diff --git a/Doc/UserManual/Assemblies.tex b/Doc/UserManual/Assemblies.tex
index 48998324e0c834cfbea8c8985ad9d88e307b0d84..fa96f2e81070f3541c21e42b6f6f25b3180f6098 100644
--- a/Doc/UserManual/Assemblies.tex
+++ b/Doc/UserManual/Assemblies.tex
@@ -815,7 +815,7 @@ we present particle assembly models that are supported in \BornAgain.
 %\index{Particles!intersecting layer boundaries}}
 
 The nanoparticles are characterized by their form factors
-(\idest the Fourier transform of the shape function - see \cref{app:ff} for a list of form factors implemented in \BornAgain) and the composing material.
+(\cref{SFF}) and the composing material.
 
 
 \Note{\indent
@@ -941,9 +941,8 @@ where $\Lambda$ is a damping length used in order to introduce some finite-size
 \label{fig:1dparas_q}
 \end{figure}
 
-In two dimensions, the paracrystal is constructed on a pseudo-regular lattice with base vectors $\v{a}$ and $\v{b}$ using the following conditions for the densities of probabilities:
-
-$\int p_{\v{a}}(\r)d^2r=\int p_{\v{b}}(\r)\d^2r=1$,
+In two dimensions, the paracrystal is constructed on a pseudo-regular lattice with base vectors $\v{a}$ and $\v{b}$ using the following conditions for the densities of probabilities:\\
+$\int p_{\v{a}}(\r)\d^2r=\int p_{\v{b}}(\r)\d^2r=1$,
 $\int \r p_{\v{a}}(\r)\d^2r=\v{a}$,
 $\int \r p_{\v{b}}(\r)\d^2r=\v{b}$.
 
@@ -1498,7 +1497,7 @@ where ($L_1$, $L_2$, $\alpha$, $\xi$) are shown in \cref{fig:2dlattice} with
 \begin{itemize}
 \item[]$L_1$, $L_2$ the lengths of the lattice cell,
 \item[]$\alpha$ the angle between the lattice basis vectors $\v{a}, \v{b}$ in direct space,
-\item[] $\xi$ is the angle defining the lattice orientation (set to $0$ by default); it is taken as the angle between the $\v{a}$ vector of the lattice basis and the $\v{x}$ axis of the reference Cartesian frame (as shown in \cref{fig:multil3d}).
+\item[] $\xi$ is the angle defining the lattice orientation (set to $0$ by default); it is taken as the angle between the $\v{a}$ vector of the lattice basis and the $\v{x}$ axis of the reference Cartesian frame (as shown in \cref{fig:2dlattice}).
 \end{itemize}
 
 \begin{figure}[tb]
diff --git a/Doc/UserManual/Macros.tex b/Doc/UserManual/Macros.tex
index 4e520068feb148ee2dc95d1a1979caf1285634c6..66cfc1b097c7ec305f94c9f60b6a74aa70414427 100644
--- a/Doc/UserManual/Macros.tex
+++ b/Doc/UserManual/Macros.tex
@@ -81,4 +81,4 @@
 %	HYPHENATION
 %-------------------------------------------------------------------------------
 
-\hyphenation{ MacOS Schrö-ding-er nano-par-ti-cle nano-par-ti-cles }
+\hyphenation{ MacOS Schrö-ding-er nano-par-ti-cle nano-par-ti-cles para-crys-tal }
diff --git a/Doc/UserManual/Usage.tex b/Doc/UserManual/Usage.tex
index d83da4839cae7a1f462c36f794f737e8e9c1fc26..b0808f032849b2a21de9ac8826dc311103bbe39e 100644
--- a/Doc/UserManual/Usage.tex
+++ b/Doc/UserManual/Usage.tex
@@ -130,7 +130,7 @@ We implement two different shapes of particles: cylinders and
 prisms (\idest  elongated particles with a constant equilateral triangular cross section).
 
 All particles implemented in \BornAgain\ are defined by their
-form factors (see \cref{app:ff}), their sizes and the material
+form factors (see \cref{SFF}), their sizes and the material
 they are made of. Here, for the
 cylindrical particle, we input its radius and height.  For the prism,
 the possible inputs are the length of one side of its equilateral triangular
@@ -237,9 +237,8 @@ The first stage is to create the \Code{Simulation()} object (line~\ref{run2}). T
 parameters (line~\ref{runbeam}). %, which are associated with the
 %sample previously defined (line~\ref{runsample}). Finally we run
 %the simulation (line~\ref{runsimul}).
-Those functions are part of the Simulation
-class.  The different incident and exit angles are
-shown in \cref{fig:multil3d}.
+Those functions are part of the Simulation class.
+The different incident and exit angles are shown in \cref{fig:multil3d}.
 
 The detector parameters are set using ranges of angles via
 the function: