git-svn-id: svn://svn.icms.temple.edu/lammps-ro/trunk@13544 f3b2605a-c512-4ea7-a41b-209d697bcdaa
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@ -59,9 +59,10 @@ Per-atom masses are defined in the data file read by the
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set to new values by the <A HREF = "set.html">set mass</A> or <A HREF = "set.html">set density</A>
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commands.
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</P>
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<P>Also note that <A HREF = "pair_eam.html">pair_style eam</A> defines the masses of
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atom types in the EAM potential file, in which case the mass command
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is normally not used.
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<P>Also note that <A HREF = "pair_eam.html">pair_style eam</A> and <A HREF = "pair_bop.html">pair_style
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bop</A> commands define the masses of atom types in their
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respective potential files, in which case the mass command is normally
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not used.
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</P>
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<P>If you define a <A HREF = "atom_style.html">hybrid atom style</A> which includes one
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(or more) sub-styles which require per-type mass and one (or more)
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@ -56,9 +56,10 @@ Per-atom masses are defined in the data file read by the
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set to new values by the "set mass"_set.html or "set density"_set.html
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commands.
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Also note that "pair_style eam"_pair_eam.html defines the masses of
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atom types in the EAM potential file, in which case the mass command
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is normally not used.
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Also note that "pair_style eam"_pair_eam.html and "pair_style
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bop"_pair_bop.html commands define the masses of atom types in their
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respective potential files, in which case the mass command is normally
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not used.
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If you define a "hybrid atom style"_atom_style.html which includes one
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(or more) sub-styles which require per-type mass and one (or more)
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@ -27,7 +27,7 @@
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</P>
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<PRE>pair_style bop
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pair_coeff * * ../potentials/CdTe_bop Cd Te
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pair_style bop 4.90 save
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pair_style bop save
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pair_coeff * * ../potentials/CdTe.bop.table Cd Te Te
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comm_modify cutoff 14.70
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</PRE>
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@ -85,8 +85,18 @@ to either stabilize or destabilize close-packed structures. The pi
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bond-order includes hopping paths of length 4. This enables the
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incorporation of dihedral angles effects.
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</P>
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<P>One option can be specified as a keyword with the
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pair_style command.
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<P>IMPORTANT NOTE: Note that unlike for other potentials, cutoffs for BOP
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potentials are not set in the pair_style or pair_coeff command; they
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are specified in the BOP potential files themselves. Likewise, the
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BOP potential files list atomic masses; thus you do not need to use
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the <A HREF = "mass.html">mass</A> command to specify them. Note that for BOP
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potentials with hydrogen, you will likely want to set the mass of H
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atoms to be 10x or 20x larger to avoid having to use a tiny timestep.
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You can do this by using the <A HREF = "mass.html">mass</A> command after using the
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<A HREF = "doc/pair_coeff.html">pair_coeff</A> command to read the BOP potential
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file.
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</P>
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<P>One option can be specified as a keyword with the pair_style command.
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</P>
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<P>The <I>save</I> keyword gives you the option to calculate in advance and
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store a set of distances, angles, and derivatives of angles. The
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@ -296,11 +306,14 @@ the previous section but is interaction type dependent)
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<P>The next section contains a line for each three body interaction type
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e_j-e_i-e_k with i=0->N, j=0->N, k=j->N
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</P>
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<LI>Line 1: g0, g1, g2... (These are coefficients for
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the angular spline of the g_(sigma,jik)(THETA_ijk) for e_1-e_1-e_1 interaction.
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The function can contain up to 10 term thus 10 constants. The first line
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can contain up to five constants. If the spline has more than five terms
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the second g0, g1, g2 (for e_1-e_1-e_2)
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<LI>Line 1: g0, g1, g2... (These are coefficients for the angular spline
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of the g_(sigma,jik)(THETA_ijk) for e_1-e_1-e_1 interaction. The
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function can contain up to 10 term thus 10 constants. The first line
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can contain up to five constants. If the spline has more than five
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terms the second line will contain the remaining constants The
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following lines will then contain the constants for the remainaing g0,
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g1, g2... (for e_1-e_1-e_2) and the other three body
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interactions
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</UL>
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<P>The rest of the table has the same structure as the previous section
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(see above).
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@ -21,7 +21,7 @@ keyword = {save} :l
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pair_style bop
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pair_coeff * * ../potentials/CdTe_bop Cd Te
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pair_style bop 4.90 save
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pair_style bop save
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pair_coeff * * ../potentials/CdTe.bop.table Cd Te Te
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comm_modify cutoff 14.70 :pre
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@ -79,8 +79,18 @@ to either stabilize or destabilize close-packed structures. The pi
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bond-order includes hopping paths of length 4. This enables the
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incorporation of dihedral angles effects.
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One option can be specified as a keyword with the
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pair_style command.
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IMPORTANT NOTE: Note that unlike for other potentials, cutoffs for BOP
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potentials are not set in the pair_style or pair_coeff command; they
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are specified in the BOP potential files themselves. Likewise, the
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BOP potential files list atomic masses; thus you do not need to use
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the "mass"_mass.html command to specify them. Note that for BOP
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potentials with hydrogen, you will likely want to set the mass of H
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atoms to be 10x or 20x larger to avoid having to use a tiny timestep.
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You can do this by using the "mass"_mass.html command after using the
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"pair_coeff"_doc/pair_coeff.html command to read the BOP potential
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file.
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One option can be specified as a keyword with the pair_style command.
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The {save} keyword gives you the option to calculate in advance and
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store a set of distances, angles, and derivatives of angles. The
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@ -268,11 +278,14 @@ the previous section but is interaction type dependent) :l,ule
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The next section contains a line for each three body interaction type
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e_j-e_i-e_k with i=0->N, j=0->N, k=j->N
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Line 1: g0, g1, g2... (These are coefficients for
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the angular spline of the g_(sigma,jik)(THETA_ijk) for e_1-e_1-e_1 interaction.
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The function can contain up to 10 term thus 10 constants. The first line
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can contain up to five constants. If the spline has more than five terms
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the second g0, g1, g2 (for e_1-e_1-e_2) :l,ule
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Line 1: g0, g1, g2... (These are coefficients for the angular spline
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of the g_(sigma,jik)(THETA_ijk) for e_1-e_1-e_1 interaction. The
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function can contain up to 10 term thus 10 constants. The first line
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can contain up to five constants. If the spline has more than five
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terms the second line will contain the remaining constants The
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following lines will then contain the constants for the remainaing g0,
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g1, g2... (for e_1-e_1-e_2) and the other three body
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interactions :l,ule
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The rest of the table has the same structure as the previous section
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(see above).
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