git-svn-id: svn://svn.icms.temple.edu/lammps-ro/trunk@2122 f3b2605a-c512-4ea7-a41b-209d697bcdaa
This commit is contained in:
BIN
doc/Eqs/pair_tersoff_zbl.jpg
Normal file
BIN
doc/Eqs/pair_tersoff_zbl.jpg
Normal file
Binary file not shown.
|
After Width: | Height: | Size: 37 KiB |
33
doc/Eqs/pair_tersoff_zbl.tex
Normal file
33
doc/Eqs/pair_tersoff_zbl.tex
Normal file
@ -0,0 +1,33 @@
|
||||
\documentclass[12pt]{article}
|
||||
|
||||
\begin{document}
|
||||
|
||||
\begin{eqnarray*}
|
||||
E & = & \frac{1}{2} \sum_i \sum_{j \neq i} V_{ij} \\
|
||||
V_{ij} & = & (1 - f_F(r_{ij})) V^{ZBL}_{ij} + f_F(r_{ij}) V^{Tersoff}_{ij} \\
|
||||
f_F(r_{ij}) & = & \frac{1}{1 + e^{-A_F(r_{ij} - r_C)}}\\
|
||||
\\
|
||||
\\
|
||||
V^{ZBL}_{ij} & = & \frac{1}{4\pi\epsilon_0} \frac{Z_1 Z_2 \,e^2}{r_{ij}} \phi(r_{ij}/a) \\
|
||||
a & = & \frac{0.8854\,a_0}{Z_{1}^{0.23} + Z_{2}^{0.23}}\\
|
||||
\phi(x) & = & 0.1818e^{-3.2x} + 0.5099e^{-0.9423x} + 0.2802e^{-0.4029x} + 0.02817e^{-0.2016x}\\
|
||||
\\
|
||||
\\
|
||||
V^{Tersoff}_{ij} & = & f_C(r_{ij}) \left[ f_R(r_{ij}) + b_{ij} f_A(r_{ij}) \right] \\
|
||||
f_C(r) & = & \left\{ \begin{array} {r@{\quad:\quad}l}
|
||||
1 & r < R - D \\
|
||||
\frac{1}{2} - \frac{1}{2} \sin \left( \frac{\pi}{2} \frac{r-R}{D} \right) &
|
||||
R-D < r < R + D \\
|
||||
0 & r > R + D
|
||||
\end{array} \right. \\
|
||||
f_R(r) & = & A \exp (-\lambda_1 r) \\
|
||||
f_A(r) & = & -B \exp (-\lambda_2 r) \\
|
||||
b_{ij} & = & \left( 1 + \beta^n {\zeta_{ij}}^n \right)^{-\frac{1}{2n}} \\
|
||||
\zeta_{ij} & = & \sum_{k \neq i,j} f_C(r_{ik}) g(\theta_{ijk})
|
||||
\exp \left[ {\lambda_3}^3 (r_{ij} - r_{ik})^m \right] \\
|
||||
g(\theta) & = & \gamma_{ijk} \left( 1 + \frac{c^2}{d^2} -
|
||||
\frac{c^2}{\left[ d^2 +
|
||||
(\cos \theta - \cos \theta_0)^2\right]} \right)
|
||||
\end{eqnarray*}
|
||||
|
||||
\end{document}
|
||||
@ -373,7 +373,7 @@ full description:
|
||||
<TR ALIGN="center"><TD ><A HREF = "pair_lj_expand.html">lj/expand</A></TD><TD ><A HREF = "pair_gromacs.html">lj/gromacs</A></TD><TD ><A HREF = "pair_gromacs.html">lj/gromacs/coul/gromacs</A></TD><TD ><A HREF = "pair_lj_smooth.html">lj/smooth</A></TD></TR>
|
||||
<TR ALIGN="center"><TD ><A HREF = "pair_lubricate.html">lubricate</A></TD><TD ><A HREF = "pair_meam.html">meam</A></TD><TD ><A HREF = "pair_morse.html">morse</A></TD><TD ><A HREF = "pair_morse.html">morse/opt</A></TD></TR>
|
||||
<TR ALIGN="center"><TD ><A HREF = "pair_resquared.html">resquared</A></TD><TD ><A HREF = "pair_peri_pmb.html">peri/pmb</A></TD><TD ><A HREF = "pair_soft.html">soft</A></TD><TD ><A HREF = "pair_sw.html">sw</A></TD></TR>
|
||||
<TR ALIGN="center"><TD ><A HREF = "pair_table.html">table</A></TD><TD ><A HREF = "pair_tersoff.html">tersoff</A></TD><TD ><A HREF = "pair_yukawa.html">yukawa</A>
|
||||
<TR ALIGN="center"><TD ><A HREF = "pair_table.html">table</A></TD><TD ><A HREF = "pair_tersoff.html">tersoff</A></TD><TD ><A HREF = "pair_tersoff_zbl.html">tersoff/zbl</A></TD><TD ><A HREF = "pair_yukawa.html">yukawa</A>
|
||||
</TD></TR></TABLE></DIV>
|
||||
|
||||
<P>These are pair styles contributed by users, which can be used if
|
||||
|
||||
@ -532,6 +532,7 @@ full description:
|
||||
"sw"_pair_sw.html,
|
||||
"table"_pair_table.html,
|
||||
"tersoff"_pair_tersoff.html,
|
||||
"tersoff/zbl"_pair_tersoff_zbl.html,
|
||||
"yukawa"_pair_yukawa.html :tb(c=4,ea=c)
|
||||
|
||||
These are pair styles contributed by users, which can be used if
|
||||
|
||||
@ -96,7 +96,7 @@ the pair_style command, and coefficients specified by the associated
|
||||
<LI><A HREF = "pair_coul.html">pair_style coul/cut</A> - cutoff Coulombic potential
|
||||
<LI><A HREF = "pair_coul.html">pair_style coul/debye</A> - cutoff Coulombic potential with Debye screening
|
||||
<LI><A HREF = "pair_coul.html">pair_style coul/long</A> - long-range Coulombic potential
|
||||
<LI><A HREF = "pair_dpd.html">pair_style dipole/cut</A> - point dipoles with cutoff
