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<li><a class="reference internal" href="#">pair_style lj/cubic command</a></li>
<li><a class="reference internal" href="#pair-style-lj-cubic-gpu-command">pair_style lj/cubic/gpu command</a></li>
<li><a class="reference internal" href="#pair-style-lj-cubic-omp-command">pair_style lj/cubic/omp command</a><ul>
<li><a class="reference internal" href="#syntax">Syntax</a></li>
<li><a class="reference internal" href="#examples">Examples</a></li>
<li><a class="reference internal" href="#description">Description</a></li>
<li><a class="reference internal" href="#restrictions">Restrictions</a></li>
<li><a class="reference internal" href="#related-commands">Related commands</a></li>
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<div class="section" id="pair-style-lj-cubic-command">
<span id="index-0"></span><h1>pair_style lj/cubic command</h1>
</div>
<div class="section" id="pair-style-lj-cubic-gpu-command">
<h1>pair_style lj/cubic/gpu command</h1>
</div>
<div class="section" id="pair-style-lj-cubic-omp-command">
<h1>pair_style lj/cubic/omp command</h1>
<div class="section" id="syntax">
<h2>Syntax</h2>
<div class="highlight-default"><div class="highlight"><pre><span></span><span class="n">pair_style</span> <span class="n">lj</span><span class="o">/</span><span class="n">cubic</span>
</pre></div>
</div>
</div>
<div class="section" id="examples">
<h2>Examples</h2>
<div class="highlight-default"><div class="highlight"><pre><span></span><span class="n">pair_style</span> <span class="n">lj</span><span class="o">/</span><span class="n">cubic</span>
<span class="n">pair_coeff</span> <span class="o">*</span> <span class="o">*</span> <span class="mf">1.0</span> <span class="mf">0.8908987</span>
</pre></div>
</div>
</div>
<div class="section" id="description">
<h2>Description</h2>
<p>The <em>lj/cubic</em> style computes a truncated LJ interaction potential
whose energy and force are continuous everywhere. Inside the
inflection point the interaction is identical to the standard 12/6
<a class="reference internal" href="pair_lj.html"><span class="doc">Lennard-Jones</span></a> potential. The LJ function outside the
inflection point is replaced with a cubic function of distance. The
energy, force, and second derivative are continuous at the inflection
point. The cubic coefficient A3 is chosen so that both energy and
force go to zero at the cutoff distance. Outside the cutoff distance
the energy and force are zero.</p>
<img alt="_images/pair_lj_cubic.jpg" class="align-center" src="_images/pair_lj_cubic.jpg" />
<p>The location of the inflection point rs is defined
by the LJ diameter, rs/sigma = (26/7)^1/6. The cutoff distance
is defined by rc/rs = 67/48 or rc/sigma = 1.737....
The analytic expression for the
the cubic coefficient
A3*rmin^3/epsilon = 27.93... is given in the paper by
Holian and Ravelo <a class="reference internal" href="#holian"><span class="std std-ref">(Holian)</span></a>.</p>
<p>This potential is commonly used to study the shock mechanics of FCC
solids, as in Ravelo et al. <a class="reference internal" href="#ravelo"><span class="std std-ref">(Ravelo)</span></a>.</p>
<p>The following coefficients must be defined for each pair of atom types
via the <a class="reference internal" href="pair_coeff.html"><span class="doc">pair_coeff</span></a> command as in the example above,
or in the data file or restart files read by the
<a class="reference internal" href="read_data.html"><span class="doc">read_data</span></a> or <a class="reference internal" href="read_restart.html"><span class="doc">read_restart</span></a>
commands, or by mixing as described below:</p>
<ul class="simple">
<li>epsilon (energy units)</li>
<li>sigma (distance units)</li>
</ul>
<p>Note that sigma is defined in the LJ formula as the zero-crossing
distance for the potential, not as the energy minimum, which is
located at rmin = 2^(1/6)*sigma. In the above example, sigma =
0.8908987, so rmin = 1.</p>
<hr class="docutils" />
<p>Styles with a <em>gpu</em>, <em>intel</em>, <em>kk</em>, <em>omp</em>, or <em>opt</em> 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 <a class="reference internal" href="Section_accelerate.html"><span class="doc">Section_accelerate</span></a>
of the manual. The accelerated styles take the same arguments and
should produce the same results, except for round-off and precision
issues.</p>
<p>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 <span class="xref std std-ref">Making LAMMPS</span> section for more info.</p>
<p>You can specify the accelerated styles explicitly in your input script
by including their suffix, or you can use the <span class="xref std std-ref">-suffix command-line switch</span> when you invoke LAMMPS, or you can
use the <a class="reference internal" href="suffix.html"><span class="doc">suffix</span></a> command in your input script.</p>
<p>See <a class="reference internal" href="Section_accelerate.html"><span class="doc">Section_accelerate</span></a> of the manual for
more instructions on how to use the accelerated styles effectively.</p>
<hr class="docutils" />
<p><strong>Mixing, shift, table, tail correction, restart, rRESPA info</strong>:</p>
<p>For atom type pairs I,J and I != J, the epsilon and sigma coefficients
and cutoff distance for all of the lj/cut pair styles can be mixed.
The default mix value is <em>geometric</em>. See the &#8220;pair_modify&#8221; command
for details.</p>
<p>The lj/cubic pair style does not support the
<a class="reference internal" href="pair_modify.html"><span class="doc">pair_modify</span></a> shift option,
since pair interaction is already smoothed to 0.0 at the
cutoff.</p>
<p>The <a class="reference internal" href="pair_modify.html"><span class="doc">pair_modify</span></a> table option is not relevant
for this pair style.</p>
<p>The lj/cubic pair style does not support the
<a class="reference internal" href="pair_modify.html"><span class="doc">pair_modify</span></a> tail option for adding long-range tail
corrections to energy and pressure, since there are no corrections for
a potential that goes to 0.0 at the cutoff.</p>
<p>The lj/cubic pair style writes its information to <a class="reference internal" href="restart.html"><span class="doc">binary restart files</span></a>, so pair_style and pair_coeff commands do
not need to be specified in an input script that reads a restart file.</p>
<p>The lj/cubic pair style can only be used via the <em>pair</em>
keyword of the <a class="reference internal" href="run_style.html"><span class="doc">run_style respa</span></a> command. It does not
support the <em>inner</em>, <em>middle</em>, <em>outer</em> keywords.</p>
</div>
<hr class="docutils" />
<div class="section" id="restrictions">
<h2>Restrictions</h2>
<blockquote>
<div>none</div></blockquote>
</div>
<div class="section" id="related-commands">
<h2>Related commands</h2>
<p><a class="reference internal" href="pair_coeff.html"><span class="doc">pair_coeff</span></a></p>
<p><strong>Default:</strong> none</p>
<hr class="docutils" />
<p id="ravelo"><span id="holian"></span><strong>(Holian)</strong> Holian and Ravelo, Phys Rev B, 51, 11275 (1995).</p>
<p><strong>(Ravelo)</strong> Ravelo, Holian, Germann and Lomdahl, Phys Rev B, 70, 014103 (2004).</p>
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