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89 Commits

Author SHA1 Message Date
9806da69f3 Stan bug fixes for fix reaxc/bonds/kk 2016-11-09 15:47:50 -07:00
bfea3dce7d Merge pull request #268 from arielzn/born_dsf
pair styles born/coul/dsf and born/coul/dsf/cs added
2016-11-09 11:57:09 -07:00
eef862ee1c Merge pull request #267 from akohlmey/pager-help
use pager for help message, if connected to stdout
2016-11-09 11:53:43 -07:00
0cc2fbf1d6 Merge pull request #266 from andeplane/IP_USER_OMP
Initializing pointers in USER-OMP
2016-11-09 11:52:05 -07:00
ae00666994 Merge pull request #265 from andeplane/IP_DIFF_DPD
Initializing pointers in USER-DIFFRACTION and USER-DPD
2016-11-09 11:51:53 -07:00
51b3b5fb35 Merge pull request #264 from andeplane/IP_SNAP_SRD
Initialize pointers in SNAP and SRD
2016-11-09 11:51:44 -07:00
176f2c3aa1 Merge pull request #263 from andeplane/IP_RIGID_SHOCK
Initialize pointers in RIGID and SHOCK
2016-11-09 11:51:36 -07:00
3f71bfb185 Merge pull request #262 from andeplane/IP_PERI_QEQ_REPLICA
Initializing pointers in PERI, QEQ and REPLICA
2016-11-09 11:51:25 -07:00
cf3ab51679 Merge pull request #261 from andeplane/IP_MISC_MOLECULE
Initialized pointers in MISC and MOLECULE
2016-11-09 11:51:09 -07:00
59922f894b Merge pull request #260 from andeplane/IP_MANYBODY_MC
Initialize pointers in MANYBODY and MC
2016-11-09 11:51:01 -07:00
5e2b9d8bf3 Merge pull request #259 from andeplane/IP_KSPACE
Initialize pointers in KSPACE
2016-11-09 11:50:50 -07:00
2d132cad6b Merge pull request #258 from andeplane/IP_GRANULAR
Initialize pointers in GRANULAR
2016-11-09 11:50:41 -07:00
ef6801f8bf Merge pull request #257 from andeplane/IP_CORESHELL
Initialize pointers in CORESHELL
2016-11-09 11:50:31 -07:00
c81a723642 Merge pull request #256 from andeplane/IP_BODY
Initialized pointers in BODY
2016-11-09 11:50:23 -07:00
f9eb2a99ce Merge pull request #255 from andeplane/IP_ASPHERE
Initialize pointers in ASPHERE
2016-11-09 11:50:11 -07:00
16a02ef27d Merge pull request #254 from andeplane/IP_root
Initialized pointers in src folder
2016-11-09 11:47:21 -07:00
2c801320c2 fixed links in Section_intro.txt 2016-11-09 11:46:10 -07:00
9de1a2a08f added input using born/coul/dsf/cs to examples/coreshell 2016-11-08 18:27:44 +01:00
cdb5d47e9f add FLERR argument to force->bounds() in born/coul/dsf 2016-11-08 18:24:54 +01:00
a23b287a7a sync with SVN for creation of stable release 2016-11-08 09:05:50 -07:00
31204aab6a sync with SVN 2016-11-08 08:57:51 -07:00
25e7d074cf documentation added for born/coul/dsf and born/coul/dsf/cs styles 2016-11-08 16:51:54 +01:00
667f4dfe28 pair style born/coul/dsf added with its coreshell version 2016-11-08 11:32:38 +01:00
21694ca3a8 improve help and it through a pager, when screen == stdout 2016-11-07 17:10:12 -05:00
9b910d5511 make name of the actual executable (i.e. arg[0]) accessible 2016-11-07 17:07:40 -05:00
054ab6bff3 Initializing pointers in USER-OMP 2016-11-07 21:07:10 +01:00
616420cda8 Initializing pointers in USER-DIFFRACTION and USER-DPD 2016-11-07 20:51:36 +01:00
fb3ac9afba Initialize pointers in SNAP and SRD 2016-11-07 20:30:38 +01:00
7cd7cda2d4 Initialize pointers in RIGID and SHOCK 2016-11-07 20:22:04 +01:00
db0524278a Initializing pointers in PERI, QEQ and REPLICA 2016-11-07 19:58:27 +01:00
1ff75eaba2 Initialized pointers in MISC and MOLECULE 2016-11-07 17:15:48 +01:00
30dede867a Initialize pointers in MANYBODY and MC 2016-11-07 17:02:32 +01:00
a5c6104d64 Initialize pointers in KSPACE 2016-11-07 16:54:59 +01:00
c5869bdee2 Initialize pointers in GRANULAR 2016-11-07 16:33:50 +01:00
e7a2c6b5d1 Initialize pointers in CORESHELL 2016-11-07 16:26:16 +01:00
06959a9c59 Initialized pointers in BODY 2016-11-07 16:21:08 +01:00
cd65d44d95 Initialize pointers in ASPHERE 2016-11-07 16:15:39 +01:00
45f2e86dd6 NULLed ptrs in files 2016-11-07 16:07:37 +01:00
f8226e8ae5 NULL ptrs in dump_custom and dump_image 2016-11-07 15:56:47 +01:00
b221b15d24 NULLing ptrs in comm_brick and dump*.cpp 2016-11-07 15:50:18 +01:00
77bbf03f0f Merge pull request #252 from akohlmey/preinstalled-vs-scm
remove the misleading "(which it is by default)" from several doc files
2016-11-04 10:59:06 -06:00
7cff08ca0a Merge pull request #249 from lammps/unstable
Incorporate merge commits from "unstable" into "master"
2016-11-04 10:58:55 -06:00
f0131393e0 Merge pull request #248 from akohlmey/collected-small-fixes
collected small bugfixes and updates
2016-11-04 10:58:42 -06:00
32e0a58343 Merge pull request #247 from akohlmey/bounds-error-with-code-line
Propagate error error locations for a few more utility functions
2016-11-04 10:58:14 -06:00
60908eeab4 Merge pull request #246 from akohlmey/manybody-short-neighbor-list
Manybody short neighbor list
2016-11-04 10:57:43 -06:00
8214555b29 Merge pull request #244 from ketankhare/patch-2
Enable write_data for dihedral style fourier
2016-11-04 10:57:20 -06:00
f48b71f46b added examples/threebody, fix reaxc/speceies/kk 2016-11-04 10:56:04 -06:00
6cc4eb19af remove the misleading "(which it is by default)" from several doc files 2016-11-04 12:20:17 -04:00
7d23a0737e add thorough checking for valid arguments to -partition or -p 2016-11-04 00:42:23 -04:00
02510ec321 add temporary force accumulation to local variables for vashishta styles 2016-11-02 22:32:30 -04:00
33140e5004 accumulate forces in temporary local variables for tersoff 2016-11-02 22:16:53 -04:00
639fb6f444 use local variables for more efficient force accumulation 2016-11-02 17:20:56 -04:00
b156771721 build short neighbor list for sw on based on ij parameters only 2016-11-02 17:09:32 -04:00
5d787f7f16 avoid tiny memory leak, when the restart command is specified multiple times 2016-11-01 21:39:12 -04:00
c8f4b55588 avoid uninitialized data for using ewald/disp with lj only 2016-11-01 16:48:30 -04:00
e13e4031cf avoid memory leak in pppm/disp/omp 2016-11-01 16:48:00 -04:00
782a328080 avoid memory leaks when using kspace solvers for lennard-jones 2016-11-01 14:55:13 -04:00
e81ae21dbd do not access uninitialized data for ewald/disp and pppm/disp 2016-11-01 14:54:16 -04:00
7fdd6e2807 remove work repetitions for 'the' 2016-11-01 11:40:07 -04:00
2e0d304c7e remove word repetitions for 'a' 2016-11-01 11:36:11 -04:00
c4b86a25a7 Merge branch 'master' into manybody-short-neighbor-list 2016-10-28 11:12:21 -04:00
218e121b41 Merge branch 'master' into bounds-error-with-code-line 2016-10-28 11:11:28 -04:00
93d393aa69 permission cleanup in tools folder 2016-10-28 10:48:35 -04:00
4216be49f3 Merge branch 'master' into collected-small-fixes 2016-10-28 10:46:33 -04:00
c3a1e72183 Version 27 Oct 2016 2016-10-27 11:40:36 -04:00
f9a9e27f5a add error location propagation to atom->set_mass() and atom->check_mass() 2016-10-26 16:01:40 -04:00
35753b8f08 add error location propagation to force->bounds() and force->boundsbig() 2016-10-26 15:53:02 -04:00
f028a9a967 region cylinder is compatible with open_faces[2], so do not disallow it. 2016-10-26 15:04:18 -04:00
ef9f7c818e fix off-by-one bug in buffer re-allocator 2016-10-26 10:14:08 -04:00
8e61bed2d8 add USER-OMP variant of manybody short neighbor list 2016-10-26 09:51:52 -04:00
3267b34590 simplify short neighbor list implementation. remove unneeded class member 2016-10-26 09:29:27 -04:00
0a417b4016 add short neighbor list support to pair style tersoff 2016-10-26 07:06:38 -04:00
399c0af150 consistent short neighbor list for vashishta and vashishta/table 2016-10-25 23:46:25 -04:00
e8b3f79690 fully tested multi-element compatible short neighbor list for Stillinger-Weber 2016-10-25 23:18:14 -04:00
7f3f5e8c38 Clean whitespace 2016-10-25 14:46:44 -04:00
f350500e69 Enable write_data 2016-10-25 14:43:12 -04:00
d7c77a419d Enable write_data for dihedral_fourier 2016-10-25 14:36:18 -04:00
d2da0fabb4 Version 20 Oct 2016 2016-10-19 15:29:13 -04:00
13ce1037f2 Version 18 Oct 2016 2016-10-18 15:46:56 -04:00
fa984b2c3b Version 13 Oct 2016 2016-10-13 19:56:33 -04:00
8540a9f038 Version 11 Oct 2016 2016-10-11 17:10:24 -04:00
13b6eb1bae Version 6 Oct 2016 2016-10-06 19:12:58 -04:00
d80a9def17 Version 5 Oct 2016 2016-10-05 18:49:08 -04:00
be4734bdce Version 30 Sep 2016 2016-09-30 11:57:15 -04:00
2551619b07 Version 29 Sep 2016 2016-09-29 10:55:26 -04:00
d8bf149edc Version 28 Sep 2016 2016-09-29 10:55:18 -04:00
473b12ded4 Version 26 Sep 2016 2016-09-29 10:55:10 -04:00
27c3149590 Version 21 Sep 2016 2016-09-29 10:54:59 -04:00
3b408d71fe Version 20 Sep 2016 2016-09-29 10:53:40 -04:00
436 changed files with 3548 additions and 1242 deletions

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@ -1,7 +1,7 @@
<!-- HTML_ONLY -->
<HEAD>
<TITLE>LAMMPS Users Manual</TITLE>
<META NAME="docnumber" CONTENT="27 Oct 2016 version">
<META NAME="docnumber" CONTENT="9 Nov 2016 version">
<META NAME="author" CONTENT="http://lammps.sandia.gov - Sandia National Laboratories">
<META NAME="copyright" CONTENT="Copyright (2003) Sandia Corporation. This software and manual is distributed under the GNU General Public License.">
</HEAD>
@ -21,7 +21,7 @@
<H1></H1>
LAMMPS Documentation :c,h3
27 Oct 2016 version :c,h4
9 Nov 2016 version :c,h4
Version info: :h4

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@ -886,6 +886,8 @@ KOKKOS, o = USER-OMP, t = OPT.
"body"_pair_body.html,
"bop"_pair_bop.html,
"born (go)"_pair_born.html,
"born/coul/dsf"_pair_born.html,
"born/coul/dsf/cs"_pair_born.html,
"born/coul/long (go)"_pair_born.html,
"born/coul/long/cs"_pair_born.html,
"born/coul/msm (o)"_pair_born.html,

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@ -2729,7 +2729,7 @@ production runs and is only required during equilibration. This way one
is consistent with literature (based on the code packages DL_POLY or
GULP for instance).
The mentioned energy transfer will typically lead to a a small drift
The mentioned energy transfer will typically lead to a small drift
in total energy over time. This internal energy can be monitored
using the "compute chunk/atom"_compute_chunk_atom.html and "compute
temp/chunk"_compute_temp_chunk.html commands. The internal kinetic
@ -2830,7 +2830,7 @@ temp/drude"_compute_temp_drude.html. This requires also to use the
command {comm_modify vel yes}.
Short-range damping of the induced dipole interactions can be achieved
using Thole functions through the the "pair style
using Thole functions through the "pair style
thole"_pair_thole.html in "pair_style hybrid/overlay"_pair_hybrid.html
with a Coulomb pair style. It may be useful to use {coul/long/cs} or
similar from the CORESHELL package if the core and Drude particle come

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@ -366,11 +366,11 @@ complementary modeling tasks.
"DL_POLY"_dlpoly
"Tinker"_tinker :ul
:link(charmm,http://www.scripps.edu/brooks)
:link(amber,http://amber.scripps.edu)
:link(charmm,http://www.charmm.org)
:link(amber,http://ambermd.org)
:link(namd,http://www.ks.uiuc.edu/Research/namd/)
:link(nwchem,http://www.emsl.pnl.gov/docs/nwchem/nwchem.html)
:link(dlpoly,http://www.cse.clrc.ac.uk/msi/software/DL_POLY)
:link(dlpoly,http://www.ccp5.ac.uk/DL_POLY_CLASSIC)
:link(tinker,http://dasher.wustl.edu/tinker)
CHARMM, AMBER, NAMD, NWCHEM, and Tinker are designed primarily for