|
||||
<LI><A HREF = "pair_dipole.html">pair_style dipole/cut</A> - point dipoles with cutoff
|
||||
<LI><A HREF = "pair_dpd.html">pair_style dpd</A> - dissipative particle dynamics (DPD)
|
||||
<LI><A HREF = "pair_eam.html">pair_style eam</A> - embedded atom method (EAM)
|
||||
<LI><A HREF = "pair_eam.html">pair_style eam/opt</A> - optimized version of EAM
|
||||
@ -135,6 +135,7 @@ the pair_style command, and coefficients specified by the associated
|
||||
<LI><A HREF = "pair_sw.html">pair_style sw</A> - Stillinger-Weber 3-body potential
|
||||
<LI><A HREF = "pair_table.html">pair_style table</A> - tabulated pair potential
|
||||
<LI><A HREF = "pair_tersoff.html">pair_style tersoff</A> - Tersoff 3-body potential
|
||||
<LI><A HREF = "pair_tersoff.html">pair_style tersoff/zbl</A> - Tersoff/ZBL 3-body potential
|
||||
<LI><A HREF = "pair_yukawa.html">pair_style yukawa</A> - Yukawa potential
|
||||
</UL>
|
||||
<P>There are also additional pair styles submitted by users which are
|
||||
|
||||
@ -92,7 +92,7 @@ the pair_style command, and coefficients specified by the associated
|
||||
"pair_style coul/cut"_pair_coul.html - cutoff Coulombic potential
|
||||
"pair_style coul/debye"_pair_coul.html - cutoff Coulombic potential with Debye screening
|
||||
"pair_style coul/long"_pair_coul.html - long-range Coulombic potential
|
||||
"pair_style dipole/cut"_pair_dpd.html - point dipoles with cutoff
|
||||
"pair_style dipole/cut"_pair_dipole.html - point dipoles with cutoff
|
||||
"pair_style dpd"_pair_dpd.html - dissipative particle dynamics (DPD)
|
||||
"pair_style eam"_pair_eam.html - embedded atom method (EAM)
|
||||
"pair_style eam/opt"_pair_eam.html - optimized version of EAM
|
||||
@ -131,6 +131,7 @@ the pair_style command, and coefficients specified by the associated
|
||||
"pair_style sw"_pair_sw.html - Stillinger-Weber 3-body potential
|
||||
"pair_style table"_pair_table.html - tabulated pair potential
|
||||
"pair_style tersoff"_pair_tersoff.html - Tersoff 3-body potential
|
||||
"pair_style tersoff/zbl"_pair_tersoff.html - Tersoff/ZBL 3-body potential
|
||||
"pair_style yukawa"_pair_yukawa.html - Yukawa potential :ul
|
||||
|
||||
There are also additional pair styles submitted by users which are
|
||||
|
||||
@ -137,6 +137,7 @@ the pair_style command, and coefficients specified by the associated
|
||||
<LI><A HREF = "pair_sw.html">pair_style sw</A> - Stillinger-Weber 3-body potential
|
||||
<LI><A HREF = "pair_table.html">pair_style table</A> - tabulated pair potential
|
||||
<LI><A HREF = "pair_tersoff.html">pair_style tersoff</A> - Tersoff 3-body potential
|
||||
<LI><A HREF = "pair_tersoff.html">pair_style tersoff/zbl</A> - Tersoff/ZBL 3-body potential
|
||||
<LI><A HREF = "pair_yukawa.html">pair_style yukawa</A> - Yukawa potential
|
||||
</UL>
|
||||
<P>There are also additional pair styles submitted by users which are
|
||||
|
||||
@ -133,6 +133,7 @@ the pair_style command, and coefficients specified by the associated
|
||||
"pair_style sw"_pair_sw.html - Stillinger-Weber 3-body potential
|
||||
"pair_style table"_pair_table.html - tabulated pair potential
|
||||
"pair_style tersoff"_pair_tersoff.html - Tersoff 3-body potential
|
||||
"pair_style tersoff/zbl"_pair_tersoff.html - Tersoff/ZBL 3-body potential
|
||||
"pair_style yukawa"_pair_yukawa.html - Yukawa potential :ul
|
||||
|
||||
There are also additional pair styles submitted by users which are
|
||||
|
||||
@ -18,7 +18,7 @@
|
||||
<P><B>Examples:</B>
|
||||
</P>
|
||||
<PRE>pair_style tersoff
|
||||
pair_coeff * * si.tersoff Si
|
||||
pair_coeff * * Si.tersoff Si
|
||||
pair_coeff * * SiC.tersoff Si C Si
|
||||
</PRE>
|
||||
<P><B>Description:</B>
|
||||
@ -124,7 +124,7 @@ specified as either 3 or 1. Tersoff used a slightly different but
|
||||
equivalent form for alloys, which we will refer to as Tersoff_2
|
||||
potential <A HREF = "#Tersoff_2">(Tersoff_2)</A>.
