11ème :

[dmems12.git] / dmems12.tex

diff --git a/dmems12.tex b/dmems12.tex
index f559661e358c7e6f2041166b10f9a7a69daf7081..10db6244de9d66bf5861f7f42700d7a49ee986ba 100644 (file)
--- a/dmems12.tex
+++ b/dmems12.tex
@@ -1,5 +1,5 @@
 
 

-\documentclass[10pt, conference, compsocconf]{IEEEtran}
+\documentclass[10pt, peerreview, compsocconf]{IEEEtran}

 %\usepackage{latex8}
 %\usepackage{times}
 \usepackage[utf8]{inputenc}
 %\usepackage{latex8}
 %\usepackage{times}
 \usepackage[utf8]{inputenc}


@@ -26,7 +26,6 @@
 \newcommand{\tab}{\ \ \ }
 
 
 \newcommand{\tab}{\ \ \ }
 
 

-

 \begin{document}
 
 
 \begin{document}
 
 


@@ -45,7 +44,7 @@
 
 
 
 
 
 

-\title{Using FPGAs for high speed and real time cantilever deflection estimation}
+\title{A new approach based on least square methods to estimate in real time cantilevers deflection with a FPGA}

 \author{\IEEEauthorblockN{Raphaël Couturier\IEEEauthorrefmark{1}, Stéphane Domas\IEEEauthorrefmark{1}, Gwenhaël Goavec-Merou\IEEEauthorrefmark{2} and Michel Lenczner\IEEEauthorrefmark{2}}
 \IEEEauthorblockA{\IEEEauthorrefmark{1}FEMTO-ST, DISC, University of Franche-Comte, Belfort, France\\
 \{raphael.couturier,stephane.domas\}@univ-fcomte.fr}
 \author{\IEEEauthorblockN{Raphaël Couturier\IEEEauthorrefmark{1}, Stéphane Domas\IEEEauthorrefmark{1}, Gwenhaël Goavec-Merou\IEEEauthorrefmark{2} and Michel Lenczner\IEEEauthorrefmark{2}}
 \IEEEauthorblockA{\IEEEauthorrefmark{1}FEMTO-ST, DISC, University of Franche-Comte, Belfort, France\\
 \{raphael.couturier,stephane.domas\}@univ-fcomte.fr}


@@ -58,7 +57,7 @@
 
 
 
 
 
 

-\maketitle
+%\maketitle

 
 \thispagestyle{empty}
 
 
 \thispagestyle{empty}
 


@@ -66,30 +65,43 @@
 
   
 
 
   
 

-{\it keywords}: FPGA, cantilever, interferometry.
+

 \end{abstract}
 
 \end{abstract}
 

+\begin{IEEEkeywords}
+FPGA, cantilever, interferometry.
+\end{IEEEkeywords}
+
+
+\IEEEpeerreviewmaketitle
+

 \section{Introduction}
 
 \section{Introduction}
 

-Cantilevers  are  used  inside  atomic  force  microscope  which  provides  high
+Cantilevers  are  used  inside  atomic  force  microscope (AFM) which  provides  high

 resolution images of  surfaces.  Several technics have been  used to measure the
 displacement  of cantilevers  in litterature.   For example,  it is  possible to
 resolution images of  surfaces.  Several technics have been  used to measure the
 displacement  of cantilevers  in litterature.   For example,  it is  possible to