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@ -706,7 +706,7 @@ future changes to LAMMPS.
User packages, such as user-atc or user-omp, have been contributed by
users, and always begin with the user prefix. If they are a single
command (single file), they are typically in the user-misc package.
Otherwise, they are a a set of files grouped together which add a
Otherwise, they are a set of files grouped together which add a
specific functionality to the code.
User packages don't necessarily meet the requirements of the standard

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@ -74,7 +74,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This angle style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -61,7 +61,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This angle style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -66,7 +66,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This angle style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -74,7 +74,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This angle style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -66,7 +66,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This angle style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -65,11 +65,11 @@ more instructions on how to use the accelerated styles effectively.
:line
[Restrictions:] none
[Restrictions:]
This angle style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
MOLECULE package. See the "Making LAMMPS"_Section_start.html#start_3
section for more info on packages.
[Related commands:]

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@ -76,7 +76,7 @@ for specific angle types.
[Restrictions:]
This angle style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
Unlike other angle styles, the hybrid angle style does not store angle

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@ -147,7 +147,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This angle style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -70,7 +70,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This bond style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
You typically should specify "special_bonds fene"_special_bonds.html

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@ -73,7 +73,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This bond style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
You typically should specify "special_bonds fene"_special_bonds.html

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@ -65,7 +65,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This bond style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -59,7 +59,7 @@ bond types.
[Restrictions:]
This bond style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
Unlike other bond styles, the hybrid bond style does not store bond

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@ -64,7 +64,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This bond style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -64,7 +64,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This bond style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -99,7 +99,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This bond style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
The {quartic} style requires that "special_bonds"_special_bonds.html

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@ -144,7 +144,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This bond style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -114,7 +114,7 @@ local defects surrounding the central atom, as described above. For
the {axes yes} case, the vector components are also unitless, since
they represent spatial directions.
Here are typical centro-symmetry values, from a a nanoindentation
Here are typical centro-symmetry values, from a nanoindentation
simulation into gold (FCC). These were provided by Jon Zimmerman
(Sandia):

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@ -536,7 +536,7 @@ For the {bin/cylinder} style the details are as follows. If {discard}
is set to {yes}, an out-of-domain atom will have its chunk ID set to
0. If {discard} is set to {no}, the atom will have its chunk ID set
to the first or last bin in both the radial and axis dimensions. If
{discard} is set to {mixed}, which is the default, the the radial
{discard} is set to {mixed}, which is the default, the radial
dimension is treated the same as for {discard} = no. But for the axis
dimensinon, it will only have its chunk ID set to the first or last
bin if bins extend to the simulation box boundary in the axis

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@ -60,7 +60,7 @@ produced by a small set of atoms (e.g. 4 atoms in a dihedral or 3
atoms in a Tersoff 3-body interaction) is assigned in equal portions
to each atom in the set. E.g. 1/4 of the dihedral virial to each of
the 4 atoms, or 1/3 of the fix virial due to SHAKE constraints applied
to atoms in a a water molecule via the "fix shake"_fix_shake.html
to atoms in a water molecule via the "fix shake"_fix_shake.html
command.
If no extra keywords are listed, all of the terms in this formula are

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@ -69,8 +69,8 @@ velocity for each atom. Note that if there is only one atom in the
bin, its thermal velocity will thus be 0.0.
After the spatially-averaged velocity field has been subtracted from
each atom, the temperature is calculated by the formula KE = (dim/2 N
- dim*Nx*Ny*Nz) k T, where KE = total kinetic energy of the group of
each atom, the temperature is calculated by the formula KE = (dim*N
- dim*Nx*Ny*Nz) k T/2, where KE = total kinetic energy of the group of
atoms (sum of 1/2 m v^2), dim = 2 or 3 = dimensionality of the
simulation, N = number of atoms in the group, k = Boltzmann constant,
and T = temperature. The dim*Nx*Ny*Nz term are degrees of freedom

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@ -109,7 +109,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This dihedral style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -76,7 +76,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This dihedral style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -69,7 +69,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This dihedral style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -77,7 +77,7 @@ for specific dihedral types.
[Restrictions:]
This dihedral style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
Unlike other dihedral styles, the hybrid dihedral style does not store

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@ -63,7 +63,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This dihedral style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -71,7 +71,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This dihedral style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -154,7 +154,7 @@ radians instead of degrees. (Note: This changes the way the forces
are scaled in the 4th column of the data file.)
The optional "CHECKU" keyword is followed by a filename. This allows
the user to save all of the the {Ntable} different entries in the
the user to save all of the {Ntable} different entries in the
interpolated energy table to a file to make sure that the interpolated
function agrees with the user's expectations. (Note: You can
temporarily increase the {Ntable} parameter to a high value for this

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@ -165,7 +165,7 @@ extra buffering.
:line
The {element} keyword applies only to the the dump {cfg}, {xyz}, and
The {element} keyword applies only to the dump {cfg}, {xyz}, and
{image} styles. It associates element names (e.g. H, C, Fe) with
LAMMPS atom types. See the list of element names at the bottom of
this page.
@ -574,7 +574,7 @@ e.g. its x-component of velocity if the atom-attribute "vx" was
specified.
The basic idea of a color map is that the atom-attribute will be
within a range of values, and that range is associated with a a series
within a range of values, and that range is associated with a series
of colors (e.g. red, blue, green). An atom's specific value (vx =
-3.2) can then mapped to the series of colors (e.g. halfway between
red and blue), and a specific color is determined via an interpolation

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@ -113,7 +113,7 @@ quantity being minimized), you MUST enable the
[Restrictions:]
This fix can only be used if LAMMPS was built with the MOLECULE
package (which it is by default). See the "Making
package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -150,7 +150,7 @@ initial box length is 100 Angstroms, and V is 10 Angstroms/psec, then
after 10 psec, the box length will have doubled. After 20 psec, it
will have tripled.
The {erate} style changes a dimension of the the box at a "constant
The {erate} style changes a dimension of the box at a "constant
engineering strain rate". The units of the specified strain rate are
1/time. See the "units"_units.html command for the time units
associated with different choices of simulation units,

View File

@ -237,7 +237,7 @@ described in the papers cited below, the purpose of this method is to
enable longer timesteps to be used (up to the numerical stability
limit of the integrator), while still producing the correct Boltzmann
distribution of atom positions. It is implemented within LAMMPS, by
changing how the the random force is applied so that it is composed of
changing how the random force is applied so that it is composed of
the average of two random forces representing half-contributions from
the previous and current time intervals.

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@ -233,7 +233,7 @@ present, the speed of sound squared is set equal to (1/3)*(dx/dt)^2.
Setting a0 > (dx/dt)^2 is not allowed, as this may lead to
instabilities.
If the {noise} keyword is used, followed by a a positive temperature
If the {noise} keyword is used, followed by a positive temperature
value, and a positive integer random number seed, a thermal
lattice-Boltzmann algorithm is used. If {LBtype} is set equal to 1
(i.e. the standard LB integrator is chosen), the thermal LB algorithm

View File

@ -8,6 +8,7 @@
fix reax/bonds command :h3
fix reax/c/bonds command :h3
fix reax/c/bonds/kk command :h3
[Syntax:]
@ -47,6 +48,31 @@ commands"_Section_howto.html#howto_15. No parameter of this fix can
be used with the {start/stop} keywords of the "run"_run.html command.
This fix is not invoked during "energy minimization"_minimize.html.
:line
Styles with a {gpu}, {intel}, {kk}, {omp}, or {opt} suffix are
functionally the same as the corresponding style without the suffix.
They have been optimized to run faster, depending on your available
hardware, as discussed in "Section_accelerate"_Section_accelerate.html
of the manual. The accelerated styles take the same arguments and
should produce the same results, except for round-off and precision
issues.
These accelerated styles are part of the GPU, USER-INTEL, KOKKOS,
USER-OMP and OPT packages, respectively. They are only enabled if
LAMMPS was built with those packages. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info.
You can specify the accelerated styles explicitly in your input script
by including their suffix, or you can use the "-suffix command-line
switch"_Section_start.html#start_7 when you invoke LAMMPS, or you can
use the "suffix"_suffix.html command in your input script.
See "Section_accelerate"_Section_accelerate.html of the manual for
more instructions on how to use the accelerated styles effectively.
:line
[Restrictions:]
The fix reax/bonds command requires that the "pair_style

View File

@ -7,6 +7,7 @@
:line
fix reax/c/species command :h3
fix reax/c/species/kk command :h3
[Syntax:]
@ -129,6 +130,31 @@ No parameter of this fix can be used with the {start/stop} keywords of
the "run"_run.html command. This fix is not invoked during "energy
minimization"_minimize.html.
:line
Styles with a {gpu}, {intel}, {kk}, {omp}, or {opt} suffix are
functionally the same as the corresponding style without the suffix.
They have been optimized to run faster, depending on your available
hardware, as discussed in "Section_accelerate"_Section_accelerate.html
of the manual. The accelerated styles take the same arguments and
should produce the same results, except for round-off and precision
issues.
These accelerated styles are part of the GPU, USER-INTEL, KOKKOS,
USER-OMP and OPT packages, respectively. They are only enabled if
LAMMPS was built with those packages. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info.
You can specify the accelerated styles explicitly in your input script
by including their suffix, or you can use the "-suffix command-line
switch"_Section_start.html#start_7 when you invoke LAMMPS, or you can
use the "suffix"_suffix.html command in your input script.
See "Section_accelerate"_Section_accelerate.html of the manual for
more instructions on how to use the accelerated styles effectively.
:line
[Restrictions:]
The fix species currently only works with

View File

@ -87,7 +87,7 @@ end of each run. A positive value N means that the diagnostics are reported once
per N time-steps.
The diagnostics report the average # of integrator steps and RHS function evaluations
and run-time per ODE as well as the the average/RMS/min/max per process. If the
and run-time per ODE as well as the average/RMS/min/max per process. If the
reporting frequency is 1, the RMS/min/max per ODE are also reported. The per ODE
statistics can be used to adjust the tolerance and min/max step parameters. The
statistics per MPI process can be useful to examine any load imbalance caused by the

View File

@ -28,7 +28,7 @@ fix 1 all smd/adjust_dt 0.1 :pre
The fix calculates a new stable time increment for use with the SMD time integrators.
The stable time increment is based on multiple conditions. For the SPH pair styles, a
CFL criterion (Courant, Friedrichs & Lewy, 1928) is evaluated, which determines the the speed of
CFL criterion (Courant, Friedrichs & Lewy, 1928) is evaluated, which determines the speed of
sound cannot propagate further than a typical spacing between particles within a single time step to ensure
no information is lost. For the contact pair styles, a linear analysis of the pair potential determines a
stable maximum time step.

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@ -101,7 +101,7 @@ particles move in the normal way via a time integration "fix"_fix.html
with a short timestep dt. SRD particles advect with a large timestep
dt_SRD >= dt.
If the {lamda} keyword is not specified, the the SRD temperature
If the {lamda} keyword is not specified, the SRD temperature
{Tsrd} is used in the above formula to compute lamda. If the {lamda}
keyword is specified, then the {Tsrd} setting is ignored and the above
equation is used to compute the SRD temperature.

View File

@ -107,7 +107,7 @@ specified as parameters to the fix. The other quantities are derived.
The form of the heat diffusion equation used here is almost the same
as that in equation 6 of "(Duffy)"_#Duffy, with the exception that the
electronic density is explicitly reprensented, rather than being part
of the the specific heat parameter.
of the specific heat parameter.
Currently, fix ttm assumes that none of the user-supplied parameters
will vary with temperature. Note that "(Duffy)"_#Duffy used a tanh()

View File

@ -77,7 +77,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This improper style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -81,7 +81,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This improper style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

View File

@ -55,7 +55,7 @@ types.
[Restrictions:]
This improper style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
Unlike other improper styles, the hybrid improper style does not store

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@ -27,7 +27,7 @@ between quadruplets of atoms, which remain in force for the duration
of the simulation. The list of improper quadruplets is read in by a
"read_data"_read_data.html or "read_restart"_read_restart.html command
from a data or restart file. Note that the ordering of the 4 atoms in
an improper quadruplet determines the the definition of the improper
an improper quadruplet determines the definition of the improper
angle used in the formula for each style. See the doc pages of
individual styles for details.

View File

@ -74,7 +74,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This improper style can only be used if LAMMPS was built with the
MOLECULE package (which it is by default). See the "Making
MOLECULE package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

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@ -284,7 +284,7 @@ ID2 x2 y2 z2
...
IDN xN yN zN :pre
The fields are the the atom ID, followed by the x,y,z coordinates.
The fields are the atom ID, followed by the x,y,z coordinates.
The lines can be listed in any order. Additional trailing information
on the line is OK, such as a comment.

View File

@ -44,7 +44,7 @@ one value from their respective list of values. A {file}-style
variable reads the next line from its associated file. An
{atomfile}-style variable reads the next set of lines (one per atom)
from its associated file. {String-} or {atom}- or {equal}- or
{world}-style variables cannot be used with the the next command,
{world}-style variables cannot be used with the next command,
since they only store a single value.
When any of the variables in the next command has no more values, a

View File

@ -168,7 +168,7 @@ This pair style can only be used via the {pair} keyword of the
[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).
if LAMMPS was built with that package.
[Related commands:]

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@ -203,9 +203,8 @@ These pair styles can only be used via the {pair} keyword of the
[Restrictions:]
These pair styles are part of the MANYBODY package. They are only
enabled if LAMMPS was built with that package (which it is by
default). See the "Making LAMMPS"_Section_start.html#start_3 section
for more info.
enabled if LAMMPS was built with that package. See the
"Making LAMMPS"_Section_start.html#start_3 section for more info.
These pair potentials require the "newton"_newton.html setting to be
"on" for pair interactions.

