<dt><b>tinit: (0) [ps]</b></dt>
<dd>starting time for your run (only makes sense for integrators <tt>md</tt>,
<tt>sd</tt> and <tt>bd</tt>)</dd>
-<dt><b>dt: (0.001) [ps]</b></dd>
+<dt><b>dt: (0.001) [ps]</b></dt></dd>
<dd>time step for integration (only makes sense for integrators <tt>md</tt>,
<tt>sd</tt> and <tt>bd</tt>)</dd>
<dt><b>nsteps: (0)</b></dt>
<dt><b>Cut-off</b></dt>
<dd>Twin range cut-off's with neighborlist cut-off <b>rlist</b> and
Coulomb cut-off <b>rcoulomb</b>,
-where <b>rcoulomb</b> &ge <b>rlist</b>.
+where <b>rcoulomb</b>≥<b>rlist</b>.
<dt><b>Ewald</b></dt>
<dd>Classical <!--Idx-->Ewald sum<!--EIdx--> electrostatics.
FFTs. Grid dimensions are controlled with <b>fourierspacing</b> and the
interpolation order with <b>pme_order</b>. With a grid spacing of 0.1
nm and cubic interpolation the electrostatic forces have an accuracy
-of 2-3e-4. Since the error from the vdw-cutoff is larger than this you
+of 2-3*10<sup>-4</sup>. Since the error from the vdw-cutoff is larger than this you
might try 0.15 nm. When running in parallel the interpolation
parallelizes better than the FFT, so try decreasing grid dimensions
while increasing interpolation.</dd>
For normal runs a single step is sufficient, but for NVE
runs where you want to conserve energy accurately or for accurate
energy minimization you might want to increase it to 2.
-<dt><b>lincs_warnangle: </b>(30) [degrees]</b></dt>
+<dt><b>lincs_warnangle: </b>(30) [degrees]</dt>
<dd>maximum angle that a bond can rotate before LINCS will complain</dd>
<dt><b>morse:</b></dt>
of (0,0,0) is used. With an absolute reference the system is no longer
translation invariant and one should think about what to do with
the <A HREF="#run">center of mass motion</A>.</dd>
-</b>
<dt><b>pull_weights0: </b></dt>
<dd>see <b>pull_weights1</b></dd>
<dt><b>pull_pbcatom0: (0)</b></dt>
<dd>see <b>pull_pbcatom1</b></dd>
<dt><b>pull_group1: </b></dt>
-<dd>The name of the pull group.</b>
+<dd>The name of the pull group.</dd>
<dt><b>pull_weights1: </b></dt>
<dd>Optional relative weights which are multiplied with the masses of the atoms
to give the total weight for the COM. The number should be 0, meaning all 1,