-determine        accurately        the        deflection       with        optic
-interferometer~\cite{CantiOptic89},     pizeoresistor~\cite{CantiPiezzo01}    or
-capacitive  sensing~\cite{CantiCapacitive03}.  In  this paper  our  attention is
-focused   on  a  method   based  on   interferometry  to   measure  cantilevers'
-displacements.   In  this  method   cantilevers  are  illiminated  by  an  optic
-source. The interferometry produces fringes on each cantilevers which enables to
-compute the  cantilever displacement.   In order to  analyze the fringes  a high
-speed camera is used. Images need  to be processed quickly and then a estimation
-method  is   required  to  determine   the  displacement  of   each  cantilever.
-In~\cite{AFMCSEM11} {\bf verifier ref}, the authors have used an algorithm based
-on spline  to estimate  the cantilevers' positions.   The overall  process gives
-accurate results  but all the computation  are performed on  a standard computer
-using labview.  Consequently,  the main drawback of this  implementation is that
-the computer is a bootleneck in the overall process. In this paper we propose to
-use a  method based on least  square and to  implement all the computation  on a
-FGPA.
+determine  accurately  the  deflection  with different  mechanisms. 
+In~\cite{CantiPiezzo01},   authors  used   piezoresistor  integrated   into  the
+cantilever.   Nevertheless this  approach  suffers from  the  complexity of  the
+microfabrication  process needed  to  implement the  sensor  in the  cantilever.
+In~\cite{CantiCapacitive03},  authors  have  presented an  cantilever  mechanism
+based on  capacitive sensing. This kind  of technic also  involves to instrument
+the cantiliver which result in a complex fabrication process.
+
+In this  paper our attention is focused  on a method based  on interferometry to
+measure cantilevers' displacements.  In  this method cantilevers are illuminated
+by  an optic  source. The  interferometry produces  fringes on  each cantilever
+which enables to  compute the cantilever displacement.  In  order to analyze the
+fringes a  high speed camera  is used. Images  need to be processed  quickly and
+then  a estimation  method is  required to  determine the  displacement  of each
+cantilever.  In~\cite{AFMCSEM11},  authors have  used an algorithm  based on
+spline to estimate the cantilevers' positions.
+
+The overall process gives accurate results but all the computations
+are performed on a standard computer using LabView.  Consequently, the
+main drawback of this implementation is that the computer is a
+bootleneck. In this paper we propose to use a method based on least
+square and to implement all the computation on a FGPA.

 
 The remainder  of the paper  is organized as  follows. Section~\ref{sec:measure}
 describes  more precisely  the measurement  process. Our  solution based  on the
 
 The remainder  of the paper  is organized as  follows. Section~\ref{sec:measure}
 describes  more precisely  the measurement  process. Our  solution based  on the


@@ -111,28 +123,73 @@ presented.
 %% avec au milieu une unité de traitement dont on ne précise pas ce
 %% qu'elle est.
 
 %% avec au milieu une unité de traitement dont on ne précise pas ce
 %% qu'elle est.
 

+In order to develop simple,  cost effective and user-friendly cantilever arrays,
+authors   of    ~\cite{AFMCSEM11}   have   developped   a    system   based   of
+interferometry. In opposition to other optical based systems, using a laser beam
+deflection scheme and  sentitive to the angular displacement  of the cantilever,
+interferometry  is sensitive  to  the  optical path  difference  induced by  the
+vertical displacement of the cantilever.
+
+The system build by these authors is based on a Linnick
+interferomter~\cite{Sinclair:05}.  It is illustrated in
+Figure~\ref{fig:AFM}.  A laser diode is first split (by the splitter)
+into a reference beam and a sample beam that reachs the cantilever
+array.  In order to be able to move the cantilever array, it is
+mounted on a translation and rotational hexapod stage with five
+degrees of freedom. The optical system is also fixed to the stage.
+Thus, the cantilever array is centered in the optical system which can
+be adjusted accurately.  The beam illuminates the array by a
+microscope objective and the light reflects on the cantilevers.
+Likewise the reference beam reflects on a movable mirror.  A CMOS
+camera chip records the reference and sample beams which are
+recombined in the beam splitter and the interferogram.  At the
+beginning of each experiment, the movable mirror is fitted manually in
+order to align the interferometric fringes approximately parallel to
+the cantilevers.  When cantilevers move due to the surface, the
+bending of cantilevers produce movements in the fringes that can be
+detected with the CMOS camera.  Finally the fringes need to be
+analyzed. In~\cite{AFMCSEM11}, authors used a LabView program to
+compute the cantilevers' deflections from the fringes.
+
+\begin{figure}    
+\begin{center}
+\includegraphics[width=\columnwidth]{AFM}
+\end{center}
+\caption{schema of the AFM}
+\label{fig:AFM}   
+\end{figure}
+
+

 %% image tirée des expériences.
 