View File

@ -382,7 +382,7 @@ This pair style can only be used via the {pair} keyword of the
[Restrictions:]
These pair styles are part of the MANYBODY package. They are only
enabled if LAMMPS was built with that package (which it is by default).
enabled if LAMMPS was built with that package.
See the "Making LAMMPS"_Section_start.html#start_3 section for more
info.

View File

@ -19,6 +19,8 @@ pair_style born/coul/msm/omp command :h3
pair_style born/coul/wolf command :h3
pair_style born/coul/wolf/gpu command :h3
pair_style born/coul/wolf/omp command :h3
pair_style born/coul/dsf command :h3
pair_style born/coul/dsf/cs command :h3
[Syntax:]
@ -37,7 +39,11 @@ args = list of arguments for a particular style :ul
{born/coul/wolf} args = alpha cutoff (cutoff2)
alpha = damping parameter (inverse distance units)
cutoff = global cutoff for non-Coulombic (and Coulombic if only 1 arg) (distance units)
cutoff2 = global cutoff for Coulombic (optional) (distance units) :pre
cutoff2 = global cutoff for Coulombic (optional) (distance units)
{born/coul/dsf} or {born/coul/dsf/cs} args = alpha cutoff (cutoff2)
alpha = damping parameter (inverse distance units)
cutoff = global cutoff for non-Coulombic (and Coulombic if only 1 arg) (distance units)
cutoff2 = global cutoff for Coulombic (distance units) :pre
[Examples:]
@ -62,6 +68,10 @@ pair_style born/coul/wolf 0.25 10.0 9.0
pair_coeff * * 6.08 0.317 2.340 24.18 11.51
pair_coeff 1 1 6.08 0.317 2.340 24.18 11.51 :pre
pair_style born/coul/dsf 0.1 10.0 12.0
pair_coeff * * 0.0 1.00 0.00 0.00 0.00
pair_coeff 1 1 480.0 0.25 0.00 1.05 0.50 :pre
[Description:]
The {born} style computes the Born-Mayer-Huggins or Tosi/Fumi
@ -90,10 +100,14 @@ term.
The {born/coul/wolf} style adds a Coulombic term as described for the
Wolf potential in the "coul/wolf"_pair_coul.html pair style.
The {born/coul/dsf} style computes the Coulomb contribution with the
damped shifted force model as in the "coul/dsf"_pair_coul.html style.
Style {born/coul/long/cs} is identical to {born/coul/long} except that
a term is added for the "core/shell model"_Section_howto.html#howto_25
to allow charges on core and shell particles to be separated by r =
0.0.
0.0. The same correction is introduced for {born/coul/dsf/cs} style
which is identical to {born/coul/dsf}.
Note that these potentials are related to the "Buckingham
potential"_pair_buck.html.
@ -116,9 +130,10 @@ The second coefficient, rho, must be greater than zero.
The last coefficient is optional. If not specified, the global A,C,D
cutoff specified in the pair_style command is used.
For {born/coul/long} and {born/coul/wolf} no Coulombic cutoff can be
specified for an individual I,J type pair. All type pairs use the
same global Coulombic cutoff specified in the pair_style command.
For {born/coul/long}, {born/coul/wolf} and {born/coul/dsf} no
Coulombic cutoff can be specified for an individual I,J type pair.
All type pairs use the same global Coulombic cutoff specified in the
pair_style command.
:line
@ -174,9 +189,8 @@ respa"_run_style.html command. They do not support the {inner},
[Restrictions:]
The {born/coul/long} style is part of the KSPACE package. It is only
enabled if LAMMPS was built with that package (which it is by
default). See the "Making LAMMPS"_Section_start.html#start_3 section
for more info.
enabled if LAMMPS was built with that package. See the
"Making LAMMPS"_Section_start.html#start_3 section for more info.
[Related commands:]

View File

@ -186,9 +186,8 @@ respa"_run_style.html command. They do not support the {inner},
The {buck/coul/long} style is part of the KSPACE package. The
{buck/coul/long/cs} style is part of the CORESHELL package. They are
only enabled if LAMMPS was built with that package (which it is by
default). See the "Making LAMMPS"_Section_start.html#start_3 section
for more info.
only enabled if LAMMPS was built with that package. See the
"Making LAMMPS"_Section_start.html#start_3 section for more info.
[Related commands:]

View File

@ -156,7 +156,7 @@ These pair styles can only be used via the {pair} keyword of the
[Restrictions:]
These pair styles are part of the MANYBODY package. It is only enabled
if LAMMPS was built with that package (which it is by default). See
if LAMMPS was built with that package. See
the "Making LAMMPS"_Section_start.html#start_3 section for more info.
These pair styles requires the "newton"_newton.html setting to be "on"

View File

@ -313,9 +313,8 @@ This pair style can only be used via the {pair} keyword of the
The {coul/long}, {coul/msm} and {tip4p/long} styles are part of the
KSPACE package. The {coul/long/cs} style is part of the CORESHELL
package. They are only enabled if LAMMPS was built with that package
(which it is by default). See the "Making
LAMMPS"_Section_start.html#start_3 section for more info.
package. They are only enabled if LAMMPS was built with that package.
See the "Making LAMMPS"_Section_start.html#start_3 section for more info.
[Related commands:]

View File

@ -8,19 +8,24 @@
pair_style born/coul/long/cs command :h3
pair_style buck/coul/long/cs command :h3
pair_style born/coul/dsf/cs command :h3
[Syntax:]
pair_style style args :pre
style = {born/coul/long/cs} or {buck/coul/long/cs}
style = {born/coul/long/cs} or {buck/coul/long/cs} or {born/coul/dsf/cs}
args = list of arguments for a particular style :ul
{born/coul/long/cs} args = cutoff (cutoff2)
cutoff = global cutoff for non-Coulombic (and Coulombic if only 1 arg) (distance units)
cutoff2 = global cutoff for Coulombic (optional) (distance units)
{buck/coul/long/cs} args = cutoff (cutoff2)
cutoff = global cutoff for Buckingham (and Coulombic if only 1 arg) (distance units)
cutoff2 = global cutoff for Coulombic (optional) (distance units) :pre
cutoff2 = global cutoff for Coulombic (optional) (distance units)
{born/coul/dsf/cs} args = alpha cutoff (cutoff2)
alpha = damping parameter (inverse distance units)
cutoff = global cutoff for non-Coulombic (and Coulombic if only 1 arg) (distance units)
cutoff2 = global cutoff for Coulombic (distance units) :pre
[Examples:]
@ -32,6 +37,10 @@ pair_style buck/coul/long/cs 10.0 8.0
pair_coeff * * 100.0 1.5 200.0
pair_coeff 1 1 100.0 1.5 200.0 9.0 :pre
pair_style born/coul/dsf/cs 0.1 10.0 12.0
pair_coeff * * 0.0 1.00 0.00 0.00 0.00
pair_coeff 1 1 480.0 0.25 0.00 1.05 0.50 :pre
[Description:]
These pair styles are designed to be used with the adiabatic
@ -39,7 +48,7 @@ core/shell model of "(Mitchell and Finchham)"_#MitchellFinchham. See
"Section 6.25"_Section_howto.html#howto_25 of the manual for an
overview of the model as implemented in LAMMPS.
These pair styles are identical to the "pair_style
The styles with a {coul/long} term are identical to the "pair_style
born/coul/long"_pair_born.html and "pair_style
buck/coul/long"_pair_buck.html styles, except they correctly treat the
special case where the distance between two charged core and shell
@ -63,6 +72,14 @@ where C is an energy-conversion constant, Qi and Qj are the charges on
the core and shell, epsilon is the dielectric constant and r_min is the
minimal distance.
The pair style {born/coul/dsf/cs} is identical to the
"pair_style born/coul/dsf"_pair_born.html style, which uses the
the damped shifted force model as in "coul/dsf"_pair_coul.html
to compute the Coulomb contribution. This approach does not require
a long-range solver, thus the only correction is the addition of a
minimal distance to avoid the possible r = 0.0 case for a
core/shell pair.
[Restrictions:]
These pair styles are part of the CORESHELL package. They are only

View File

@ -412,9 +412,8 @@ The eam pair styles can only be used via the {pair} keyword of the
[Restrictions:]
All of these styles except the {eam/cd} style are part of the MANYBODY
package. They are only enabled if LAMMPS was built with that package
(which it is by default). See the "Making
LAMMPS"_Section_start.html#start_3 section for more info.
package. They are only enabled if LAMMPS was built with that package.
See the "Making LAMMPS"_Section_start.html#start_3 section for more info.
The {eam/cd} style is part of the USER-MISC package and also requires
the MANYBODY package. It is only enabled if LAMMPS was built with

View File

@ -159,7 +159,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This style is part of the MANYBODY package. It is only enabled if
LAMMPS was built with that package (which it is by default).
LAMMPS was built with that package.
[Related commands:]

View File

@ -72,7 +72,7 @@ This pair style can only be used via the {pair} keyword of the
[Restrictions:]
This pair styles is part of the MANYBODY package. It is only enabled
if LAMMPS was built with that package (which it is by default). See
if LAMMPS was built with that package. See
the "Making LAMMPS"_Section_start.html#start_3 section for more info.
This pair potential requires the "newton"_newton.html setting to be

View File

@ -113,7 +113,7 @@ more instructions on how to use the accelerated styles effectively.
[Restrictions:]
This pair style can only be used if LAMMPS was built with the MANYBODY
package (which it is by default). See the "Making
package. See the "Making
LAMMPS"_Section_start.html#start_3 section for more info on packages.
[Related commands:]

View File

@ -191,7 +191,7 @@ input script. If using read_data, atomic masses must be defined in the
atomic structure data file.
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
LAMMPS was built with that package. See the
"Making LAMMPS"_Section_start.html#start_3 section for more info.
This pair potential requires the "newtion"_newton.html setting to be

View File

@ -15,7 +15,7 @@ pair_style snap :pre
[Examples:]
pair_style snap
pair_coeff * * snap InP.snapcoeff In P InP.snapparam In In P P :pre
pair_coeff * * InP.snapcoeff In P InP.snapparam In In P P :pre
[Description:]
@ -27,9 +27,9 @@ it uses bispectrum components
to characterize the local neighborhood of each atom
in a very general way. The mathematical definition of the
bispectrum calculation used by SNAP is identical
to that used of "compute sna/atom"_compute_sna_atom.html.
to that used by "compute sna/atom"_compute_sna_atom.html.
In SNAP, the total energy is decomposed into a sum over
atom energies. The energy of atom {i} is
atom energies. The energy of atom {i } is
expressed as a weighted sum over bispectrum components.
:c,image(Eqs/pair_snap.jpg)
@ -183,8 +183,7 @@ LAMMPS"_Section_start.html#start_3 section for more info.
:line
:link(Thompson2014)
[(Thompson)] Thompson, Swiler, Trott, Foiles, Tucker, under review, preprint
available at "arXiv:1409.3880"_http://arxiv.org/abs/1409.3880
[(Thompson)] Thompson, Swiler, Trott, Foiles, Tucker, J Comp Phys, 285, 316 (2015).
:link(Bartok2010)
[(Bartok2010)] Bartok, Payne, Risi, Csanyi, Phys Rev Lett, 104, 136403 (2010).

View File

@ -99,7 +99,7 @@ The optional {exclude} keyword determines if forces are computed
between first neighbor (directly connected) bonds. For a setting of
{no}, first neighbor forces are computed; for {yes} they are not
computed. A setting of {no} cannot be used with the {min} option for
distance calculation because the the minimum distance between directly
distance calculation because the minimum distance between directly
connected bonds is zero.
Pair style {srp} turns off normalization of thermodynamic properties

View File

@ -192,7 +192,7 @@ This pair style can only be used via the {pair} keyword of the
[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
if LAMMPS was built with that package. See
the "Making LAMMPS"_Section_start.html#start_3 section for more info.
This pair style requires the "newton"_newton.html setting to be "on"

View File

@ -222,7 +222,7 @@ This pair style can only be used via the {pair} keyword of the
[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
if LAMMPS was built with that package. See
the "Making LAMMPS"_Section_start.html#start_3 section for more info.
This pair style requires the "newton"_newton.html setting to be "on"

View File

@ -156,7 +156,7 @@ This pair style can only be used via the {pair} keyword of the
[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
if LAMMPS was built with that package. See
the "Making LAMMPS"_Section_start.html#start_3 section for more info.
This pair style requires the "newton"_newton.html setting to be "on"

View File

@ -232,7 +232,7 @@ This pair style can only be used via the {pair} keyword of the
[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
if LAMMPS was built with that package. See
the "Making LAMMPS"_Section_start.html#start_3 section for more info.
This pair style requires the "newton"_newton.html setting to be "on"

View File

@ -212,9 +212,8 @@ This pair style can only be used via the {pair} keyword of the
[Restrictions:]
These pair style are part of the MANYBODY package. They is only
enabled if LAMMPS was built with that package (which it is by
default). See the "Making LAMMPS"_Section_start.html#start_3 section
for more info.
enabled if LAMMPS was built with that package. See the
"Making LAMMPS"_Section_start.html#start_3 section for more info.
These pair styles requires the "newton"_newton.html setting to be "on"
for pair interactions.

View File

@ -214,7 +214,7 @@ when a correlated event occurs during the third stage of the loop
listed above, i.e. when only one replica is running dynamics.
When more than one replica detects an event at the end of the same
event check (every {t_event} steps) during the the second stage, then
event check (every {t_event} steps) during the second stage, then
one of them is chosen at random. The number of coincident events is
the number of replicas that detected an event. Normally, this value
should be 1. If it is often greater than 1, then either the number of
@ -241,7 +241,7 @@ time was spent in each stage (dephasing, dynamics, quenching, etc).
Any "dump files"_dump.html defined in the input script, will be
written to during a PRD run at timesteps corresponding to both
uncorrelated and correlated events. This means the the requested dump
uncorrelated and correlated events. This means the requested dump
frequency in the "dump"_dump.html command is ignored. There will be
one dump file (per dump command) created for all partitions.