|
||||
</P>
|
||||
<P>LAMMPS parameter values for Tersoff_2 can be obtained as follows.
|
||||
<P>LAMMPS parameter values for Tersoff_2 can be obtained as follows:
|
||||
gamma = 1, just as for Tersoff_1, but now lambda3 = 0 and the value of
|
||||
m has no effect. The parameters for species i and j can be calculated
|
||||
using the Tersoff_2 mixing rules:
|
||||
|
||||
@ -15,7 +15,7 @@ pair_style tersoff :pre
|
||||
[Examples:]
|
||||
|
||||
pair_style tersoff
|
||||
pair_coeff * * si.tersoff Si
|
||||
pair_coeff * * Si.tersoff Si
|
||||
pair_coeff * * SiC.tersoff Si C Si :pre
|
||||
|
||||
[Description:]
|
||||
@ -121,7 +121,7 @@ specified as either 3 or 1. Tersoff used a slightly different but
|
||||
equivalent form for alloys, which we will refer to as Tersoff_2
|
||||
potential "(Tersoff_2)"_#Tersoff_2.
|
||||
|
||||
LAMMPS parameter values for Tersoff_2 can be obtained as follows.
|
||||
LAMMPS parameter values for Tersoff_2 can be obtained as follows:
|
||||
gamma = 1, just as for Tersoff_1, but now lambda3 = 0 and the value of
|
||||
m has no effect. The parameters for species i and j can be calculated
|
||||
using the Tersoff_2 mixing rules:
|
||||
|
||||
243
doc/pair_tersoff_zbl.html
Normal file
243
doc/pair_tersoff_zbl.html
Normal file
@ -0,0 +1,243 @@
|
||||
<HTML>
|
||||
<CENTER><A HREF = "http://lammps.sandia.gov">LAMMPS WWW Site</A> - <A HREF = "Manual.html">LAMMPS Documentation</A> - <A HREF = "Section_commands.html#comm">LAMMPS Commands</A>
|
||||
</CENTER>
|
||||
|
||||
|
||||
|
||||
|
||||
|
||||
|
||||
<HR>
|
||||
|
||||
<H3>pair_style tersoff/zbl command
|
||||
</H3>
|
||||
<P><B>Syntax:</B>
|
||||
</P>
|
||||
<PRE>pair_style tersoff/zbl
|
||||
</PRE>
|
||||
<P><B>Examples:</B>
|
||||
</P>
|
||||
<PRE>pair_style tersoff/zbl
|
||||
pair_coeff * * SiC.tersoff.zbl Si C Si
|
||||
</PRE>
|
||||
<P><B>Description:</B>
|
||||
</P>
|
||||
<P>The <I>tersoff/zbl</I> style computes a 3-body Tersoff potential
|
||||
<A HREF = "#Tersoff_1">(Tersoff_1)</A> with a close-separation pairwise modification
|
||||
based on a Coulomb potential and the Ziegler-Biersack-Littmark
|
||||
universal screening function <A HREF = "#ZBL">(ZBL)</A>, giving the energy E of a
|
||||
system of atoms as
|
||||
</P>
|
||||
<CENTER><IMG SRC = "Eqs/pair_tersoff_zbl.jpg">
|
||||
</CENTER>
|
||||
<P>The f_F term is a fermi-like function used to smoothly connect the ZBL
|
||||
repulsive potential with the Tersoff potential. There are 2
|
||||
parameters used to adjust it: A_F and r_C. A_F controls how "sharp"
|
||||
the transition is between the two, and r_C is essentially the cutoff
|
||||
for the ZBL potential.
