diff --git a/Doc/pages/analysis.rst b/Doc/pages/analysis.rst
index 15e61d8bd..98bf553fc 100644
--- a/Doc/pages/analysis.rst
+++ b/Doc/pages/analysis.rst
@@ -121,19 +121,13 @@ Box Translated Trajectory
 
 Center Of Masses Trajectory
 '''''''''''''''''''''''''''
-.. note::
-
-    **This job is under development MDANSE and is currently not available.
-    The documentation here is out-dated and only left here for referencing
-    purposes.**
-
-    The center of mass trajectory (COMT) analysis consists in deriving the
-    trajectory of the respective centres of mass of a set of groups of
-    atoms. In order to produce a visualizable trajectory, MDANSE assigns
-    the centres of mass to pseudo-hydrogen atoms whose mass is equal to the
-    mass of their associated group. Thus, the produced trajectory can be
-    reused for other analysis. In that sense, COMT analysis is a practical
-    way to reduce noticeably the dimensionality of a system.
+The center of mass trajectory (COMT) analysis consists in deriving the
+trajectory of the respective centres of mass of a set of groups of
+atoms. In order to produce a visualizable trajectory, MDANSE assigns
+the centres of mass to pseudo-hydrogen atoms whose mass is equal to the
+mass of their associated group. Thus, the produced trajectory can be
+reused for other analysis. In that sense, COMT analysis is a practical
+way to reduce noticeably the dimensionality of a system.
 
 .. _cropped-trajectory:
 
diff --git a/Doc/pages/scattering.rst b/Doc/pages/scattering.rst
index df1d4765d..6bc81f6bc 100644
--- a/Doc/pages/scattering.rst
+++ b/Doc/pages/scattering.rst
@@ -776,12 +776,18 @@ Naturally, similar expressions apply to the dynamic structure factors,
 
 Structure Factor From Scattering Function
 '''''''''''''''''''''''''''''''''''''''''
-The structure factor from scattering function is a concept used in
-scientific research, particularly in the field of neutron scattering
-experiments. It relates to how particles or atoms within a material
-contribute to its overall structural properties based on their scattering
-behavior. This concept provides valuable insights into the material's
-internal structure, dynamics, and interactions. Researchers use the Structure
-Factor From Scattering Function to better understand the atomic-level details
-of materials, which has applications in diverse areas, including materials
-science and condensed matter physics
+.. note::
+
+    **This job is under development and may change in future versions
+    of MDANSE. The documentation here is out-dated and only left here
+    for referencing purposes.**
+
+    The structure factor from scattering function is a concept used in
+    scientific research, particularly in the field of neutron scattering
+    experiments. It relates to how particles or atoms within a material
+    contribute to its overall structural properties based on their scattering
+    behavior. This concept provides valuable insights into the material's
+    internal structure, dynamics, and interactions. Researchers use the Structure
+    Factor From Scattering Function to better understand the atomic-level details
+    of materials, which has applications in diverse areas, including materials
+    science and condensed matter physics
diff --git a/Doc/pages/weights.rst b/Doc/pages/weights.rst
index 51d337739..d9b245ed7 100644
--- a/Doc/pages/weights.rst
+++ b/Doc/pages/weights.rst
@@ -154,13 +154,13 @@ Double Atom-Type Properties (Other)
 
 For calculation other than the DCSF and current correlation function (CCF)
 a slightly different weight scheme must be used as their partials are
-normalized slightly differently. In MDANSE the (weighted) partial static structure
+normalized slightly differently. In MDANSE the partial static structure
 factor (SSF) is
 
 .. math::
     :label: ws14
 
-    S_{\alpha\beta}(q) = W_{\alpha\beta} \left[ 1 + \frac{4 \pi \rho}{q} \int\limits_{0}^{\infty} \mathrm{d}r  \, \left[ g_{\alpha\beta}(r) - 1\right] r\sin(qr)\right]
+    S_{\alpha\beta}(q) = 1 + \frac{4 \pi \rho}{q} \int\limits_{0}^{\infty} \mathrm{d}r  \, \left[ g_{\alpha\beta}(r) - 1\right] r\sin(qr)
 
 where