View File

@ -188,7 +188,7 @@ is assumed to have been previously loaded by another python command.
Note that the Python code that is loaded and run must contain a
function with the specified {func} name. To operate properly when
later invoked, the the function code must match the {input} and
later invoked, the function code must match the {input} and
{return} and {format} keywords specified by the python command.
Otherwise Python will generate an error.

View File

@ -185,7 +185,7 @@ For dump files in {xyz} format, only the {x}, {y}, and {z} fields are
supported. The dump file does not store atom IDs, so these are
assigned consecutively to the atoms as they appear in the dump file,
starting from 1. Thus you should insure that order of atoms is
consistent from snapshot to snapshot in the the XYZ dump file. See
consistent from snapshot to snapshot in the XYZ dump file. See
the "dump_modify sort"_dump_modify.html command if the XYZ dump file
was written by LAMMPS.
@ -195,7 +195,7 @@ velocities, or their respective plugins may not support reading of
velocities. The molfile dump files do not store atom IDs, so these
are assigned consecutively to the atoms as they appear in the dump
file, starting from 1. Thus you should insure that order of atoms are
consistent from snapshot to snapshot in the the molfile dump file.
consistent from snapshot to snapshot in the molfile dump file.
See the "dump_modify sort"_dump_modify.html command if the dump file
was written by LAMMPS.

View File

@ -94,6 +94,13 @@ Of course this is also possible by not using any suffix commands, and
explictly appending or not appending the suffix to the relevant
commands in your input script.
NOTE: The default "run_style"_run_style.html verlet is invoked prior to
reading the input script and is therefore not affected by a suffix command
in the input script. The KOKKOS package requires "run_style verlet/kk",
so when using the KOKKOS package it is necessary to either use the command
line "-sf kk" command or add an explicit "run_style verlet" command to the
input script.
[Restrictions:] none
[Related commands:]

View File

@ -231,7 +231,7 @@ time was spent in each stage (NEB, dynamics, quenching, etc).
Any "dump files"_dump.html defined in the input script will be written
to during a TAD run at timesteps when an event is executed. This
means the the requested dump frequency in the "dump"_dump.html command
means the requested dump frequency in the "dump"_dump.html command
is ignored. There will be one dump file (per dump command) created
for all partitions. The atom coordinates of the dump snapshot are
those of the minimum energy configuration resulting from quenching

View File

@ -33,7 +33,7 @@ created by the surrounding particles. Drude oscillators represent
these dipoles by two fixed charges: the core (DC) and the Drude
particle (DP) bound by a harmonic potential. The Drude particle can be
thought of as the electron cloud whose center can be displaced from
the position of the the corresponding nucleus.
the position of the corresponding nucleus.
The sum of the masses of a core-Drude pair should be the mass of the
initial (unsplit) atom, \(m_C + m_D = m\). The sum of their charges

View File

@ -0,0 +1,71 @@
# Testsystem for core-shell model compared to Mitchel and Finchham
# Hendrik Heenen, June 2014
# ------------------------ INITIALIZATION ----------------------------
units metal
dimension 3
boundary p p p
atom_style full
# ----------------------- ATOM DEFINITION ----------------------------
fix csinfo all property/atom i_CSID
read_data data.coreshell fix csinfo NULL CS-Info
group cores type 1 2
group shells type 3 4
neighbor 2.0 bin
comm_modify vel yes
# ------------------------ FORCE FIELDS ------------------------------
pair_style born/coul/dsf/cs 0.1 20.0 20.0 # A, rho, sigma=0, C, D
pair_coeff * * 0.0 1.000 0.00 0.00 0.00
pair_coeff 3 3 487.0 0.23768 0.00 1.05 0.50 #Na-Na
pair_coeff 3 4 145134.0 0.23768 0.00 6.99 8.70 #Na-Cl
pair_coeff 4 4 405774.0 0.23768 0.00 72.40 145.40 #Cl-Cl
bond_style harmonic
bond_coeff 1 63.014 0.0
bond_coeff 2 25.724 0.0
# ------------------------ Equilibration Run -------------------------------
reset_timestep 0
thermo 50
thermo_style custom step etotal pe ke temp press &
epair evdwl ecoul elong ebond fnorm fmax vol
compute CSequ all temp/cs cores shells
# output via chunk method
#compute prop all property/atom i_CSID
#compute cs_chunk all chunk/atom c_prop
#compute cstherm all temp/chunk cs_chunk temp internal com yes cdof 3.0
#fix ave_chunk all ave/time 100 1 100 c_cstherm file chunk.dump mode vector
thermo_modify temp CSequ
# velocity bias option
velocity all create 1427 134 dist gaussian mom yes rot no bias yes temp CSequ
velocity all scale 1427 temp CSequ
fix thermoberendsen all temp/berendsen 1427 1427 0.4
fix nve all nve
fix_modify thermoberendsen temp CSequ
# 2 fmsec timestep
timestep 0.002
run 500
unfix thermoberendsen
# ------------------------ Dynamic Run -------------------------------
run 1000

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@ -0,0 +1,185 @@
LAMMPS (27 Oct 2016)
# Testsystem for core-shell model compared to Mitchel and Finchham
# Hendrik Heenen, June 2014
# ------------------------ INITIALIZATION ----------------------------
units metal
dimension 3
boundary p p p
atom_style full
# ----------------------- ATOM DEFINITION ----------------------------
fix csinfo all property/atom i_CSID
read_data data.coreshell fix csinfo NULL CS-Info
orthogonal box = (0 0 0) to (24.096 24.096 24.096)
1 by 1 by 1 MPI processor grid
reading atoms ...
432 atoms
scanning bonds ...
1 = max bonds/atom
reading bonds ...
216 bonds
1 = max # of 1-2 neighbors
0 = max # of 1-3 neighbors
0 = max # of 1-4 neighbors
1 = max # of special neighbors
group cores type 1 2
216 atoms in group cores
group shells type 3 4
216 atoms in group shells
neighbor 2.0 bin
comm_modify vel yes
# ------------------------ FORCE FIELDS ------------------------------
pair_style born/coul/dsf/cs 0.1 20.0 20.0 # A, rho, sigma=0, C, D
pair_coeff * * 0.0 1.000 0.00 0.00 0.00
pair_coeff 3 3 487.0 0.23768 0.00 1.05 0.50 #Na-Na
pair_coeff 3 4 145134.0 0.23768 0.00 6.99 8.70 #Na-Cl
pair_coeff 4 4 405774.0 0.23768 0.00 72.40 145.40 #Cl-Cl
bond_style harmonic
bond_coeff 1 63.014 0.0
bond_coeff 2 25.724 0.0
# ------------------------ Equilibration Run -------------------------------
reset_timestep 0
thermo 50
thermo_style custom step etotal pe ke temp press epair evdwl ecoul elong ebond fnorm fmax vol
compute CSequ all temp/cs cores shells
# output via chunk method
#compute prop all property/atom i_CSID
#compute cs_chunk all chunk/atom c_prop
#compute cstherm all temp/chunk cs_chunk temp internal com yes cdof 3.0
#fix ave_chunk all ave/time 100 1 100 c_cstherm file chunk.dump mode vector
thermo_modify temp CSequ
# velocity bias option
velocity all create 1427 134 dist gaussian mom yes rot no bias yes temp CSequ
Neighbor list info ...
1 neighbor list requests
update every 1 steps, delay 10 steps, check yes
max neighbors/atom: 2000, page size: 100000
master list distance cutoff = 22
ghost atom cutoff = 22
binsize = 11 -> bins = 3 3 3
velocity all scale 1427 temp CSequ
fix thermoberendsen all temp/berendsen 1427 1427 0.4
fix nve all nve
fix_modify thermoberendsen temp CSequ
# 2 fmsec timestep
timestep 0.002
run 500
Memory usage per processor = 7.04355 Mbytes
Step TotEng PotEng KinEng Temp Press E_pair E_vdwl E_coul E_long E_bond Fnorm Fmax Volume
0 -635.80596 -675.46362 39.657659 1427 -21302.622 -675.46362 1.6320365 -677.09565 0 0 1.3517686e-14 2.942091e-15 13990.5
50 -633.9898 -666.02679 32.03699 1152.7858 -4578.5681 -668.50431 37.800204 -706.30452 0 2.4775226 14.568073 4.3012389 13990.5
100 -631.89604 -661.96148 30.065442 1081.8436 -3536.6738 -664.61798 39.18583 -703.80381 0 2.6564973 14.677968 3.9051029 13990.5
150 -630.08723 -662.95879 32.871559 1182.816 -109.19506 -665.76772 46.247821 -712.01554 0 2.8089226 15.270039 2.9328953 13990.5
200 -628.55895 -663.97376 35.414806 1274.3296 -1748.35 -666.58439 41.738552 -708.32294 0 2.6106349 14.148282 3.1047826 13990.5
250 -627.28761 -661.92274 34.635123 1246.2743 -1280.4899 -664.917 43.045475 -707.96247 0 2.9942594 14.248617 2.4694705 13990.5
300 -626.6163 -663.65651 37.040209 1332.8164 -1887.9043 -666.35215 40.84964 -707.20179 0 2.6956373 13.142643 1.9263242 13990.5
350 -625.76781 -664.66441 38.896607 1399.6151 -1839.482 -667.47659 40.999206 -708.47579 0 2.8121749 13.601238 1.9262698 13990.5
400 -625.02586 -661.46042 36.434568 1311.0236 -868.2031 -664.40231 43.21398 -707.61629 0 2.9418875 14.945389 2.7493413 13990.5
450 -624.3278 -660.50844 36.180639 1301.8865 -2203.3944 -663.49896 40.008669 -703.50763 0 2.9905179 14.158866 1.7299899 13990.5
500 -623.56254 -661.33839 37.775849 1359.2869 -810.50736 -664.11652 42.993999 -707.11052 0 2.7781274 13.68709 2.9115277 13990.5
Loop time of 10.7162 on 1 procs for 500 steps with 432 atoms
Performance: 8.063 ns/day, 2.977 hours/ns, 46.658 timesteps/s
99.9% CPU use with 1 MPI tasks x no OpenMP threads
MPI task timing breakdown:
Section | min time | avg time | max time |%varavg| %total
---------------------------------------------------------------
Pair | 10.478 | 10.478 | 10.478 | 0.0 | 97.78
Bond | 0.0029511 | 0.0029511 | 0.0029511 | 0.0 | 0.03
Neigh | 0.14159 | 0.14159 | 0.14159 | 0.0 | 1.32
Comm | 0.074382 | 0.074382 | 0.074382 | 0.0 | 0.69
Output | 0.00054097 | 0.00054097 | 0.00054097 | 0.0 | 0.01
Modify | 0.010588 | 0.010588 | 0.010588 | 0.0 | 0.10
Other | | 0.007748 | | | 0.07
Nlocal: 432 ave 432 max 432 min
Histogram: 1 0 0 0 0 0 0 0 0 0
Nghost: 9280 ave 9280 max 9280 min
Histogram: 1 0 0 0 0 0 0 0 0 0
Neighs: 297636 ave 297636 max 297636 min
Histogram: 1 0 0 0 0 0 0 0 0 0
Total # of neighbors = 297636
Ave neighs/atom = 688.972
Ave special neighs/atom = 1
Neighbor list builds = 20
Dangerous builds = 0
unfix thermoberendsen
# ------------------------ Dynamic Run -------------------------------
run 1000
Memory usage per processor = 7.04355 Mbytes
Step TotEng PotEng KinEng Temp Press E_pair E_vdwl E_coul E_long E_bond Fnorm Fmax Volume
500 -623.56254 -661.33839 37.775849 1359.2869 -810.50736 -664.11652 42.993999 -707.11052 0 2.7781274 13.68709 2.9115277 13990.5
550 -623.5004 -660.74472 37.244326 1340.1611 -1413.4326 -663.99669 41.875014 -705.8717 0 3.2519651 15.097948 2.278405 13990.5
600 -623.46963 -659.61729 36.147655 1300.6997 -521.50578 -662.54994 43.956071 -706.50601 0 2.9326492 14.99649 2.6334959 13990.5
650 -623.49291 -661.50698 38.014069 1367.8588 -1230.0925 -664.21074 42.027844 -706.23859 0 2.7037578 13.982308 1.6247207 13990.5
700 -623.4913 -660.11564 36.62434 1317.8522 -727.89052 -663.24921 43.413397 -706.66261 0 3.1335699 15.009937 2.0563966 13990.5
750 -623.50292 -657.95982 34.4569 1239.8613 636.46644 -661.16971 46.539267 -707.70898 0 3.2098934 15.25993 2.1864622 13990.5
800 -623.5176 -659.92032 36.402711 1309.8773 -912.75799 -662.84989 42.668309 -705.5182 0 2.9295708 13.577516 2.0006099 13990.5
850 -623.44098 -660.92727 37.486295 1348.8679 -550.40358 -664.08308 43.667245 -707.75033 0 3.1558098 14.836208 2.279198 13990.5
900 -623.46361 -661.21737 37.753765 1358.4923 1267.8647 -664.52195 47.67284 -712.19479 0 3.3045765 15.058502 1.886141 13990.5
950 -623.50114 -660.58464 37.083492 1334.3739 1754.7359 -663.48186 48.70363 -712.18549 0 2.897226 15.519042 2.2654928 13990.5
1000 -623.50161 -660.02915 36.527539 1314.369 228.76104 -663.31152 45.374099 -708.68562 0 3.2823685 14.783709 2.4201134 13990.5
1050 -623.45985 -660.57417 37.114321 1335.4832 -1490.604 -663.75391 41.258878 -705.01279 0 3.1797391 14.250262 2.3153255 13990.5
1100 -623.51051 -661.20338 37.692871 1356.3011 1791.7899 -664.01042 48.626451 -712.63687 0 2.807039 15.559872 3.184101 13990.5
1150 -623.51067 -663.19545 39.684776 1427.9758 1023.0584 -666.07723 46.5628 -712.64003 0 2.8817804 13.895322 2.3950292 13990.5
1200 -623.49625 -659.6715 36.175253 1301.6927 1600.2805 -662.62259 48.522365 -711.14495 0 2.9510854 15.567834 2.1677651 13990.5
1250 -623.48282 -660.56735 37.084533 1334.4113 -871.67341 -663.86673 42.560699 -706.42743 0 3.2993759 14.569539 2.0093709 13990.5
1300 -623.47744 -663.63125 40.153811 1444.853 1343.7147 -666.39564 47.104842 -713.50048 0 2.7643857 14.186019 1.4599359 13990.5
1350 -623.49121 -661.42731 37.936096 1365.0531 589.73669 -664.46099 45.947687 -710.40867 0 3.0336821 14.801223 2.7486556 13990.5
1400 -623.50803 -660.03912 36.53109 1314.4968 362.97431 -663.24909 45.772904 -709.02199 0 3.2099708 14.566488 1.9170714 13990.5
1450 -623.51243 -659.65548 36.143052 1300.534 2853.0755 -663.0534 51.355353 -714.40875 0 3.3979157 15.890282 2.5251359 13990.5
1500 -623.51621 -661.87741 38.361201 1380.3496 740.04973 -665.00896 46.208742 -711.2177 0 3.1315492 15.168927 2.4710846 13990.5
Loop time of 22.2766 on 1 procs for 1000 steps with 432 atoms
Performance: 7.757 ns/day, 3.094 hours/ns, 44.890 timesteps/s
99.9% CPU use with 1 MPI tasks x no OpenMP threads
MPI task timing breakdown:
Section | min time | avg time | max time |%varavg| %total
---------------------------------------------------------------
Pair | 21.8 | 21.8 | 21.8 | 0.0 | 97.86
Bond | 0.005852 | 0.005852 | 0.005852 | 0.0 | 0.03
Neigh | 0.30423 | 0.30423 | 0.30423 | 0.0 | 1.37
Comm | 0.14388 | 0.14388 | 0.14388 | 0.0 | 0.65
Output | 0.0010855 | 0.0010855 | 0.0010855 | 0.0 | 0.00
Modify | 0.0064189 | 0.0064189 | 0.0064189 | 0.0 | 0.03
Other | | 0.01527 | | | 0.07
Nlocal: 432 ave 432 max 432 min
Histogram: 1 0 0 0 0 0 0 0 0 0
Nghost: 9318 ave 9318 max 9318 min
Histogram: 1 0 0 0 0 0 0 0 0 0
Neighs: 297131 ave 297131 max 297131 min
Histogram: 1 0 0 0 0 0 0 0 0 0
Total # of neighbors = 297131
Ave neighs/atom = 687.803
Ave special neighs/atom = 1
Neighbor list builds = 44
Dangerous builds = 0
Total wall time: 0:00:33

