diff --git a/Doc/UserManual/Assemblies.tex b/Doc/UserManual/Assemblies.tex index 12587e15d9367cc82827597caee366eb1bf7f194..8dab0c182696a3a571cc8c1f8ac6d17e7310640e 100644 --- a/Doc/UserManual/Assemblies.tex +++ b/Doc/UserManual/Assemblies.tex @@ -287,7 +287,7 @@ integral equals the square of the number of particles that contribute to the sca \end{equation} with $N_p$ the number of scattering centers. \nomenclature{$N_p$}{Number of scattering centers} - + In the following, we will present different physical models that provide computable approximations @@ -451,9 +451,7 @@ They are available through constructors like \begin{lstlisting} FormFactorCone(radius, height, alpha) \end{lstlisting} -These functions are documented in Appendix~\ref{SFF}. -Some background information on how the form factors are computed -is given in Appendix~\ref{SFFcomp}. +These functions are documented in \cref{SFF}. \index{Form factor!tutorial}% \index{Form factor!examples}% @@ -900,7 +898,7 @@ S(q) =\Re \left(\frac{1+\Phi(q) }{1 - \Phi(q)} \right), \quad \mathrm{where}\qua \end{align*} where $\Lambda$ is a damping length used in order to introduce some finite-size effects. -Figure~\ref{fig:1dparas_q} shows the evolution of $S(q)$ for different values of $\omega /D$. +\Cref{fig:1dparas_q} shows the evolution of $S(q)$ for different values of $\omega /D$. \begin{figure}[tb] \begin{center} @@ -1042,7 +1040,7 @@ where $q_{\plll}$ is the component of the scattering beam in the plane of the in \vspace{18pt} -Figure~\ref{fig:SchemDWBA} illustrates the four scattering processes for a supported particle, taken into account in the DWBA. The first term of eq.~\ref{Edwbaair} corresponds to the Born approximation. Each term of $F_{\rm{DWBA}}$ is weighted by a Fresnel coefficient. +\Cref{fig:SchemDWBA} illustrates the four scattering processes for a supported particle, taken into account in the DWBA. The first term of eq.~\ref{Edwbaair} corresponds to the Born approximation. Each term of $F_{\rm{DWBA}}$ is weighted by a Fresnel coefficient. \begin{figure}[tb] \begin{center} @@ -1061,7 +1059,7 @@ Script~\ref{lst:badwba} illustrates the difference between BA and DWBA in \BornA \item in the BA, a sample composed of the particles in air. \end{itemize} -Figure~\ref{fig:spheroidbadwba} shows the intensity contour plot generated using this script with truncated spheroids as particles. +\Cref{fig:spheroidbadwba} shows the intensity contour plot generated using this script with truncated spheroids as particles. \newpage @@ -1145,7 +1143,7 @@ where index $n$ is related to the layers, $z$ to the vertical component, and $j$ \end{figure} -Figure~\ref{fig:dwbaburied} shows a typical example of the output intensity scattered from a sample made of 3 layers: air, substrate, and in between, spherical particles embedded in the middle of a 30~nm-thick layer. This figure had been generated using listing~\ref{lst:dwbaburied}. +\Cref{fig:dwbaburied} shows a typical example of the output intensity scattered from a sample made of 3 layers: air, substrate, and in between, spherical particles embedded in the middle of a 30~nm-thick layer. This figure had been generated using listing~\ref{lst:dwbaburied}. \begin{lstlisting}[language=python, style=eclipseboxed,numbers=none,nolol,caption={\Code{Python} script to generate a sample where spherical particles are embedded in the middle of a layer on a substrate.},label={lst:dwbaburied}] def get_sample(): @@ -1309,7 +1307,7 @@ The interference function is specified when building the sample. It is linked wi The particles are placed randomly in the dilute limit and are considered as individual, non-interacting scatterers. The scattered intensity is function of the form factors only. -\paragraph{Example} The sample is made of a substrate on which are deposited half-spheres. Script~\ref{lst:nointerf} details the commands necessary to generate such a sample. Figure~\ref{fig:nointerf} shows an example of output intensity: Script~\ref{lst:nointerf} + detector's + input beam's characterizations. +\paragraph{Example} The sample is made of a substrate on which are deposited half-spheres. Script~\ref{lst:nointerf} details the commands necessary to generate such a sample. \Cref{fig:nointerf} shows an example of output intensity: Script~\ref{lst:nointerf} + detector's + input beam's characterizations. \begin{figure}[tb]