|
||||
</P>
|
||||
<P>For the ZBL portion, there are two terms. The first is the Coulomb
|
||||
repulsive term, with Z1, Z2 as the number of protons in each nucleus,
|
||||
e as the electron charge (1 for metal and real units) and epsilon0 as
|
||||
the permittivity of vacuum. The second part is the ZBL universal
|
||||
screening function, with a0 being the Bohr radius (typically 0.529
|
||||
Angstroms), and the remainder of the coefficients provided by the
|
||||
original paper. This screening function should be applicable to most
|
||||
systems. However, it is only accurate for small separations
|
||||
(i.e. less than 1 Angstrom).
|
||||
</P>
|
||||
<P>For the Tersoff portion, f_R is a two-body term and f_A includes
|
||||
three-body interactions. The summations in the formula are over all
|
||||
neighbors J and K of atom I within a cutoff distance = R + D.
|
||||
</P>
|
||||
<P>Only a single pair_coeff command is used with the <I>tersoff/zbl</I> style
|
||||
which specifies a Tersoff/ZBL potential file with parameters for all
|
||||
needed elements. These are mapped to LAMMPS atom types by specifying
|
||||
N additional arguments after the filename in the pair_coeff command,
|
||||
where N is the number of LAMMPS atom types:
|
||||
</P>
|
||||
<UL><LI>filename
|
||||
<LI>N element names = mapping of Tersoff/ZBL elements to atom types
|
||||
</UL>
|
||||
<P>As an example, imagine the SiC.tersoff.zbl file has Tersoff/ZBL values
|
||||
for Si and C. If your LAMMPS simulation has 4 atoms types and you
|
||||
want the 1st 3 to be Si, and the 4th to be C, you would use the
|
||||
following pair_coeff command:
|
||||
</P>
|
||||
<PRE>pair_coeff * * SiC.tersoff Si Si Si C
|
||||
</PRE>
|
||||
<P>The 1st 2 arguments must be * * so as to span all LAMMPS atom types.
|
||||
The first three Si arguments map LAMMPS atom types 1,2,3 to the Si
|
||||
element in the Tersoff/ZBL file. The final C argument maps LAMMPS
|
||||
atom type 4 to the C element in the Tersoff/ZBL file. If a mapping
|
||||
value is specified as NULL, the mapping is not performed. This can be
|
||||
used when a <I>tersoff/zbl</I> potential is used as part of the <I>hybrid</I>
|
||||
pair style. The NULL values are placeholders for atom types that will
|
||||
be used with other potentials.
|
||||
</P>
|
||||
<P>Tersoff/ZBL files in the <I>potentials</I> directory of the LAMMPS
|
||||
distribution have a ".tersoff.zbl" suffix. Lines that are not blank
|
||||
or comments (starting with #) define parameters for a triplet of
|
||||
elements. The parameters in a single entry correspond to coefficients
|
||||
in the formula above:
|
||||
</P>
|
||||
<UL><LI>element 1 (the center atom in a 3-body interaction)
|
||||
<LI>element 2 (the atom bonded to the center atom)
|
||||
<LI>element 3 (the atom influencing the 1-2 bond in a bond-order sense)
|
||||
<LI>m
|
||||
<LI>gamma
|
||||
<LI>lambda3 (1/distance units)
|
||||
<LI>c
|
||||
<LI>d
|
||||
<LI>costheta0 (can be a value < -1 or > 1)
|
||||
<LI>n
|
||||
<LI>beta
|
||||
<LI>lambda2 (1/distance units)
|
||||
<LI>B (energy units)
|
||||
<LI>R (distance units)
|
||||
<LI>D (distance units)
|
||||
<LI>lambda1 (1/distance units)
|
||||
<LI>A (energy units)
|
||||
<LI>Z_i
|
||||
<LI>Z_j
|
||||
<LI>ZBLcut (distance units)
|
||||
<LI>ZBLexpscale (1/distance units)
|
||||
</UL>
|
||||
<P>The n, beta, lambda2, B, lambda1, and A parameters are only used for
|
||||
two-body interactions. The m, gamma, lambda3, c, d, and costheta0
|
||||
parameters are only used for three-body interactions. The R and D
|
||||
parameters are used for both two-body and three-body interactions. The
|
||||
Z_i,Z_j, ZBLcut, ZBLexpscale parameters are used in the ZBL repulsive
|
||||
portion of the potential and in the Fermi-like function. The
|
||||
non-annotated parameters are unitless. The value of m must be 3 or 1.
|
||||
</P>
|
||||
<P>The Tersoff/ZBL potential file must contain entries for all the
|
||||
elements listed in the pair_coeff command. It can also contain
|
||||
entries for additional elements not being used in a particular
|
||||
simulation; LAMMPS ignores those entries.
|
||||
</P>
|
||||
<P>For a single-element simulation, only a single entry is required
|
||||
(e.g. SiSiSi). For a two-element simulation, the file must contain 8
|
||||
entries (for SiSiSi, SiSiC, SiCSi, SiCC, CSiSi, CSiC, CCSi, CCC), that
|
||||
specify Tersoff parameters for all permutations of the two elements
|
||||
interacting in three-body configurations. Thus for 3 elements, 27
|
||||
entries would be required, etc.