 \subsection{Cantilever deflection estimation}
 \label{sec:deflest}
 
 %% image tirée des expériences.
 
 \subsection{Cantilever deflection estimation}
 \label{sec:deflest}
 

-As shown on image \ref{img:img-xp}, each cantilever is covered by
-interferometric fringes. The fringes will distort when cantilevers are
-deflected. Estimating the deflection is done by computing this
-distortion. For that, (ref A. Meister + M Favre) proposed a method
-based on computing the phase of the fringes, at the base of each
-cantilever, near the tip, and on the base of the array. They assume
-that a linear relation binds these phases, which can be use to
-"unwrap" the phase at the tip and to determine the deflection.\\
+\begin{figure}    
+\begin{center}
+\includegraphics[width=\columnwidth]{lever-xp}
+\end{center}
+\caption{Portion of an image picked by the camera}
+\label{fig:img-xp}   
+\end{figure}

 
 

-More precisely, segment of pixels are extracted from images taken by a
-high-speed camera. These segments are large enough to cover several
-interferometric fringes and are placed at the base and near the tip of
-the cantilevers. They are called base profile and tip profile in the
-following. Furthermore, a reference profile is taken on the base of
-the cantilever array.
+As shown on image \ref{fig:img-xp}, each cantilever is covered by
+several interferometric fringes. The fringes will distort when
+cantilevers are deflected. Estimating the deflection is done by
+computing this distortion. For that, authors of \cite{AFMCSEM11}
+proposed a method based on computing the phase of the fringes, at the
+base of each cantilever, near the tip, and on the base of the
+array. They assume that a linear relation binds these phases, which
+can be use to "unwrap" the phase at the tip and to determine the deflection.\\

 
 

-The pixels intensity $I$ (in gray level) of each profile is modelized by :
+More precisely, segment of pixels are extracted from images taken by
+the camera. These segments are large enough to cover several
+interferometric fringes. As said above, they are placed at the base
+and near the tip of the cantilevers. They are called base profile and
+tip profile in the following. Furthermore, a reference profile is
+taken on the base of the cantilever array.
+
+The pixels intensity $I$ (in gray level) of each profile is modelized by:

 
 \begin{equation}
 \label{equ:profile}
 
 \begin{equation}
 \label{equ:profile}


@@ -147,45 +204,157 @@ on spline interpolation (see section \ref{algo-spline}). It also
 computes the coefficient used for unwrapping the phase. The second one
 is the acquisition loop, while which images are taken at regular time
 steps. For each image, the phase $\theta$ of all profiles is computed
 computes the coefficient used for unwrapping the phase. The second one
 is the acquisition loop, while which images are taken at regular time
 steps. For each image, the phase $\theta$ of all profiles is computed

-to obtain, after unwrapping, the deflection of cantilevers.
+to obtain, after unwrapping, the deflection of
+cantilevers. Originally, this computation was also done with an
+algorithm based on spline. This article proposes a new version based
+on a least square method.

 
 \subsection{Design goals}
 \label{sec:goals}
 
 
 \subsection{Design goals}
 \label{sec:goals}
 

+The main goal is to implement a computing unit to estimate the
+deflection of about $10\times10$ cantilevers, faster than the stream of
+images coming from the camera. The accuracy of results must be close
+to the maximum precision ever obtained experimentally on the
+architecture, i.e. 0.3nm. Finally, the latency between an image
+entering in the unit and the deflections must be as small as possible
+(NB: future works plan to add some control on the cantilevers).\\
+