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@ -0,0 +1,74 @@
# DATE: 2013-03-21 CONTRIBUTOR: Cem Sevik CITATION: Kinaci, Haskins, Sevik and Cagin, Phys Rev B, 86, 115410 (2012)
# Tersoff parameters for B, C, and BN-C hybrid based graphene like nano structures
# multiple entries can be added to this file, LAMMPS reads the ones it needs
# these entries are in LAMMPS "metal" units:
# A,B = eV; lambda1,lambda2,lambda3 = 1/Angstroms; R,D = Angstroms
# other quantities are unitless
# Cem Sevik (csevik at anadolu.edu.tr) takes full blame for this
# file. It specifies B-N, B-C, and N-C interaction parameters
# generated and published by the reseacrh group of Prof. Tahir Cagin.
# 1. Physical Review B 84, 085409 2011
# Characterization of thermal transport in low-dimensional boron nitride nanostructures,
#
# 2. Physical Review B 86, 075403 2012
# Influence of disorder on thermal transport properties of boron nitride nanostructures
#
# 3. Physical Review B 86, 075403 2012, Please see for further information about B-C and N-C parameters
# Thermal conductivity of BN-C nanostructures
#
# The file also specifies C-C, interaction parameters
# generated and published by the reseacrh group of Dr. D. A. Broido
# Physical Review B 81, 205441 2010
# Optimized Tersoff and Brenner empirical potential parameters for
# lattice dynamics and phonon thermal transport in carbon nanotubes and graphene
# Users in referring the full parameters can cite the full parameter paper (3) as:
# A. Kinaci, J. B. Haskins, C. Sevik, T. Cagin, Physical Review B 86, 115410 (2012)
# Thermal conductivity of BN-C nanostructures
#
# format of a single entry (one or more lines):
# element 1, element 2, element 3,
# m, gamma, lambda3, c, d, costheta0, n, beta, lambda2, B, R, D, lambda1, A
N B B 3.0 1.0 0.0 25000 4.3484 -0.89000 0.72751 1.25724e-7 2.199 340.00 1.95 0.05 3.568 1380.0
N B N 3.0 1.0 0.0 25000 4.3484 -0.89000 0.72751 1.25724e-7 2.199 340.00 1.95 0.05 3.568 1380.0
N B C 3.0 1.0 0.0 25000 4.3484 -0.89000 0.72751 1.25724e-7 2.199 340.00 1.95 0.05 3.568 1380.0
B N B 3.0 1.0 0.0 25000 4.3484 -0.89000 0.72751 1.25724e-7 2.199 340.00 1.95 0.05 3.568 1380.0
B N N 3.0 1.0 0.0 25000 4.3484 -0.89000 0.72751 1.25724e-7 2.199 340.00 1.95 0.05 3.568 1380.0
B N C 3.0 1.0 0.0 25000 4.3484 -0.89000 0.72751 1.25724e-7 2.199 340.00 1.95 0.05 3.568 1380.0
N N B 3.0 1.0 0.0 17.7959 5.9484 0.00000 0.6184432 0.019251 2.6272721 138.77866 2.0 0.1 2.8293093 128.86866
N N N 3.0 1.0 0.0 17.7959 5.9484 0.00000 0.6184432 0.019251 2.6272721 138.77866 2.0 0.1 2.8293093 128.86866
N N C 3.0 1.0 0.0 17.7959 5.9484 0.00000 0.6184432 0.019251 2.6272721 138.77866 2.0 0.1 2.8293093 128.86866
B B B 3.0 1.0 0.0 0.52629 0.001587 0.5 3.9929061 1.6e-6 2.0774982 43.132016 2.0 0.1 2.2372578 40.0520156
B B N 3.0 1.0 0.0 0.52629 0.001587 0.5 3.9929061 1.6e-6 2.0774982 43.132016 2.0 0.1 2.2372578 40.0520156
B B C 3.0 1.0 0.0 0.52629 0.001587 0.5 3.9929061 1.6e-6 2.0774982 43.132016 2.0 0.1 2.2372578 40.0520156
C C C 3.0 1.0 0.0 3.8049e4 4.3484 -0.93000 0.72751 1.5724e-7 2.2119 430.00 1.95 0.15 3.4879 1393.6
C C B 3.0 1.0 0.0 3.8049e4 4.3484 -0.93000 0.72751 1.5724e-7 2.2119 430.00 1.95 0.15 3.4879 1393.6
C C N 3.0 1.0 0.0 3.8049e4 4.3484 -0.93000 0.72751 1.5724e-7 2.2119 430.00 1.95 0.15 3.4879 1393.6
C B B 3.0 1.0 0.0 3.8049e4 4.3484 -0.93000 0.72751 1.5724e-7 2.2054 339.068910 1.95 0.10 3.5279 1386.78
C B N 3.0 1.0 0.0 3.8049e4 4.3484 -0.93000 0.72751 1.5724e-7 2.2054 339.068910 1.95 0.10 3.5279 1386.78
C B C 3.0 1.0 0.0 3.8049e4 4.3484 -0.93000 0.72751 1.5724e-7 2.2054 339.068910 1.95 0.10 3.5279 1386.78
C N B 3.0 1.0 0.0 3.8049e4 4.3484 -0.93000 0.72751 1.5724e-7 2.2054 387.575152 1.95 0.10 3.5279 1386.78
C N N 3.0 1.0 0.0 3.8049e4 4.3484 -0.93000 0.72751 1.5724e-7 2.2054 387.575152 1.95 0.10 3.5279 1386.78
C N C 3.0 1.0 0.0 3.8049e4 4.3484 -0.93000 0.72751 1.5724e-7 2.2054 387.575152 1.95 0.10 3.5279 1386.78
B C C 3.0 1.0 0.0 25000 4.3484 -0.89000 0.72751 1.25724e-7 2.2054 339.068910 1.95 0.10 3.5279 1386.78
B C B 3.0 1.0 0.0 25000 4.3484 -0.89000 0.72751 1.25724e-7 2.2054 339.068910 1.95 0.10 3.5279 1386.78
B C N 3.0 1.0 0.0 25000 4.3484 -0.89000 0.72751 1.25724e-7 2.2054 339.068910 1.95 0.10 3.5279 1386.78
N C C 3.0 1.0 0.0 25000 4.3484 -0.89000 0.72751 1.25724e-7 2.2054 387.575152 1.95 0.10 3.5279 1386.78
N C B 3.0 1.0 0.0 25000 4.3484 -0.89000 0.72751 1.25724e-7 2.2054 387.575152 1.95 0.10 3.5279 1386.78
N C N 3.0 1.0 0.0 25000 4.3484 -0.89000 0.72751 1.25724e-7 2.2054 387.575152 1.95 0.10 3.5279 1386.78