|
||||
</P>
|
||||
<P>As annotated above, the first element in the entry is the center atom
|
||||
in a three-body interaction and it is bonded to the 2nd atom and the
|
||||
bond is influenced by the 3rd atom. Thus an entry for SiCC means Si
|
||||
bonded to a C with another C atom influencing the bond. Thus
|
||||
three-body parameters for SiCSi and SiSiC entries will not, in
|
||||
general, be the same. The parameters used for the two-body
|
||||
interaction come from the entry where the 2nd element is repeated.
|
||||
Thus the two-body parameters for Si interacting with C, comes from the
|
||||
SiCC entry. By symmetry, the twobody parameters in the SiCC and CSiSi
|
||||
entries should thus be the same. The parameters used for a particular
|
||||
three-body interaction come from the entry with the corresponding
|
||||
three elements. The parameters used only for two-body interactions
|
||||
(n, beta, lambda2, B, lambda1, and A) in entries whose 2nd and 3rd
|
||||
element are different (e.g. SiCSi) are not used for anything and can
|
||||
be set to 0.0 if desired.
|
||||
</P>
|
||||
<P>We chose the above form so as to enable users to define all commonly
|
||||
used variants of the Tersoff portion of the potential. In particular,
|
||||
our form reduces to the original Tersoff form when m = 3 and gamma =
|
||||
1, while it reduces to the form of <A HREF = "#Albe">Albe et al.</A> when beta = 1
|
||||
and m = 1. Note that in the current Tersoff implementation in LAMMPS,
|
||||
m must be specified as either 3 or 1. Tersoff used a slightly
|
||||
different but equivalent form for alloys, which we will refer to as
|
||||
Tersoff_2 potential <A HREF = "#Tersoff_2">(Tersoff_2)</A>.
|
||||
</P>
|
||||
<P>LAMMPS parameter values for Tersoff_2 can be obtained as follows:
|
||||
gamma = 1, just as for Tersoff_1, but now lambda3 = 0 and the value of
|
||||
m has no effect. The parameters for species i and j can be calculated
|
||||
using the Tersoff_2 mixing rules:
|
||||
</P>
|
||||
<CENTER><IMG SRC = "Eqs/pair_tersoff_2.jpg">
|
||||
</CENTER>
|
||||
<P>Values not shown are determined by the first<73>atom type. Finally, the
|
||||
Tersoff_2 parameters R and S must be converted to the LAMMPS
|
||||
parameters R and D (R is different in both forms), using the following
|
||||
relations: R=(R'+S')/2 and D=(S'-R')/2, where the primes indicate the
|
||||
Tersoff_2 parameters.
|
||||
</P>
|
||||
<P>In the potentials directory, the file SiCGe.tersoff provides the
|
||||
LAMMPS parameters for Tersoff's various versions of Si, as well as his
|
||||
alloy parameters for Si, C, and Ge. This file can be used for pure Si,
|
||||
(three different versions), pure C, pure Ge, binary SiC, and binary
|
||||
SiGe. LAMMPS will generate an error if this file is used with any
|
||||
combination involving C and Ge, since there are no entries for the GeC
|
||||
interactions (Tersoff did not publish parameters for this
|
||||
cross-interaction.) Tersoff files are also provided for the SiC alloy
|
||||
(SiC.tersoff) and the GaN (GaN.tersoff) alloys.
|
||||
</P>
|
||||
<P>Many thanks to Rutuparna Narulkar, David Farrell, and Xiaowang Zhou
|
||||
for helping clarify how Tersoff parameters for alloys have been
|
||||
defined in various papers. Also thanks to Ram Devanathan for
|
||||
providing the base ZBL implementation.
|
||||
</P>
|
||||
<HR>
|
||||
|
||||
<P><B>Mixing, shift, table, tail correction, restart, rRESPA info</B>:
|
||||
</P>
|
||||
<P>For atom type pairs I,J and I != J, where types I and J correspond to
|
||||
two different element types, mixing is performed by LAMMPS as
|
||||
described above from values in the potential file.
|
||||
</P>
|
||||
<P>This pair style does not support the <A HREF = "pair_modify.html">pair_modify</A>
|
||||
shift, table, and tail options.
|
||||
</P>
|
||||
<P>This pair style does not write its information to <A HREF = "restart.html">binary restart
|
||||
files</A>, since it is stored in potential files. Thus, you
|
||||
need to re-specify the pair_style and pair_coeff commands in an input
|
||||
script that reads a restart file.
|
||||
</P>
|
||||
<P>This pair style can only be used via the <I>pair</I> keyword of the
|
||||
<A HREF = "run_style.html">run_style respa</A> command. It does not support the
|
||||
<I>inner</I>, <I>middle</I>, <I>outer</I> keywords.