 If we put aside some hardware issues like the speed of the link
 between the camera and the computation unit, the time to deserialize
 pixels and to store them in memory, ... the phase computation is
 obviously the bottle-neck of the whole process. For example, if we
 consider the camera actually in use, an exposition time of 2.5ms for
 If we put aside some hardware issues like the speed of the link
 between the camera and the computation unit, the time to deserialize
 pixels and to store them in memory, ... the phase computation is
 obviously the bottle-neck of the whole process. For example, if we
 consider the camera actually in use, an exposition time of 2.5ms for

-$1024\times 1204$ pixels seems the minimum that can be reached. For a
-$10\times 10$ cantilever array, if we neglect the time to extract
-pixels, it implies that computing the deflection of a single
+$1024\times 1204$ pixels seems the minimum that can be reached. For
+100 cantilevers, if we neglect the time to extract pixels, it implies
+that computing the deflection of a single

 cantilever should take less than 25$\mu$s, thus 12.5$\mu$s by phase.\\
 
 In fact, this timing is a very hard constraint. Let consider a very
 small programm that initializes twenty million of doubles in memory
 and then does 1000000 cumulated sums on 20 contiguous values
 (experimental profiles have about this size). On an intel Core 2 Duo
 cantilever should take less than 25$\mu$s, thus 12.5$\mu$s by phase.\\
 
 In fact, this timing is a very hard constraint. Let consider a very
 small programm that initializes twenty million of doubles in memory
 and then does 1000000 cumulated sums on 20 contiguous values
 (experimental profiles have about this size). On an intel Core 2 Duo

-E6650 at 2.33GHz, this program reaches an average of 155Mflops. It
-implies that the phase computation algorithm should not take more than
-$240\times 12.5 = 1937$ floating operations. For integers, it gives
-$3000$ operations.
-
-%% to be continued ...
-
-%% � faire : timing de l'algo spline en C avec atan et tout le bordel.
-
-
+E6650 at 2.33GHz, this program reaches an average of 155Mflops. 
+
+%%Itimplies that the phase computation algorithm should not take more than
+%%$155\times 12.5 = 1937$ floating operations. For integers, it gives $3000$ operations. 
+
+Obviously, some cache effects and optimizations on
+huge amount of computations can drastically increase these
+performances: peak efficiency is about 2.5Gflops for the considered
+CPU. But this is not the case for phase computation that used only few
+tenth of values.\\
+
+In order to evaluate the original algorithm, we translated it in C
+language. As said further, for 20 pixels, it does about 1550
+operations, thus an estimated execution time of $1550/155
+=$10$\mu$s. For a more realistic evaluation, we constructed a file of
+1Mo containing 200 profiles of 20 pixels, equally scattered. This file
+is equivalent to an image stored in a device file representing the
+camera. We obtained an average of 10.5$\mu$s by profile (including I/O
+accesses). It is under are requirements but close to the limit. In
+case of an occasional load of the system, it could be largely
+overtaken. A solution would be to use a real-time operating system but
+another one to search for a more efficient algorithm.
+
+But the main drawback is the latency of such a solution: since each
+profile must be treated one after another, the deflection of 100
+cantilevers takes about $200\times 10.5 = 2.1$ms, which is inadequate
+for an efficient control. An obvious solution is to parallelize the
+computations, for example on a GPU. Nevertheless, the cost to transfer
+profile in GPU memory and to take back results would be prohibitive
+compared to computation time. It is certainly more efficient to
+pipeline the computation. For example, supposing that 200 profiles of
+20 pixels can be pushed sequentially in the pipelined unit cadenced at
+a 100MHz (i.e. a pixel enters in the unit each 10ns), all profiles
+would be treated in $200\times 20\times 10.10^{-9} =$ 40$\mu$s plus
+the latency of the pipeline. This is about 500 times faster than
+actual results.\\
+
+For these reasons, an FPGA as the computation unit is the best choice
+to achieve the required performance. Nevertheless, passing from
+a C code to a pipelined version in VHDL is not obvious at all. As
+explained in the next section, it can even be impossible because of
+some hardware constraints specific to FPGAs.