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@ -0,0 +1,233 @@
### DATE: 2013-08-09 CONTRIBUTOR: X. W. Zhou, xzhou@sandia.gov, CITATION: Zhou, Ward, Martin, van Swol, Cruz-Campa, and D. Zubia, Phys. Rev. B, 88, 085309 (2013).
#
# Note that the way the parameters can be entered is not unique.
# As one way, we assume that eps_ijk is equal to eps_ik and
# lambda_ijk is equal to sqrt(lambda_ij*eps_ij*lambda_ik*eps_ik)/eps_ik,
# and all other parameters in the ijk line are for ik.
#
# The twobody ik pair parameters are entered on the i*k lines, where *
# can be any species. This is consistent with the LAMMPS requirement
# that twobody ik parameters be defined on the ikk line. Entries on all
# the other i*k lines are ignored by LAMMPS
#
# These entries are in LAMMPS "metal" units: epsilon = eV;
# sigma = Angstroms; other quantities are unitless
#
# cutoff distance = 4.632
# eps sigma a lambda gamma cos(theta) A B p q tol
Cd Cd Cd 1.182358e+00 2.663951e+00 1.527956e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.674460e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd Cd Te 1.385284e+00 2.352141e+00 1.810919e+00 3.002537e+01 1.200000e+00 -3.333333e-01 7.049600e+00 8.861252e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd Cd Zn 6.908179e-01 2.238699e+00 1.812616e+00 4.251831e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.010632e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd Cd Se 1.352371e+00 2.045165e+00 1.953387e+00 3.038855e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.116149e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd Cd Hg 4.881231e-01 2.432694e+00 1.677987e+00 5.058167e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.250999e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd Cd S 1.300376e+00 1.804151e+00 2.124568e+00 3.099013e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.540087e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd Te Cd 1.182358e+00 2.663951e+00 1.527956e+00 3.517858e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.674460e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd Te Te 1.385284e+00 2.352141e+00 1.810919e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 8.861252e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd Te Zn 6.908179e-01 2.238699e+00 1.812616e+00 4.602259e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.010632e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd Te Se 1.352371e+00 2.045165e+00 1.953387e+00 3.289311e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.116149e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd Te Hg 4.881231e-01 2.432694e+00 1.677987e+00 5.475051e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.250999e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd Te S 1.300376e+00 1.804151e+00 2.124568e+00 3.354428e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.540087e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd Zn Cd 1.182358e+00 2.663951e+00 1.527956e+00 2.484224e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.674460e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd Zn Te 1.385284e+00 2.352141e+00 1.810919e+00 2.295069e+01 1.200000e+00 -3.333333e-01 7.049600e+00 8.861252e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd Zn Zn 6.908179e-01 2.238699e+00 1.812616e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.010632e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd Zn Se 1.352371e+00 2.045165e+00 1.953387e+00 2.322829e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.116149e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd Zn Hg 4.881231e-01 2.432694e+00 1.677987e+00 3.866344e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.250999e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd Zn S 1.300376e+00 1.804151e+00 2.124568e+00 2.368813e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.540087e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd Se Cd 1.182358e+00 2.663951e+00 1.527956e+00 3.475816e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.674460e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd Se Te 1.385284e+00 2.352141e+00 1.810919e+00 3.211159e+01 1.200000e+00 -3.333333e-01 7.049600e+00 8.861252e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd Se Zn 6.908179e-01 2.238699e+00 1.812616e+00 4.547256e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.010632e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd Se Se 1.352371e+00 2.045165e+00 1.953387e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.116149e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd Se Hg 4.881231e-01 2.432694e+00 1.677987e+00 5.409618e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.250999e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd Se S 1.300376e+00 1.804151e+00 2.124568e+00 3.314338e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.540087e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd Hg Cd 1.182358e+00 2.663951e+00 1.527956e+00 2.088207e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.674460e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd Hg Te 1.385284e+00 2.352141e+00 1.810919e+00 1.929206e+01 1.200000e+00 -3.333333e-01 7.049600e+00 8.861252e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd Hg Zn 6.908179e-01 2.238699e+00 1.812616e+00 2.731909e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.010632e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd Hg Se 1.352371e+00 2.045165e+00 1.953387e+00 1.952541e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.116149e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd Hg Hg 4.881231e-01 2.432694e+00 1.677987e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.250999e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd Hg S 1.300376e+00 1.804151e+00 2.124568e+00 1.991194e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.540087e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd S Cd 1.182358e+00 2.663951e+00 1.527956e+00 3.408343e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.674460e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd S Te 1.385284e+00 2.352141e+00 1.810919e+00 3.148823e+01 1.200000e+00 -3.333333e-01 7.049600e+00 8.861252e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd S Zn 6.908179e-01 2.238699e+00 1.812616e+00 4.458985e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.010632e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd S Se 1.352371e+00 2.045165e+00 1.953387e+00 3.186911e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.116149e+00 4.000000e+00 0.000000e+00 0.000000e+00
Cd S Hg 4.881231e-01 2.432694e+00 1.677987e+00 5.304605e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.250999e-01 4.000000e+00 0.000000e+00 0.000000e+00
Cd S S 1.300376e+00 1.804151e+00 2.124568e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.540087e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te Cd Cd 1.385284e+00 2.352141e+00 1.810919e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 8.861252e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te Cd Te 1.849775e+00 2.905254e+00 1.594353e+00 2.812506e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.307283e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te Cd Zn 1.546239e+00 2.056363e+00 1.907922e+00 3.076200e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.255846e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te Cd Se 1.295053e+00 2.231716e+00 1.809645e+00 3.361313e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.005396e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te Cd Hg 1.204715e+00 2.135591e+00 1.892491e+00 3.485063e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.445180e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te Cd S 1.450015e+00 2.297301e+00 1.726905e+00 3.176630e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.794685e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te Te Cd 1.385284e+00 2.352141e+00 1.810919e+00 3.755548e+01 1.200000e+00 -3.333333e-01 7.049600e+00 8.861252e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te Te Te 1.849775e+00 2.905254e+00 1.594353e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.307283e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te Te Zn 1.546239e+00 2.056363e+00 1.907922e+00 3.554713e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.255846e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te Te Se 1.295053e+00 2.231716e+00 1.809645e+00 3.884177e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.005396e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te Te Hg 1.204715e+00 2.135591e+00 1.892491e+00 4.027176e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.445180e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te Te S 1.450015e+00 2.297301e+00 1.726905e+00 3.670765e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.794685e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te Zn Cd 1.385284e+00 2.352141e+00 1.810919e+00 3.433620e+01 1.200000e+00 -3.333333e-01 7.049600e+00 8.861252e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te Zn Te 1.849775e+00 2.905254e+00 1.594353e+00 2.971408e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.307283e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te Zn Zn 1.546239e+00 2.056363e+00 1.907922e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.255846e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te Zn Se 1.295053e+00 2.231716e+00 1.809645e+00 3.551222e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.005396e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te Zn Hg 1.204715e+00 2.135591e+00 1.892491e+00 3.681964e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.445180e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te Zn S 1.450015e+00 2.297301e+00 1.726905e+00 3.356105e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.794685e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te Se Cd 1.385284e+00 2.352141e+00 1.810919e+00 3.142373e+01 1.200000e+00 -3.333333e-01 7.049600e+00 8.861252e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te Se Te 1.849775e+00 2.905254e+00 1.594353e+00 2.719366e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.307283e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te Se Zn 1.546239e+00 2.056363e+00 1.907922e+00 2.974328e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.255846e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te Se Se 1.295053e+00 2.231716e+00 1.809645e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.005396e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te Se Hg 1.204715e+00 2.135591e+00 1.892491e+00 3.369652e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.445180e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te Se S 1.450015e+00 2.297301e+00 1.726905e+00 3.071433e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.794685e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te Hg Cd 1.385284e+00 2.352141e+00 1.810919e+00 3.030791e+01 1.200000e+00 -3.333333e-01 7.049600e+00 8.861252e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te Hg Te 1.849775e+00 2.905254e+00 1.594353e+00 2.622805e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.307283e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te Hg Zn 1.546239e+00 2.056363e+00 1.907922e+00 2.868714e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.255846e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te Hg Se 1.295053e+00 2.231716e+00 1.809645e+00 3.134597e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.005396e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te Hg Hg 1.204715e+00 2.135591e+00 1.892491e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.445180e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te Hg S 1.450015e+00 2.297301e+00 1.726905e+00 2.962370e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.794685e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te S Cd 1.385284e+00 2.352141e+00 1.810919e+00 3.325065e+01 1.200000e+00 -3.333333e-01 7.049600e+00 8.861252e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te S Te 1.849775e+00 2.905254e+00 1.594353e+00 2.877465e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.307283e-01 4.000000e+00 0.000000e+00 0.000000e+00
Te S Zn 1.546239e+00 2.056363e+00 1.907922e+00 3.147250e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.255846e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te S Se 1.295053e+00 2.231716e+00 1.809645e+00 3.438949e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.005396e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te S Hg 1.204715e+00 2.135591e+00 1.892491e+00 3.565557e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.445180e+00 4.000000e+00 0.000000e+00 0.000000e+00
Te S S 1.450015e+00 2.297301e+00 1.726905e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.794685e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Cd Cd 6.908179e-01 2.238699e+00 1.812616e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.010632e+00 4.000000e+00 0.000000e+00 0.000000e+00
Zn Cd Te 1.546239e+00 2.056363e+00 1.907922e+00 2.172335e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.255846e+00 4.000000e+00 0.000000e+00 0.000000e+00
Zn Cd Zn 1.392961e+00 2.367650e+00 1.525521e+00 2.288736e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.676279e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Cd Se 1.691181e+00 2.028827e+00 1.836907e+00 2.077161e+01 1.200000e+00 -3.333333e-01 7.049600e+00 9.510930e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Cd Hg 4.951616e-01 2.239186e+00 1.761363e+00 3.838766e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.461167e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Cd S 2.208390e+00 2.323783e+00 1.589241e+00 1.817721e+01 1.200000e+00 -3.333333e-01 7.049600e+00 4.643181e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Te Cd 6.908179e-01 2.238699e+00 1.812616e+00 4.862279e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.010632e+00 4.000000e+00 0.000000e+00 0.000000e+00
Zn Te Te 1.546239e+00 2.056363e+00 1.907922e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.255846e+00 4.000000e+00 0.000000e+00 0.000000e+00
Zn Te Zn 1.392961e+00 2.367650e+00 1.525521e+00 3.424146e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.676279e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Te Se 1.691181e+00 2.028827e+00 1.836907e+00 3.107611e+01 1.200000e+00 -3.333333e-01 7.049600e+00 9.510930e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Te Hg 4.951616e-01 2.239186e+00 1.761363e+00 5.743124e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.461167e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Te S 2.208390e+00 2.323783e+00 1.589241e+00 2.719467e+01 1.200000e+00 -3.333333e-01 7.049600e+00 4.643181e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Zn Cd 6.908179e-01 2.238699e+00 1.812616e+00 4.614993e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.010632e+00 4.000000e+00 0.000000e+00 0.000000e+00
Zn Zn Te 1.546239e+00 2.056363e+00 1.907922e+00 3.084711e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.255846e+00 4.000000e+00 0.000000e+00 0.000000e+00
Zn Zn Zn 1.392961e+00 2.367650e+00 1.525521e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.676279e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Zn Se 1.691181e+00 2.028827e+00 1.836907e+00 2.949563e+01 1.200000e+00 -3.333333e-01 7.049600e+00 9.510930e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Zn Hg 4.951616e-01 2.239186e+00 1.761363e+00 5.451040e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.461167e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Zn S 2.208390e+00 2.323783e+00 1.589241e+00 2.581160e+01 1.200000e+00 -3.333333e-01 7.049600e+00 4.643181e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Se Cd 6.908179e-01 2.238699e+00 1.812616e+00 5.085067e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.010632e+00 4.000000e+00 0.000000e+00 0.000000e+00
Zn Se Te 1.546239e+00 2.056363e+00 1.907922e+00 3.398914e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.255846e+00 4.000000e+00 0.000000e+00 0.000000e+00
Zn Se Zn 1.392961e+00 2.367650e+00 1.525521e+00 3.581039e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.676279e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Se Se 1.691181e+00 2.028827e+00 1.836907e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 9.510930e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Se Hg 4.951616e-01 2.239186e+00 1.761363e+00 6.006272e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.461167e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Se S 2.208390e+00 2.323783e+00 1.589241e+00 2.844072e+01 1.200000e+00 -3.333333e-01 7.049600e+00 4.643181e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Hg Cd 6.908179e-01 2.238699e+00 1.812616e+00 2.751535e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.010632e+00 4.000000e+00 0.000000e+00 0.000000e+00
Zn Hg Te 1.546239e+00 2.056363e+00 1.907922e+00 1.839156e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.255846e+00 4.000000e+00 0.000000e+00 0.000000e+00
Zn Hg Zn 1.392961e+00 2.367650e+00 1.525521e+00 1.937704e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.676279e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Hg Se 1.691181e+00 2.028827e+00 1.836907e+00 1.758578e+01 1.200000e+00 -3.333333e-01 7.049600e+00 9.510930e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Hg Hg 4.951616e-01 2.239186e+00 1.761363e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.461167e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn Hg S 2.208390e+00 2.323783e+00 1.589241e+00 1.538930e+01 1.200000e+00 -3.333333e-01 7.049600e+00 4.643181e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn S Cd 6.908179e-01 2.238699e+00 1.812616e+00 5.810847e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.010632e+00 4.000000e+00 0.000000e+00 0.000000e+00
Zn S Te 1.546239e+00 2.056363e+00 1.907922e+00 3.884033e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.255846e+00 4.000000e+00 0.000000e+00 0.000000e+00
Zn S Zn 1.392961e+00 2.367650e+00 1.525521e+00 4.092153e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.676279e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn S Se 1.691181e+00 2.028827e+00 1.836907e+00 3.713865e+01 1.200000e+00 -3.333333e-01 7.049600e+00 9.510930e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn S Hg 4.951616e-01 2.239186e+00 1.761363e+00 6.863534e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.461167e-01 4.000000e+00 0.000000e+00 0.000000e+00
Zn S S 2.208390e+00 2.323783e+00 1.589241e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 4.643181e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se Cd Cd 1.352371e+00 2.045165e+00 1.953387e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.116149e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se Cd Te 1.295053e+00 2.231716e+00 1.809645e+00 3.321142e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.005396e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se Cd Zn 1.691181e+00 2.028827e+00 1.836907e+00 2.906271e+01 1.200000e+00 -3.333333e-01 7.049600e+00 9.510930e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se Cd Se 2.400781e+00 2.789002e+00 1.544925e+00 2.439242e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.672131e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se Cd Hg 1.299758e+00 2.113406e+00 1.831821e+00 3.315126e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.150200e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se Cd S 1.307592e+00 2.229392e+00 1.747782e+00 3.305180e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.932325e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se Te Cd 1.352371e+00 2.045165e+00 1.953387e+00 3.180382e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.116149e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se Te Te 1.295053e+00 2.231716e+00 1.809645e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.005396e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se Te Zn 1.691181e+00 2.028827e+00 1.836907e+00 2.844016e+01 1.200000e+00 -3.333333e-01 7.049600e+00 9.510930e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se Te Se 2.400781e+00 2.789002e+00 1.544925e+00 2.386992e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.672131e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se Te Hg 1.299758e+00 2.113406e+00 1.831821e+00 3.244113e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.150200e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se Te S 1.307592e+00 2.229392e+00 1.747782e+00 3.234380e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.932325e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se Zn Cd 1.352371e+00 2.045165e+00 1.953387e+00 3.634382e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.116149e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se Zn Te 1.295053e+00 2.231716e+00 1.809645e+00 3.713938e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.005396e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se Zn Zn 1.691181e+00 2.028827e+00 1.836907e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 9.510930e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se Zn Se 2.400781e+00 2.789002e+00 1.544925e+00 2.727735e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.672131e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se Zn Hg 1.299758e+00 2.113406e+00 1.831821e+00 3.707211e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.150200e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se Zn S 1.307592e+00 2.229392e+00 1.747782e+00 3.696088e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.932325e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se Se Cd 1.352371e+00 2.045165e+00 1.953387e+00 4.330238e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.116149e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se Se Te 1.295053e+00 2.231716e+00 1.809645e+00 4.425026e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.005396e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se Se Zn 1.691181e+00 2.028827e+00 1.836907e+00 3.872260e+01 1.200000e+00 -3.333333e-01 7.049600e+00 9.510930e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se Se Se 2.400781e+00 2.789002e+00 1.544925e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.672131e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se Se Hg 1.299758e+00 2.113406e+00 1.831821e+00 4.417011e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.150200e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se Se S 1.307592e+00 2.229392e+00 1.747782e+00 4.403758e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.932325e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se Hg Cd 1.352371e+00 2.045165e+00 1.953387e+00 3.186153e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.116149e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se Hg Te 1.295053e+00 2.231716e+00 1.809645e+00 3.255898e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.005396e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se Hg Zn 1.691181e+00 2.028827e+00 1.836907e+00 2.849177e+01 1.200000e+00 -3.333333e-01 7.049600e+00 9.510930e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se Hg Se 2.400781e+00 2.789002e+00 1.544925e+00 2.391323e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.672131e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se Hg Hg 1.299758e+00 2.113406e+00 1.831821e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.150200e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se Hg S 1.307592e+00 2.229392e+00 1.747782e+00 3.240249e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.932325e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se S Cd 1.352371e+00 2.045165e+00 1.953387e+00 3.195742e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.116149e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se S Te 1.295053e+00 2.231716e+00 1.809645e+00 3.265696e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.005396e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se S Zn 1.691181e+00 2.028827e+00 1.836907e+00 2.857751e+01 1.200000e+00 -3.333333e-01 7.049600e+00 9.510930e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se S Se 2.400781e+00 2.789002e+00 1.544925e+00 2.398520e+01 1.200000e+00 -3.333333e-01 7.917000e+00 7.672131e-01 4.000000e+00 0.000000e+00 0.000000e+00
Se S Hg 1.299758e+00 2.113406e+00 1.831821e+00 3.259780e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.150200e+00 4.000000e+00 0.000000e+00 0.000000e+00
Se S S 1.307592e+00 2.229392e+00 1.747782e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.932325e-01 4.000000e+00 0.000000e+00 0.000000e+00
Hg Cd Cd 4.881231e-01 2.432694e+00 1.677987e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.250999e-01 4.000000e+00 0.000000e+00 0.000000e+00
Hg Cd Te 1.204715e+00 2.135591e+00 1.892491e+00 2.068740e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.445180e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Cd Zn 4.951616e-01 2.239186e+00 1.761363e+00 3.226819e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.461167e-01 4.000000e+00 0.000000e+00 0.000000e+00
Hg Cd Se 1.299758e+00 2.113406e+00 1.831821e+00 1.991668e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.150200e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Cd Hg 1.272807e+00 2.699097e+00 1.498503e+00 2.012643e+01 1.200000e+00 -3.333333e-01 7.917000e+00 1.211532e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Cd S 1.531211e+00 2.025045e+00 1.833708e+00 1.834976e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.184541e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Te Cd 4.881231e-01 2.432694e+00 1.677987e+00 5.105765e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.250999e-01 4.000000e+00 0.000000e+00 0.000000e+00
Hg Te Te 1.204715e+00 2.135591e+00 1.892491e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.445180e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Te Zn 4.951616e-01 2.239186e+00 1.761363e+00 5.069347e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.461167e-01 4.000000e+00 0.000000e+00 0.000000e+00
Hg Te Se 1.299758e+00 2.113406e+00 1.831821e+00 3.128919e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.150200e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Te Hg 1.272807e+00 2.699097e+00 1.498503e+00 3.161872e+01 1.200000e+00 -3.333333e-01 7.917000e+00 1.211532e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Te S 1.531211e+00 2.025045e+00 1.833708e+00 2.882756e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.184541e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Zn Cd 4.881231e-01 2.432694e+00 1.677987e+00 3.273348e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.250999e-01 4.000000e+00 0.000000e+00 0.000000e+00
Hg Zn Te 1.204715e+00 2.135591e+00 1.892491e+00 2.083602e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.445180e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Zn Zn 4.951616e-01 2.239186e+00 1.761363e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.461167e-01 4.000000e+00 0.000000e+00 0.000000e+00
Hg Zn Se 1.299758e+00 2.113406e+00 1.831821e+00 2.005976e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.150200e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Zn Hg 1.272807e+00 2.699097e+00 1.498503e+00 2.027102e+01 1.200000e+00 -3.333333e-01 7.917000e+00 1.211532e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Zn S 1.531211e+00 2.025045e+00 1.833708e+00 1.848159e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.184541e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Se Cd 4.881231e-01 2.432694e+00 1.677987e+00 5.303345e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.250999e-01 4.000000e+00 0.000000e+00 0.000000e+00
Hg Se Te 1.204715e+00 2.135591e+00 1.892491e+00 3.375766e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.445180e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Se Zn 4.951616e-01 2.239186e+00 1.761363e+00 5.265518e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.461167e-01 4.000000e+00 0.000000e+00 0.000000e+00
Hg Se Se 1.299758e+00 2.113406e+00 1.831821e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.150200e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Se Hg 1.272807e+00 2.699097e+00 1.498503e+00 3.284228e+01 1.200000e+00 -3.333333e-01 7.917000e+00 1.211532e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Se S 1.531211e+00 2.025045e+00 1.833708e+00 2.994311e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.184541e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Hg Cd 4.881231e-01 2.432694e+00 1.677987e+00 5.248074e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.250999e-01 4.000000e+00 0.000000e+00 0.000000e+00
Hg Hg Te 1.204715e+00 2.135591e+00 1.892491e+00 3.340584e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.445180e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Hg Zn 4.951616e-01 2.239186e+00 1.761363e+00 5.210641e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.461167e-01 4.000000e+00 0.000000e+00 0.000000e+00
Hg Hg Se 1.299758e+00 2.113406e+00 1.831821e+00 3.216129e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.150200e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Hg Hg 1.272807e+00 2.699097e+00 1.498503e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.917000e+00 1.211532e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg Hg S 1.531211e+00 2.025045e+00 1.833708e+00 2.963105e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.184541e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg S Cd 4.881231e-01 2.432694e+00 1.677987e+00 5.756205e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.250999e-01 4.000000e+00 0.000000e+00 0.000000e+00
Hg S Te 1.204715e+00 2.135591e+00 1.892491e+00 3.664028e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.445180e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg S Zn 4.951616e-01 2.239186e+00 1.761363e+00 5.715148e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.461167e-01 4.000000e+00 0.000000e+00 0.000000e+00
Hg S Se 1.299758e+00 2.113406e+00 1.831821e+00 3.527522e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.150200e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg S Hg 1.272807e+00 2.699097e+00 1.498503e+00 3.564673e+01 1.200000e+00 -3.333333e-01 7.917000e+00 1.211532e+00 4.000000e+00 0.000000e+00 0.000000e+00
Hg S S 1.531211e+00 2.025045e+00 1.833708e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.184541e+00 4.000000e+00 0.000000e+00 0.000000e+00
S Cd Cd 1.300376e+00 1.804151e+00 2.124568e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.540087e+00 4.000000e+00 0.000000e+00 0.000000e+00
S Cd Te 1.450015e+00 2.297301e+00 1.726905e+00 3.077737e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.794685e-01 4.000000e+00 0.000000e+00 0.000000e+00
S Cd Zn 2.208390e+00 2.323783e+00 1.589241e+00 2.493905e+01 1.200000e+00 -3.333333e-01 7.049600e+00 4.643181e-01 4.000000e+00 0.000000e+00 0.000000e+00
S Cd Se 1.307592e+00 2.229392e+00 1.747782e+00 3.241019e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.932325e-01 4.000000e+00 0.000000e+00 0.000000e+00
S Cd Hg 1.531211e+00 2.025045e+00 1.833708e+00 2.995023e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.184541e+00 4.000000e+00 0.000000e+00 0.000000e+00
S Cd S 2.434871e+00 2.423171e+00 1.711097e+00 2.375088e+01 1.200000e+00 -3.333333e-01 7.917000e+00 1.049688e+00 4.000000e+00 0.000000e+00 0.000000e+00
S Te Cd 1.300376e+00 1.804151e+00 2.124568e+00 3.431904e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.540087e+00 4.000000e+00 0.000000e+00 0.000000e+00
S Te Te 1.450015e+00 2.297301e+00 1.726905e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.794685e-01 4.000000e+00 0.000000e+00 0.000000e+00
S Te Zn 2.208390e+00 2.323783e+00 1.589241e+00 2.633490e+01 1.200000e+00 -3.333333e-01 7.049600e+00 4.643181e-01 4.000000e+00 0.000000e+00 0.000000e+00
S Te Se 1.307592e+00 2.229392e+00 1.747782e+00 3.422421e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.932325e-01 4.000000e+00 0.000000e+00 0.000000e+00
S Te Hg 1.531211e+00 2.025045e+00 1.833708e+00 3.162656e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.184541e+00 4.000000e+00 0.000000e+00 0.000000e+00
S Te S 2.434871e+00 2.423171e+00 1.711097e+00 2.508023e+01 1.200000e+00 -3.333333e-01 7.917000e+00 1.049688e+00 4.000000e+00 0.000000e+00 0.000000e+00
S Zn Cd 1.300376e+00 1.804151e+00 2.124568e+00 4.235326e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.540087e+00 4.000000e+00 0.000000e+00 0.000000e+00
S Zn Te 1.450015e+00 2.297301e+00 1.726905e+00 4.010837e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.794685e-01 4.000000e+00 0.000000e+00 0.000000e+00
S Zn Zn 2.208390e+00 2.323783e+00 1.589241e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 4.643181e-01 4.000000e+00 0.000000e+00 0.000000e+00
S Zn Se 1.307592e+00 2.229392e+00 1.747782e+00 4.223622e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.932325e-01 4.000000e+00 0.000000e+00 0.000000e+00
S Zn Hg 1.531211e+00 2.025045e+00 1.833708e+00 3.903046e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.184541e+00 4.000000e+00 0.000000e+00 0.000000e+00
S Zn S 2.434871e+00 2.423171e+00 1.711097e+00 3.095161e+01 1.200000e+00 -3.333333e-01 7.917000e+00 1.049688e+00 4.000000e+00 0.000000e+00 0.000000e+00
S Se Cd 1.300376e+00 1.804151e+00 2.124568e+00 3.259006e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.540087e+00 4.000000e+00 0.000000e+00 0.000000e+00
S Se Te 1.450015e+00 2.297301e+00 1.726905e+00 3.086266e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.794685e-01 4.000000e+00 0.000000e+00 0.000000e+00
S Se Zn 2.208390e+00 2.323783e+00 1.589241e+00 2.500815e+01 1.200000e+00 -3.333333e-01 7.049600e+00 4.643181e-01 4.000000e+00 0.000000e+00 0.000000e+00
S Se Se 1.307592e+00 2.229392e+00 1.747782e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.932325e-01 4.000000e+00 0.000000e+00 0.000000e+00
S Se Hg 1.531211e+00 2.025045e+00 1.833708e+00 3.003322e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.184541e+00 4.000000e+00 0.000000e+00 0.000000e+00
S Se S 2.434871e+00 2.423171e+00 1.711097e+00 2.381670e+01 1.200000e+00 -3.333333e-01 7.917000e+00 1.049688e+00 4.000000e+00 0.000000e+00 0.000000e+00
S Hg Cd 1.300376e+00 1.804151e+00 2.124568e+00 3.526684e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.540087e+00 4.000000e+00 0.000000e+00 0.000000e+00
S Hg Te 1.450015e+00 2.297301e+00 1.726905e+00 3.339756e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.794685e-01 4.000000e+00 0.000000e+00 0.000000e+00
S Hg Zn 2.208390e+00 2.323783e+00 1.589241e+00 2.706220e+01 1.200000e+00 -3.333333e-01 7.049600e+00 4.643181e-01 4.000000e+00 0.000000e+00 0.000000e+00
S Hg Se 1.307592e+00 2.229392e+00 1.747782e+00 3.516939e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.932325e-01 4.000000e+00 0.000000e+00 0.000000e+00
S Hg Hg 1.531211e+00 2.025045e+00 1.833708e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.184541e+00 4.000000e+00 0.000000e+00 0.000000e+00
S Hg S 2.434871e+00 2.423171e+00 1.711097e+00 2.577288e+01 1.200000e+00 -3.333333e-01 7.917000e+00 1.049688e+00 4.000000e+00 0.000000e+00 0.000000e+00
S S Cd 1.300376e+00 1.804151e+00 2.124568e+00 4.447203e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.540087e+00 4.000000e+00 0.000000e+00 0.000000e+00
S S Te 1.450015e+00 2.297301e+00 1.726905e+00 4.211484e+01 1.200000e+00 -3.333333e-01 7.049600e+00 7.794685e-01 4.000000e+00 0.000000e+00 0.000000e+00
S S Zn 2.208390e+00 2.323783e+00 1.589241e+00 3.412585e+01 1.200000e+00 -3.333333e-01 7.049600e+00 4.643181e-01 4.000000e+00 0.000000e+00 0.000000e+00
S S Se 1.307592e+00 2.229392e+00 1.747782e+00 4.434914e+01 1.200000e+00 -3.333333e-01 7.049600e+00 6.932325e-01 4.000000e+00 0.000000e+00 0.000000e+00
S S Hg 1.531211e+00 2.025045e+00 1.833708e+00 4.098300e+01 1.200000e+00 -3.333333e-01 7.049600e+00 1.184541e+00 4.000000e+00 0.000000e+00 0.000000e+00
S S S 2.434871e+00 2.423171e+00 1.711097e+00 3.250000e+01 1.200000e+00 -3.333333e-01 7.917000e+00 1.049688e+00 4.000000e+00 0.000000e+00 0.000000e+00