|
||||
</P>
|
||||
<HR>
|
||||
|
||||
<P><B>Restrictions:</B>
|
||||
</P>
|
||||
<P>This pair style is part of the "manybody" package. It is only enabled
|
||||
if LAMMPS was built with that package (which it is by default). See
|
||||
the <A HREF = "Section_start.html#2_3">Making LAMMPS</A> section for more info.
|
||||
</P>
|
||||
<P>This pair style requires the <A HREF = "newton.html">newton</A> setting to be "on"
|
||||
for pair interactions.
|
||||
</P>
|
||||
<P>The Tersoff/ZBL potential files provided with LAMMPS (see the
|
||||
potentials directory) are parameterized for metal <A HREF = "units.html">units</A>.
|
||||
You can use the Tersoff potential with any LAMMPS units, but you would
|
||||
need to create your own Tersoff potential file with coefficients
|
||||
listed in the appropriate units if your simulation doesn't use "metal"
|
||||
units.
|
||||
</P>
|
||||
<P><B>Related commands:</B>
|
||||
</P>
|
||||
<P><A HREF = "pair_coeff.html">pair_coeff</A>
|
||||
</P>
|
||||
<P><B>Default:</B> none
|
||||
</P>
|
||||
<HR>
|
||||
|
||||
<A NAME = "Tersoff_1"></A>
|
||||
|
||||
<P><B>(Tersoff_1)</B> J. Tersoff, Phys Rev B, 37, 6991 (1988).
|
||||
</P>
|
||||
<A NAME = "ZBL"></A>
|
||||
|
||||
<P><B>(ZBL)</B> J.F. Ziegler, J.P. Biersack, U. Littmark, 'Stopping and Ranges
|
||||
of Ions in Matter' Vol 1, 1985, Pergamon Press.
|
||||
</P>
|
||||
<A NAME = "Albe"></A>
|
||||
|
||||
<P><B>(Albe)</B> J. Nord, K. Albe, P. Erhartand K. Nordlund, J. Phys.:
|
||||
Condens. Matter, 15, 5649(2003).
|
||||
</P>
|
||||
<A NAME = "Tersoff_2"></A>
|
||||
|
||||
<P><B>(Tersoff_2)</B> J. Tersoff, Phys Rev B, 39, 5566 (1989)
|
||||
</P>
|
||||
</HTML>
|
||||
234
doc/pair_tersoff_zbl.txt
Normal file
234
doc/pair_tersoff_zbl.txt
Normal file
@ -0,0 +1,234 @@
|
||||
"LAMMPS WWW Site"_lws - "LAMMPS Documentation"_ld - "LAMMPS Commands"_lc :c
|
||||
|
||||
:link(lws,http://lammps.sandia.gov)
|
||||
:link(ld,Manual.html)
|
||||
:link(lc,Section_commands.html#comm)
|
||||
|
||||
:line
|
||||
|
||||
pair_style tersoff/zbl command :h3
|
||||
|
||||
[Syntax:]
|
||||
|
||||
pair_style tersoff/zbl :pre
|
||||
|
||||
[Examples:]
|
||||
|
||||
pair_style tersoff/zbl
|
||||
pair_coeff * * SiC.tersoff.zbl Si C Si :pre
|
||||
|
||||
[Description:]
|
||||
|
||||
The {tersoff/zbl} style computes a 3-body Tersoff potential
|
||||
"(Tersoff_1)"_#Tersoff_1 with a close-separation pairwise modification
|
||||
based on a Coulomb potential and the Ziegler-Biersack-Littmark
|
||||
universal screening function "(ZBL)"_#ZBL, giving the energy E of a
|
||||
system of atoms as
|
||||
|
||||
:c,image(Eqs/pair_tersoff_zbl.jpg)
|
||||
|
||||
The f_F term is a fermi-like function used to smoothly connect the ZBL
|
||||
repulsive potential with the Tersoff potential. There are 2
|
||||
parameters used to adjust it: A_F and r_C. A_F controls how "sharp"
|
||||
the transition is between the two, and r_C is essentially the cutoff
|
||||
for the ZBL potential.
|
||||
|
||||
For the ZBL portion, there are two terms. The first is the Coulomb
|
||||
repulsive term, with Z1, Z2 as the number of protons in each nucleus,
|
||||
e as the electron charge (1 for metal and real units) and epsilon0 as
|
||||
the permittivity of vacuum. The second part is the ZBL universal
|
||||
screening function, with a0 being the Bohr radius (typically 0.529
|
||||
Angstroms), and the remainder of the coefficients provided by the
|
||||
original paper. This screening function should be applicable to most
|
||||
systems. However, it is only accurate for small separations
|
||||
(i.e. less than 1 Angstrom).
|
||||
|
||||
For the Tersoff portion, f_R is a two-body term and f_A includes
|
||||
three-body interactions. The summations in the formula are over all
|
||||
neighbors J and K of atom I within a cutoff distance = R + D.