 
 
 \section{Proposed solution}
 \label{sec:solus}
 
 
 
 \section{Proposed solution}
 \label{sec:solus}
 

-
-\subsection{FPGA constraints}
-
-%% contraintes imposées par le FPGA : algo pipeline/parallele, pas d'op math complexe, ...
-
+Project Oscar aims  to provide a hardware and  software architecture to estimate
+and  control the  deflection of  cantilevers. The  hardware part  consists  in a
+high-speed camera,  linked on an embedded  board hosting FPGAs. By  the way, the
+camera output stream can be pushed  directly into the FPGA. The software part is
+mostly the VHDL  code that deserializes the camera  stream, extracts profile and
+computes  the deflection. Before  focusing on  our work  to implement  the phase
+computation, we give some general information about FPGAs and the board we use.
+
+\subsection{FPGAs}
+
+A field-programmable gate  array (FPGA) is an integrated  circuit designed to be
+configured by the customer. FGPAs are composed of programmable logic components,
+called  configurable logic blocks  (CLB). These  blocks mainly  contains look-up
+tables  (LUT), flip/flops (F/F)  and latches,  organized in  one or  more slices
+connected together. Each CLB can be configured to perform simple (AND, XOR, ...)
+or complex  combinational functions.  They are interconnected  by reconfigurable
+links.  Modern FPGAs  contain memory  elements and  multipliers which  enable to
+simplify the  design and  to increase the  performance. Nevertheless,  all other
+complex  operations, like  division, trigonometric  functions, $\ldots$  are not
+available  and  must  be  done  by   configuring  a  set  of  CLBs.  Since  this
+configuration  is not  obvious at  all, it  can be  done via  a  framework, like
+ISE~\cite{ISE}. Such  a software  can synthetize a  design written in  a hardware
+description language  (HDL), map it onto  CLBs, place/route them  for a specific
+FPGA, and finally  produce a bitstream that is used to  configre the FPGA. Thus,
+from  the developper  point of  view,  the main  difficulty is  to translate  an
+algorithm in HDL code, taking  account FPGA resources and constraints like clock
+signals and I/O values that drive the FPGA.
+
+Indeed, HDL programming is very different from classic languages like
+C. A program can be seen as a state-machine, manipulating signals that
+evolve from state to state. By the way, HDL instructions can execute
+concurrently. Basic logic operations are used to agregate signals to
+produce new states and assign it to another signal. States are mainly
+expressed as arrays of bits. Fortunaltely, libraries propose some
+higher levels representations like signed integers, and arithmetic
+operations.
+
+Furthermore, even if FPGAs are cadenced more slowly than classic
+processors, they can perform pipeline as well as parallel
+operations. A pipeline consists in cutting a process in sequence of
+small tasks, taking the same execution time. It accepts a new data at
+each clock top, thus, after a known latency, it also provides a result
+at each clock top. However, using a pipeline consumes more logics
+since the components of a task are not reusable by another
+one. Nevertheless it is probably the most efficient technique on
+FPGA. Because of its architecture, it is also very easy to process
+several data concurrently. When it is possible, the best performance
+is reached using parallelism to handle simultaneously several
+pipelines in order to handle multiple data streams.
+
+\subsection{The board}
+
+The board we use is designed by the Armadeus compagny, under the name
+SP Vision. It consists in a development board hosting a i.MX27 ARM
+processor (from Freescale). The board includes all classical
+connectors: USB, Ethernet, ... A Flash memory contains a Linux kernel
+that can be launched after booting the board via u-Boot.
+
+The processor is directly connected to a Spartan3A FPGA (from Xilinx)
+via its special interface called WEIM. The Spartan3A is itself
+connected to a Spartan6 FPGA. Thus, it is possible to develop programs
+that communicate between i.MX and Spartan6, using Spartan3 as a
+tunnel. By default, the WEIM interface provides a clock signal at
+100MHz that is connected to dedicated FPGA pins.
+
+The Spartan6 is an LX100 version. It has 15822 slices, each slice
+containing 4 LUTs and 8 flip/flops. It is equivalent to 101261 logic
+cells. There are 268 internal block RAM of 18Kbits, and 180 dedicated
+multiply-adders (named DSP48), which is largely enough for our
+project.
+
+Some I/O pins of Spartan6 are connected to two $2\times 17$ headers
+that can be used as user wants. For the project, they will be
+connected to the interface card of the camera.

