Update for the new hugo website

paper/submission/TUIO02.tex

@@ -3,15 +3,11 @@
 \documentclass[a4paper, keeplastbox, biblatex]{jacow}
 
 \usepackage{graphicx}
-\usepackage{tabularx}
-\usepackage{booktabs}
-\usepackage{bm}
 \usepackage{subcaption}
 \usepackage{siunitx}
 \usepackage[USenglish, english]{babel}
 \setcounter{footnote}{1}
 \setlist[itemize]{noitemsep}
-\usepackage[colorlinks=true, allcolors=blue]{hyperref}
 \addbibresource{TUIO02.bib}
 \author{T. Dehaeze\textsuperscript{1,}\thanks{thomas.dehaeze@esrf.fr}, J. Bonnefoy, ESRF, Grenoble, France \\ C. Collette\textsuperscript{1}, Université Libre de Bruxelles, BEAMS department, Brussels, Belgium \\ \textsuperscript{1}also at Precision Mechatronics Laboratory, University of Liege, Belgium}
 \date{2021-07-26}
@@ -39,14 +35,14 @@ With the new \(4^\text{th}\) generation machines, there is an increasing need of
 These systems are usually including feedback control loops and therefore their performances are not only depending on the quality of the mechanical design, but also on its correct integration with the actuators, sensors and control system.
 
 In order to optimize the performances of such system, it is essential to consider a design approach in which the structural design and the control design are integrated.
-This approach, also called the ``mechatronics approach'', was shown to be very effective for the design many complex systems \cite{rankers98_machin,schmidt20_desig_high_perfor_mechat_third_revis_edition}.
-Such design methodology was recently used for the development of several systems used by the synchrotron community \cite{geraldes17_mechat_concep_new_high_dynam_dcm_sirius,holler18_omny_tomog_nano_cryo_stage,brendike19_esrf_doubl_cryst_monoc_protot}.
+This approach, also called the ``mechatronics approach'', was shown to be very effective for the design many complex systems \cite{rankers97_machin,schmidt20_desig_high_perfor_mechat}.
+Such design methodology was recently used for the development of several systems used by the synchrotron community \cite{geraldes17_mechat_concep_new_high_dynam_dcm_sirius,holler18_omny_tomog_nano_cryo_stage,brendike19_esrf_doubl_cryst_monoc_protot_contr_concep}.
 
 The present paper presents how the ``mechatronic approach'' was used for the design of a Nano Active Stabilization System (NASS) for the ESRF ID31 beamline.
 
 \section{NASS - MECHATRONICS APPROACH}
 \subsection{The ID31 Micro-Station}
-The ID31 micro-station is used to position samples along complex trajectories \cite{dehaeze18_sampl_stabil_for_tomog_exper}.
+The ID31 micro-station is used to position samples along complex trajectories \cite{dehaeze18_sampl_stabil_tomog_exper_presen}.
 It is composed of several stacked stages (represented in yellow in Fig.~\ref{fig:nass_concept_schematic}) which allows an high mobility.
 This however limits the position accuracy to tens of micrometers.
 
@@ -63,7 +59,7 @@ This system should be able to actively stabilize the sample position down to ten
 
 \begin{figure}[htbp]
 \centering
-\includegraphics[scale=1,scale=0.9]{TUIO02_f1.pdf}
+\includegraphics[scale=0.9]{TUIO02_f1.pdf}
 \caption{\label{fig:nass_concept_schematic}NASS - Schematic representation. 1) Micro-station, 2) Nano-hexapod, 3) Sample, 4) Metrology system.}
 \end{figure}
 
@@ -73,7 +69,7 @@ It consists of three main phases:
 
 \begin{figure*}
 \centering
-\includegraphics[scale=1,width=0.9\linewidth]{TUIO02_f2.pdf}
+\includegraphics[width=0.9\linewidth]{TUIO02_f2.pdf}
 \caption{\label{fig:nass_mechatronics_approach}Overview of the mechatronics approach used for the design of the NASS.}
 \end{figure*}
 
@@ -195,7 +191,7 @@ The mounted nano-hexapod is shown in Fig.~\ref{fig:nano_hexapod_picture}.
 
 \begin{figure}[htbp]
 \centering
-\includegraphics[scale=1,width=0.9\linewidth]{TUIO02_f5.pdf}
+\includegraphics[width=0.9\linewidth]{TUIO02_f5.pdf}
 \caption{\label{fig:nano_hexapod_picture}Nano-hexapod on top of the micro-station.}
 \end{figure}
 
@@ -225,7 +221,7 @@ The same bench was also used with the struts in order to study the added effects
 
 \begin{figure}[htbp]
 \centering
-\includegraphics[scale=1,scale=1]{TUIO02_f6.pdf}
+\includegraphics[scale=1]{TUIO02_f6.pdf}
 \caption{\label{fig:test_bench_apa_schematic}Schematic of the bench used to identify the APA dynamics.}
 \end{figure}
 
@@ -267,13 +263,13 @@ Even the off-diagonal elements (effect of one actuator on the encoder fixed in p
 \begin{figure}[htbp]
   \begin{subfigure}[t]{0.49\linewidth}
     \centering
-    \includegraphics[width=0.95\linewidth]{TUIO02_f8a.pdf}
+    \includegraphics[width=0.98\linewidth]{TUIO02_f8a.pdf}
     \caption{\label{fig:nano_hexapod_identification_comp_simscape_de} Encoder $d_{e_i}/u_i$.}
   \end{subfigure}
   \hfill
   \begin{subfigure}[t]{0.49\linewidth}
     \centering
-    \includegraphics[width=0.95\linewidth]{TUIO02_f8b.pdf}
+    \includegraphics[width=0.98\linewidth]{TUIO02_f8b.pdf}
     \caption{\label{fig:nano_hexapod_identification_comp_simscape_Vs} Force sensor $V_{s_i}/u_i$.}
   \end{subfigure}
   \caption{\label{fig:nano_hexapod_identification_comp_simscape}Comparison of the measured Frequency Response functions (FRF) with the Simscape model. From the excitation voltage to the associated encoder (\subref{fig:apa_test_bench_results_de}) and to the associated force sensor stack (\subref{fig:apa_test_bench_results_Vs}).}