|
||||
|
||||
Only a single pair_coeff command is used with the {tersoff/zbl} style
|
||||
which specifies a Tersoff/ZBL potential file with parameters for all
|
||||
needed elements. These are mapped to LAMMPS atom types by specifying
|
||||
N additional arguments after the filename in the pair_coeff command,
|
||||
where N is the number of LAMMPS atom types:
|
||||
|
||||
filename
|
||||
N element names = mapping of Tersoff/ZBL elements to atom types :ul
|
||||
|
||||
As an example, imagine the SiC.tersoff.zbl file has Tersoff/ZBL values
|
||||
for Si and C. If your LAMMPS simulation has 4 atoms types and you
|
||||
want the 1st 3 to be Si, and the 4th to be C, you would use the
|
||||
following pair_coeff command:
|
||||
|
||||
pair_coeff * * SiC.tersoff Si Si Si C :pre
|
||||
|
||||
The 1st 2 arguments must be * * so as to span all LAMMPS atom types.
|
||||
The first three Si arguments map LAMMPS atom types 1,2,3 to the Si
|
||||
element in the Tersoff/ZBL file. The final C argument maps LAMMPS
|
||||
atom type 4 to the C element in the Tersoff/ZBL file. If a mapping
|
||||
value is specified as NULL, the mapping is not performed. This can be
|
||||
used when a {tersoff/zbl} potential is used as part of the {hybrid}
|
||||
pair style. The NULL values are placeholders for atom types that will
|
||||
be used with other potentials.
|
||||
|
||||
Tersoff/ZBL files in the {potentials} directory of the LAMMPS
|
||||
distribution have a ".tersoff.zbl" suffix. Lines that are not blank
|
||||
or comments (starting with #) define parameters for a triplet of
|
||||
elements. The parameters in a single entry correspond to coefficients
|
||||
in the formula above:
|
||||
|
||||
element 1 (the center atom in a 3-body interaction)
|
||||
element 2 (the atom bonded to the center atom)
|
||||
element 3 (the atom influencing the 1-2 bond in a bond-order sense)
|
||||
m
|
||||
gamma
|
||||
lambda3 (1/distance units)
|
||||
c
|
||||
d
|
||||
costheta0 (can be a value < -1 or > 1)
|
||||
n
|
||||
beta
|
||||
lambda2 (1/distance units)
|
||||
B (energy units)
|
||||
R (distance units)
|
||||
D (distance units)
|
||||
lambda1 (1/distance units)
|
||||
A (energy units)
|
||||
Z_i
|
||||
Z_j
|
||||
ZBLcut (distance units)
|
||||
ZBLexpscale (1/distance units) :ul
|
||||
|
||||
The n, beta, lambda2, B, lambda1, and A parameters are only used for
|
||||
two-body interactions. The m, gamma, lambda3, c, d, and costheta0
|
||||
parameters are only used for three-body interactions. The R and D
|
||||
parameters are used for both two-body and three-body interactions. The
|
||||
Z_i,Z_j, ZBLcut, ZBLexpscale parameters are used in the ZBL repulsive
|
||||
portion of the potential and in the Fermi-like function. The
|
||||
non-annotated parameters are unitless. The value of m must be 3 or 1.
|
||||
|
||||
The Tersoff/ZBL potential file must contain entries for all the
|
||||
elements listed in the pair_coeff command. It can also contain
|
||||
entries for additional elements not being used in a particular
|
||||
simulation; LAMMPS ignores those entries.
|
||||
|
||||
For a single-element simulation, only a single entry is required
|
||||
(e.g. SiSiSi). For a two-element simulation, the file must contain 8
|
||||
entries (for SiSiSi, SiSiC, SiCSi, SiCC, CSiSi, CSiC, CCSi, CCC), that
|
||||
specify Tersoff parameters for all permutations of the two elements
|
||||
interacting in three-body configurations. Thus for 3 elements, 27
|
||||
entries would be required, etc.
|
||||
|
||||
As annotated above, the first element in the entry is the center atom
|
||||
in a three-body interaction and it is bonded to the 2nd atom and the
|
||||
bond is influenced by the 3rd atom. Thus an entry for SiCC means Si
|
||||
bonded to a C with another C atom influencing the bond. Thus
|
||||
three-body parameters for SiCSi and SiSiC entries will not, in
|
||||
general, be the same. The parameters used for the two-body
|
||||
interaction come from the entry where the 2nd element is repeated.
|
||||
Thus the two-body parameters for Si interacting with C, comes from the
|
||||
SiCC entry. By symmetry, the twobody parameters in the SiCC and CSiSi
|
||||
entries should thus be the same. The parameters used for a particular
|
||||
three-body interaction come from the entry with the corresponding
|
||||
three elements. The parameters used only for two-body interactions
|
||||
(n, beta, lambda2, B, lambda1, and A) in entries whose 2nd and 3rd
|
||||
element are different (e.g. SiCSi) are not used for anything and can
|
||||
be set to 0.0 if desired.
