diff --git a/doc/html/_sources/compute_hexorder_atom.txt b/doc/html/_sources/compute_hexorder_atom.txt index efe3e1a78f..acc219a34d 100644 --- a/doc/html/_sources/compute_hexorder_atom.txt +++ b/doc/html/_sources/compute_hexorder_atom.txt @@ -70,7 +70,7 @@ In an isotropic liquid, local neighborhoods may still exhibit weak hexagonal symmetry, but because the orientational correlation decays quickly with distance, the value of phi will be different for different atoms, and so when *q*\ 6 is averaged over all the atoms -in the system, |<\ *q*\ 6>| << 1. +in the system, \|<\ *q*\ 6>\| << 1. The value of *qn* is set to zero for atoms not in the specified compute group, as well as for atoms that have less than diff --git a/doc/html/compute_hexorder_atom.html b/doc/html/compute_hexorder_atom.html index 8310ca14e2..7f7ef8f450 100644 --- a/doc/html/compute_hexorder_atom.html +++ b/doc/html/compute_hexorder_atom.html @@ -183,7 +183,7 @@ In an isotropic liquid, local neighborhoods may still exhibit weak hexagonal symmetry, but because the orientational correlation decays quickly with distance, the value of phi will be different for different atoms, and so when q6 is averaged over all the atoms -in the system, |<\ *q*\ 6>| << 1.

+in the system, |<q6>| << 1.

The value of qn is set to zero for atoms not in the specified compute group, as well as for atoms that have less than nnn neighbors within the distance cutoff.