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C: N: O: F: Ne:
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Na: Mg: Al: Si: P:
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S: Cl: Ar: K: Ca:
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Sc: Ti: V: Cr: Mn:
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Fe: Co: Ni: Cu: Zn:
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Ga: Ge: As: Se: Br:
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Kr: Rb: Sr: Y: Zr:
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Nb: Mo: Tc: Ru: Rh:
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Pd: Ag: Cd: In: Sn:
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Sb: Te: I: Xe: Cs:
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Ba: La: Ce: Pr: Nd:
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Pm: Sm: Eu: Gd: Tb:
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Dy: Ho: Er: Tm: Yb:
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Lu: Hf: Ta: W: Re:
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Os: Ir: Pt: Au: Hg:
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Tl: Pb: Bi: Po: At:
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Rn: Fr: Ra: Ac: Th:
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Pa: U: Np: Pu: Am:
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Cm: Bk: Cf:tb(c=5,s=:)
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If the {echo} keyword is specified, compute saed will provide extra
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@ -18,6 +18,7 @@ dihedral_coeff 1 1 286.1 1 124 1 1 90.0 0 1 90.0 0
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dihedral_coeff 1 3 69.3 1 93.9 1 1 90 0 1 90 0 &
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49.1 0 0.00 0 1 74.4 1 0 0.00 0 &
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25.2 0 0.00 0 0 0.00 0 1 48.1 1
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:pre
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[Description:]
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@ -68,7 +68,7 @@ matrix that gives canonical sampling for a given A is computed automatically.
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However, the GLE framework also allow for non-equilibrium sampling, that
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can be used for instance to model inexpensively zero-point energy
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effects "(Ceriotti2)"_#Ceriotti2. This is achieved specifying the {noneq}
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keyword followed by the name of the file that contains the static covariance
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keyword followed by the name of the file that contains the static covariance
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matrix for the non-equilibrium dynamics. Please note, that the covariance
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matrix is expected to be given in [temperature units].
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@ -67,11 +67,11 @@ The Langevin forces are computed as
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\(F_r'\) is a random force proportional to
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\(\sqrt \{ \frac \{2\, k_B \mathtt\{Tcom\}\, m'\}
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\{\mathrm dt\, \mathtt\{damp\_com\} \}
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\} \). :b
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\} \).
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\(f_r'\) is a random force proportional to
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\(\sqrt \{ \frac \{2\, k_B \mathtt\{Tdrude\}\, m'\}
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\{\mathrm dt\, \mathtt\{damp\_drude\} \}
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\} \). :b
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\} \).
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Then the real forces acting on the particles are computed from the inverse
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transform:
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\begin\{equation\} F = \frac M \{M'\}\, F' - f' \end\{equation\}
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@ -574,9 +574,9 @@ is used. If it is not used, you must invoke the package intel
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command in your input script or or via the "-pk intel" "command-line
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switch"_Section_start.html#start_7.
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For the KOKKOS package, the option defaults neigh = full, neigh/qeq
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= full, newton = off, binsize = 0.0, and comm = device. These settings
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are made automatically by the required "-k on" "command-line
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For the KOKKOS package, the option defaults neigh = full,
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neigh/qeq = full, newton = off, binsize = 0.0, and comm = device.
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These settings are made automatically by the required "-k on" "command-line
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switch"_Section_start.html#start_7. You can change them bu using the
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package kokkos command in your input script or via the "-pk kokkos"
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"command-line switch"_Section_start.html#start_7.
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@ -74,7 +74,7 @@ placeholders for atom types that will be used with other potentials.
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The python potential file has to start with the following code:
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from __future__ import print_function
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#
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class LAMMPSPairPotential(object):
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def __init__(self):
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self.pmap=dict()
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@ -163,9 +163,10 @@ pair_write 1 1 2000 rsq 0.01 2.5 lj1_lj2.table lj :pre
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Note that it is strongly recommended to try to [delete] the potential
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table file before generating it. Since the {pair_write} command will
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always append to a table file, which pair style table will use the
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first match. Thus when changing the potential function in the python
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class, the table pair style will still read the old variant.
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always [append] to a table file, while pair style table will use the
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[first match]. Thus when changing the potential function in the python
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class, the table pair style will still read the old variant unless the
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table file is first deleted.
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After switching the pair style to {table}, the potential tables need
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to be assigned to the LAMMPS atom types like this:
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@ -10,7 +10,8 @@ pair_style snap command :h3
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[Syntax:]
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pair_style snap :pre
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pair_style snap
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:pre
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[Examples:]
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@ -19,11 +20,11 @@ pair_coeff * * InP.snapcoeff In P InP.snapparam In In P P :pre
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[Description:]
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Style {snap} computes interactions
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Pair style {snap} computes interactions
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using the spectral neighbor analysis potential (SNAP)
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"(Thompson)"_#Thompson20142. Like the GAP framework of Bartok et al.
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"(Bartok2010)"_#Bartok20102, "(Bartok2013)"_#Bartok2013
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it uses bispectrum components
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which uses bispectrum components
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to characterize the local neighborhood of each atom
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in a very general way. The mathematical definition of the
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bispectrum calculation used by SNAP is identical
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@ -14,7 +14,7 @@ pair_style zero cutoff {nocoeff} :pre
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zero = style name of this pair style
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cutoff = global cutoff (distance units)
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nocoeff = ignore all pair_coeff parameters (optional) :l
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nocoeff = ignore all pair_coeff parameters (optional) :ul
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[Examples:]
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@ -10,6 +10,7 @@ PyLammps Tutorial :h1
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<!-- RST
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.. contents::
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END_RST -->
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Overview :h2
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