|
||||
|
||||
We chose the above form so as to enable users to define all commonly
|
||||
used variants of the Tersoff portion of the potential. In particular,
|
||||
our form reduces to the original Tersoff form when m = 3 and gamma =
|
||||
1, while it reduces to the form of "Albe et al."_#Albe when beta = 1
|
||||
and m = 1. Note that in the current Tersoff implementation in LAMMPS,
|
||||
m must be specified as either 3 or 1. Tersoff used a slightly
|
||||
different but equivalent form for alloys, which we will refer to as
|
||||
Tersoff_2 potential "(Tersoff_2)"_#Tersoff_2.
|
||||
|
||||
LAMMPS parameter values for Tersoff_2 can be obtained as follows:
|
||||
gamma = 1, just as for Tersoff_1, but now lambda3 = 0 and the value of
|
||||
m has no effect. The parameters for species i and j can be calculated
|
||||
using the Tersoff_2 mixing rules:
|
||||
|
||||
:c,image(Eqs/pair_tersoff_2.jpg)
|
||||
|
||||
Values not shown are determined by the first<73>atom type. Finally, the
|
||||
Tersoff_2 parameters R and S must be converted to the LAMMPS
|
||||
parameters R and D (R is different in both forms), using the following
|
||||
relations: R=(R'+S')/2 and D=(S'-R')/2, where the primes indicate the
|
||||
Tersoff_2 parameters.
|
||||
|
||||
In the potentials directory, the file SiCGe.tersoff provides the
|
||||
LAMMPS parameters for Tersoff's various versions of Si, as well as his
|
||||
alloy parameters for Si, C, and Ge. This file can be used for pure Si,
|
||||
(three different versions), pure C, pure Ge, binary SiC, and binary
|
||||
SiGe. LAMMPS will generate an error if this file is used with any
|
||||
combination involving C and Ge, since there are no entries for the GeC
|
||||
interactions (Tersoff did not publish parameters for this
|
||||
cross-interaction.) Tersoff files are also provided for the SiC alloy
|
||||
(SiC.tersoff) and the GaN (GaN.tersoff) alloys.
|
||||
|
||||
Many thanks to Rutuparna Narulkar, David Farrell, and Xiaowang Zhou
|
||||
for helping clarify how Tersoff parameters for alloys have been
|
||||
defined in various papers. Also thanks to Ram Devanathan for
|
||||
providing the base ZBL implementation.
|
||||
|
||||
:line
|
||||
|
||||
[Mixing, shift, table, tail correction, restart, rRESPA info]:
|
||||
|
||||
For atom type pairs I,J and I != J, where types I and J correspond to
|
||||
two different element types, mixing is performed by LAMMPS as
|
||||
described above from values in the potential file.
|
||||
|
||||
This pair style does not support the "pair_modify"_pair_modify.html
|
||||
shift, table, and tail options.
|
||||
|
||||
This pair style does not write its information to "binary restart
|
||||
files"_restart.html, since it is stored in potential files. Thus, you
|
||||
need to re-specify the pair_style and pair_coeff commands in an input
|
||||
script that reads a restart file.
|
||||
|
||||
This pair style can only be used via the {pair} keyword of the
|
||||
"run_style respa"_run_style.html command. It does not support the
|
||||
{inner}, {middle}, {outer} keywords.
|
||||
|
||||
:line
|
||||
|
||||
[Restrictions:]
|
||||
|
||||
This pair style is part of the "manybody" package. It is only enabled
|
||||
if LAMMPS was built with that package (which it is by default). See
|
||||
the "Making LAMMPS"_Section_start.html#2_3 section for more info.
|
||||
|
||||
This pair style requires the "newton"_newton.html setting to be "on"
|
||||
for pair interactions.
|
||||
|
||||
The Tersoff/ZBL potential files provided with LAMMPS (see the
|
||||
potentials directory) are parameterized for metal "units"_units.html.
|
||||
You can use the Tersoff potential with any LAMMPS units, but you would
|
||||
need to create your own Tersoff potential file with coefficients
|
||||
listed in the appropriate units if your simulation doesn't use "metal"
|
||||
units.
|
||||
|
||||
[Related commands:]
|
||||
|
||||
"pair_coeff"_pair_coeff.html
|
||||
|
||||
[Default:] none
|
||||
|
||||
:line
|
||||
|
||||
:link(Tersoff_1)
|
||||
[(Tersoff_1)] J. Tersoff, Phys Rev B, 37, 6991 (1988).
|
||||
|
||||
:link(ZBL)
|
||||
[(ZBL)] J.F. Ziegler, J.P. Biersack, U. Littmark, 'Stopping and Ranges
|
||||
of Ions in Matter' Vol 1, 1985, Pergamon Press.
|
||||
|
||||
:link(Albe)
|
||||
[(Albe)] J. Nord, K. Albe, P. Erhartand K. Nordlund, J. Phys.:
|
||||
Condens. Matter, 15, 5649(2003).
|
||||
|
||||
:link(Tersoff_2)
|
||||
[(Tersoff_2)] J. Tersoff, Phys Rev B, 39, 5566 (1989)
|
||||
Reference in New Issue
Block a user