From 03cb7870255e86f2bb801b6553258ec9e70cc79f Mon Sep 17 00:00:00 2001
From: sjplimp <sjplimp@f3b2605a-c512-4ea7-a41b-209d697bcdaa>
Date: Tue, 10 May 2016 14:39:05 +0000
Subject: [PATCH] git-svn-id: svn://svn.icms.temple.edu/lammps-ro/trunk@14983
 f3b2605a-c512-4ea7-a41b-209d697bcdaa

---
 doc/html/fix_pimd.html | 4 ++--
 1 file changed, 2 insertions(+), 2 deletions(-)

diff --git a/doc/html/fix_pimd.html b/doc/html/fix_pimd.html
index 9fd1a77fa6..57ee90e294 100644
--- a/doc/html/fix_pimd.html
+++ b/doc/html/fix_pimd.html
@@ -171,7 +171,7 @@ index (the second term in the effective potential above).  The
 quasi-beads also interact with the two neighboring quasi-beads through
 the spring potential in imaginary-time space (first term in effective
 potential).  To sample the canonical ensemble, a Nose-Hoover massive
-chain thermostat is applied <a class="reference internal" href="run_style.html#tuckerman"><span class="std std-ref">(Tuckerman)</span></a>.  With the
+chain thermostat is applied <a class="reference internal" href="#pimd-tuckerman"><span class="std std-ref">(Tuckerman)</span></a>.  With the
 massive chain algorithm, a chain of NH thermostats is coupled to each
 degree of freedom for each quasi-bead.  The keyword <em>temp</em> sets the
 target temperature for the system and the keyword <em>nhc</em> sets the
@@ -271,7 +271,7 @@ and nhc = 2.</p>
 <hr class="docutils" />
 <p id="feynman"><strong>(Feynman)</strong> R. Feynman and A. Hibbs, Chapter 7, Quantum Mechanics and
 Path Integrals, McGraw-Hill, New York (1965).</p>
-<p id="tuckerman"><strong>(Tuckerman)</strong> M. Tuckerman and B. Berne, J Chem Phys, 99, 2796 (1993).</p>
+<p id="pimd-tuckerman"><strong>(Tuckerman)</strong> M. Tuckerman and B. Berne, J Chem Phys, 99, 2796 (1993).</p>
 <p id="cao1"><strong>(Cao1)</strong> J. Cao and B. Berne, J Chem Phys, 99, 2902 (1993).</p>
 <p id="cao2"><strong>(Cao2)</strong> J. Cao and G. Voth, J Chem Phys, 100, 5093 (1994).</p>
 <p id="hone"><strong>(Hone)</strong> T. Hone, P. Rossky, G. Voth, J Chem Phys, 124,