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@ -0,0 +1,38 @@
# DATE: 2015-10-14 CONTRIBUTOR: Aidan Thompson, athomps@sandia.gov CITATION: Branicio, Rino, Gan and Tsuzuki, J. Phys Condensed Matter 21 (2009) 095002
#
# Vashishta potential file for InP, Branicio, Rino, Gan and Tsuzuki,
# J. Phys Condensed Matter 21 (2009) 095002
#
# These entries are in LAMMPS "metal" units:
# H = eV*Angstroms^eta; Zi, Zj = |e| (e = electronic charge);
# lambda1, lambda4, rc, r0, gamma = Angstroms;
# D = eV*Angstroms^4; W = eV*Angstroms^6; B = eV;
# other quantities are unitless
# element1 element2 element3
# H eta Zi Zj lambda1 D lambda4
# W rc B gamma r0 C cos(theta)
In In In 273.584 7 -1.21 -1.21 4.5 0.0 2.75
0.0 6.0 0.0 0.0 0.0 0.0 0.0
P P P 1813.06 7 1.21 1.21 4.5 52.7067 2.75
0.0 6.0 0.0 0.0 0.0 0.0 -0.333333333333
In P P 4847.09 9 1.21 -1.21 4.5 26.3533 2.75
270.105 6.0 4.34967 1.0 3.55 7.0 -0.333333333333
P In In 4847.09 9 1.21 -1.21 4.5 26.3533 2.75
270.105 6.0 4.34967 1.0 3.55 7.0 -0.333333333333
In In P 0.0 0.0 0.0 0.0 0.0 0.0 0.0
0.0 0.0 0.0 0.0 0.0 0.0 0.0
In P In 0.0 0.0 0.0 0.0 0.0 0.0 0.0
0.0 0.0 0.0 0.0 0.0 0.0 0.0
P In P 0.0 0.0 0.0 0.0 0.0 0.0 0.0
0.0 0.0 0.0 0.0 0.0 0.0 0.0
P P In 0.0 0.0 0.0 0.0 0.0 0.0 0.0
0.0 0.0 0.0 0.0 0.0 0.0 0.0

18
examples/threebody/Si.sw Normal file
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@ -0,0 +1,18 @@
# DATE: 2007-06-11 CONTRIBUTOR: Aidan Thompson, athomps@sandia.gov CITATION: Stillinger and Weber, Phys Rev B, 31, 5262, (1985)
# Stillinger-Weber parameters for various elements and mixtures
# multiple entries can be added to this file, LAMMPS reads the ones it needs
# these entries are in LAMMPS "metal" units:
# epsilon = eV; sigma = Angstroms
# other quantities are unitless
# format of a single entry (one or more lines):
# element 1, element 2, element 3,
# epsilon, sigma, a, lambda, gamma, costheta0, A, B, p, q, tol
# Here are the original parameters in metal units, for Silicon from:
#
# Stillinger and Weber, Phys. Rev. B, v. 31, p. 5262, (1985)
#
Si Si Si 2.1683 2.0951 1.80 21.0 1.20 -0.333333333333
7.049556277 0.6022245584 4.0 0.0 0.0

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@ -0,0 +1,116 @@
# Simple regression tests for threebody potentials
# NOTE: These are not intended to represent real materials
units metal
atom_style atomic
atom_modify map array
boundary p p p
atom_modify sort 0 0.0
# temperature
variable t equal 1800.0
# cubic diamond unit cell
variable a equal 5.431
lattice custom $a &
a1 1.0 0.0 0.0 &
a2 0.0 1.0 0.0 &
a3 0.0 0.0 1.0 &
basis 0.0 0.0 0.0 &
basis 0.0 0.5 0.5 &
basis 0.5 0.0 0.5 &
basis 0.5 0.5 0.0 &
basis 0.25 0.25 0.25 &
basis 0.25 0.75 0.75 &
basis 0.75 0.25 0.75 &
basis 0.75 0.75 0.25
region myreg block 0 4 &
0 4 &
0 4
create_box 8 myreg
create_atoms 1 region myreg &
basis 1 1 &
basis 2 2 &
basis 3 3 &
basis 4 4 &
basis 5 5 &
basis 6 6 &
basis 7 7 &
basis 8 8
mass * 28.06
velocity all create $t 5287287 mom yes rot yes dist gaussian
# Equilibrate using Stillinger-Weber model for silicon
pair_style sw
pair_coeff * * Si.sw Si Si Si Si Si Si Si Si
thermo 10
fix 1 all nvt temp $t $t 0.1
fix_modify 1 energy yes
timestep 1.0e-3
neighbor 1.0 bin
neigh_modify every 1 delay 10 check yes
run 100
write_restart restart.equil
# Test Stillinger-Weber model for Cd/Te/Zn/Se/Hg/S
clear
read_restart restart.equil
pair_style sw
pair_coeff * * CdTeZnSeHgS0.sw Cd Zn Hg Cd Te S Se Te
thermo 10
fix 1 all nvt temp $t $t 0.1
fix_modify 1 energy yes
timestep 1.0e-3
neighbor 1.0 bin
neigh_modify every 1 delay 10 check yes
run 100
# Test Vashishta model for In/P
clear
read_restart restart.equil
pair_style vashishta
pair_coeff * * InP.vashishta In In In In P P P P
thermo 10
fix 1 all nvt temp $t $t 0.1
fix_modify 1 energy yes
timestep 1.0e-3
neighbor 1.0 bin
neigh_modify every 1 delay 10 check yes
run 100
# Test Tersoff model for B/N/C
clear
read_restart restart.equil
variable fac equal 0.6
change_box all x scale ${fac} y scale ${fac} z scale ${fac} remap
pair_style tersoff
pair_coeff * * BNC.tersoff N N N C B B C B
thermo 10
fix 1 all nvt temp $t $t 0.1
fix_modify 1 energy yes
timestep 1.0e-3
neighbor 1.0 bin
neigh_modify every 1 delay 10 check yes
run 100

View File

@ -18,9 +18,11 @@
# sqrt(lambda_ij*epsilon_ij*lambda_ik*epsilon_ik)/lambda_ik, and the
# results are directly entered in this table. Obviously, this
# conversion does not change the two-body parameters epsilon_ijj.
# All other ik pair parameters are entered on the i*k line, where *
# can be any species. This is consistent with the requirement of
# the ik parameter being on the ikk line.
# The twobody ik pair parameters are entered on the i*k lines, where *
# can be any species. This is consistent with the LAMMPS requirement
# that twobody ik parameters be defined on the ikk line. Entries on all
# the other i*k lines are ignored by LAMMPS
# These entries are in LAMMPS "metal" units: epsilon = eV;
# sigma = Angstroms; other quantities are unitless

View File

@ -1,9 +1,17 @@
### DATE: 2013-08-09 CONTRIBUTOR: X. W. Zhou, xzhou@sandia.gov, CITATION: Zhou, Ward, Martin, van Swol, Cruz-Campa, and D. Zubia, Phys. Rev. B, 88, 085309 (2013).
#
# Note that the way the parameters can be entered is not unique. As one way, we assume that eps_ijk is equal to eps_ik and lambda_ijk is equal to
# sqrt(lambda_ij*eps_ij*lambda_ik*eps_ik)/eps_ik, and all other parameters in the ijk line are for ik.
# Note that the way the parameters can be entered is not unique.
# As one way, we assume that eps_ijk is equal to eps_ik and
# lambda_ijk is equal to sqrt(lambda_ij*eps_ij*lambda_ik*eps_ik)/eps_ik,
# and all other parameters in the ijk line are for ik.
#
# The twobody ik pair parameters are entered on the i*k lines, where *
# can be any species. This is consistent with the LAMMPS requirement
# that twobody ik parameters be defined on the ikk line. Entries on all
# the other i*k lines are ignored by LAMMPS
#
# These entries are in LAMMPS "metal" units: epsilon = eV; sigma = Angstroms; other quantities are unitless;
# These entries are in LAMMPS "metal" units: epsilon = eV;
# sigma = Angstroms; other quantities are unitless
#
# cutoff distance = 4.632
# eps sigma a lambda gamma cos(theta) A B p q tol

2
src/.gitignore vendored
View File

@ -976,6 +976,8 @@
/fix_ttm_mod.h
/pair_born_coul_long_cs.cpp
/pair_born_coul_long_cs.h
/pair_born_coul_dsf_cs.cpp
/pair_born_coul_dsf_cs.h
/pair_buck_coul_long_cs.cpp
/pair_buck_coul_long_cs.h
/pair_coul_long_cs.cpp

View File

@ -38,7 +38,8 @@ enum{ROTATE,ALL};
/* ---------------------------------------------------------------------- */
ComputeTempAsphere::ComputeTempAsphere(LAMMPS *lmp, int narg, char **arg) :
Compute(lmp, narg, arg)
Compute(lmp, narg, arg),
id_bias(NULL), tbias(NULL), avec(NULL)
{
if (narg < 3) error->all(FLERR,"Illegal compute temp/asphere command");

View File

@ -297,8 +297,8 @@ void PairGayBerne::coeff(int narg, char **arg)
if (!allocated) allocate();
int ilo,ihi,jlo,jhi;
force->bounds(arg[0],atom->ntypes,ilo,ihi);
force->bounds(arg[1],atom->ntypes,jlo,jhi);
force->bounds(FLERR,arg[0],atom->ntypes,ilo,ihi);
force->bounds(FLERR,arg[1],atom->ntypes,jlo,jhi);
double epsilon_one = force->numeric(FLERR,arg[2]);
double sigma_one = force->numeric(FLERR,arg[3]);

View File

@ -371,8 +371,8 @@ void PairLineLJ::coeff(int narg, char **arg)
if (!allocated) allocate();
int ilo,ihi,jlo,jhi;
force->bounds(arg[0],atom->ntypes,ilo,ihi);
force->bounds(arg[1],atom->ntypes,jlo,jhi);
force->bounds(FLERR,arg[0],atom->ntypes,ilo,ihi);
force->bounds(FLERR,arg[1],atom->ntypes,jlo,jhi);
double size_itype = force->numeric(FLERR,arg[2]);
double size_jtype = force->numeric(FLERR,arg[3]);

View File

@ -269,8 +269,8 @@ void PairRESquared::coeff(int narg, char **arg)
if (!allocated) allocate();
int ilo,ihi,jlo,jhi;
force->bounds(arg[0],atom->ntypes,ilo,ihi);
force->bounds(arg[1],atom->ntypes,jlo,jhi);
force->bounds(FLERR,arg[0],atom->ntypes,ilo,ihi);
force->bounds(FLERR,arg[1],atom->ntypes,jlo,jhi);
double epsilon_one = force->numeric(FLERR,arg[2]);
double sigma_one = force->numeric(FLERR,arg[3]);

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@ -442,8 +442,8 @@ void PairTriLJ::coeff(int narg, char **arg)
if (!allocated) allocate();
int ilo,ihi,jlo,jhi;
force->bounds(arg[0],atom->ntypes,ilo,ihi);
force->bounds(arg[1],atom->ntypes,jlo,jhi);
force->bounds(FLERR,arg[0],atom->ntypes,ilo,ihi);
force->bounds(FLERR,arg[1],atom->ntypes,jlo,jhi);
double epsilon_one = force->numeric(FLERR,arg[2]);
double sigma_one = force->numeric(FLERR,arg[3]);

View File

@ -28,7 +28,7 @@ enum{SPHERE,LINE,TRI}; // also in DumpImage
/* ---------------------------------------------------------------------- */
BodyNparticle::BodyNparticle(LAMMPS *lmp, int narg, char **arg) :
Body(lmp, narg, arg)
Body(lmp, narg, arg), imflag(NULL), imdata(NULL)
{
if (narg != 3) error->all(FLERR,"Invalid body nparticle command");

View File

@ -33,7 +33,7 @@ enum{ID,TYPE,INDEX};
/* ---------------------------------------------------------------------- */
ComputeBodyLocal::ComputeBodyLocal(LAMMPS *lmp, int narg, char **arg) :
Compute(lmp, narg, arg)
Compute(lmp, narg, arg), which(NULL), index(NULL), avec(NULL), bptr(NULL)
{
if (narg < 4) error->all(FLERR,"Illegal compute body/local command");

View File

@ -37,7 +37,7 @@ enum{ROTATE,ALL};
/* ---------------------------------------------------------------------- */
ComputeTempBody::ComputeTempBody(LAMMPS *lmp, int narg, char **arg) :
Compute(lmp, narg, arg)
Compute(lmp, narg, arg), id_bias(NULL), tbias(NULL), avec(NULL)
{
if (narg < 3) error->all(FLERR,"Illegal compute temp/body command");

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@ -388,8 +388,8 @@ void PairBody::coeff(int narg, char **arg)
if (!allocated) allocate();
int ilo,ihi,jlo,jhi;
force->bounds(arg[0],atom->ntypes,ilo,ihi);
force->bounds(arg[1],atom->ntypes,jlo,jhi);
force->bounds(FLERR,arg[0],atom->ntypes,ilo,ihi);
force->bounds(FLERR,arg[1],atom->ntypes,jlo,jhi);
double epsilon_one = force->numeric(FLERR,arg[2]);
double sigma_one = force->numeric(FLERR,arg[3]);

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@ -271,7 +271,7 @@ void AngleClass2::coeff(int narg, char **arg)
if (!allocated) allocate();
int ilo,ihi;
force->bounds(arg[0],atom->nangletypes,ilo,ihi);
force->bounds(FLERR,arg[0],atom->nangletypes,ilo,ihi);
int count = 0;

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@ -132,7 +132,7 @@ void BondClass2::coeff(int narg, char **arg)
if (!allocated) allocate();
int ilo,ihi;
force->bounds(arg[0],atom->nbondtypes,ilo,ihi);
force->bounds(FLERR,arg[0],atom->nbondtypes,ilo,ihi);
double r0_one = force->numeric(FLERR,arg[1]);
double k2_one = force->numeric(FLERR,arg[2]);

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@ -640,7 +640,7 @@ void DihedralClass2::coeff(int narg, char **arg)
if (!allocated) allocate();
int ilo,ihi;
force->bounds(arg[0],atom->ndihedraltypes,ilo,ihi);
force->bounds(FLERR,arg[0],atom->ndihedraltypes,ilo,ihi);
int count = 0;

View File

@ -529,7 +529,7 @@ void ImproperClass2::coeff(int narg, char **arg)
if (!allocated) allocate();
int ilo,ihi;
force->bounds(arg[0],atom->nimpropertypes,ilo,ihi);
force->bounds(FLERR,arg[0],atom->nimpropertypes,ilo,ihi);
int count = 0;

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@ -189,8 +189,8 @@ void PairLJClass2::coeff(int narg, char **arg)
if (!allocated) allocate();
int ilo,ihi,jlo,jhi;
force->bounds(arg[0],atom->ntypes,ilo,ihi);
force->bounds(arg[1],atom->ntypes,jlo,jhi);
force->bounds(FLERR,arg[0],atom->ntypes,ilo,ihi);
force->bounds(FLERR,arg[1],atom->ntypes,jlo,jhi);
double epsilon_one = force->numeric(FLERR,arg[2]);
double sigma_one = force->numeric(FLERR,arg[3]);

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