 
 \subsection{Considered algorithms}
 
 
 \subsection{Considered algorithms}
 


@@ -196,7 +365,7 @@ phase. The second one, detailed in this article, is based on a
 classical least square method but suppose that frequency is already
 known.
 
 classical least square method but suppose that frequency is already
 known.
 

-\subsubsection{Spline algorithm}
+\subsubsection{Spline algorithm (SPL)}

 \label{sec:algo-spline}
 Let consider a profile $P$, that is a segment of $M$ pixels with an
 intensity in gray levels. Let call $I(x)$ the intensity of profile in $x
 \label{sec:algo-spline}
 Let consider a profile $P$, that is a segment of $M$ pixels with an
 intensity in gray levels. Let call $I(x)$ the intensity of profile in $x


@@ -213,12 +382,12 @@ In order to have the frequency, the mean line $a.x+b$ (see equation \ref{equ:pro
 computed. Finding intersections of $I^s$ and this line allow to obtain
 the period thus the frequency.
 
 computed. Finding intersections of $I^s$ and this line allow to obtain
 the period thus the frequency.
 

-The phase is computed via the equation :
+The phase is computed via the equation:

 \begin{equation}
 \theta = atan \left[ \frac{\sum_{i=0}^{N-1} sin(2\pi f x^s_i) \times I^s(x^s_i)}{\sum_{i=0}^{N-1} cos(2\pi f x^s_i) \times I^s(x^s_i)} \right]
 \end{equation}
 
 \begin{equation}
 \theta = atan \left[ \frac{\sum_{i=0}^{N-1} sin(2\pi f x^s_i) \times I^s(x^s_i)}{\sum_{i=0}^{N-1} cos(2\pi f x^s_i) \times I^s(x^s_i)} \right]
 \end{equation}
 

-Two things can be noticed :
+Two things can be noticed:

 \begin{itemize}
 \item the frequency could also be obtained using the derivates of
   spline equations, which only implies to solve quadratic equations.
 \begin{itemize}
 \item the frequency could also be obtained using the derivates of
   spline equations, which only implies to solve quadratic equations.


@@ -228,12 +397,12 @@ Two things can be noticed :
   computation of $\theta$.
 \end{itemize}
 
   computation of $\theta$.
 \end{itemize}
 

-\subsubsection{Least square algorithm}
+\subsubsection{Least square algorithm (LSQ)}

 
 Assuming that we compute the phase during the acquisition loop,
 
 Assuming that we compute the phase during the acquisition loop,

-equation \ref{equ:profile} has only 4 parameters :$a, b, A$, and
+equation \ref{equ:profile} has only 4 parameters: $a, b, A$, and

 $\theta$, $f$ and $x$ being already known. Since $I$ is non-linear, a
 $\theta$, $f$ and $x$ being already known. Since $I$ is non-linear, a

-least square method based an Gauss-newton algorithm must be used to
+least square method based on a Gauss-newton algorithm can be used to

 determine these four parameters. Since it is an iterative process
 ending with a convergence criterion, it is obvious that it is not
 particularly adapted to our design goals.
 determine these four parameters. Since it is an iterative process
 ending with a convergence criterion, it is obvious that it is not
 particularly adapted to our design goals.


@@ -241,16 +410,16 @@ particularly adapted to our design goals.
 Fortunatly, it is quite simple to reduce the number of parameters to
 only $\theta$. Let $x^p$ be the coordinates of pixels in a segment of
 size $M$. Thus, $x^p = 0, 1, \ldots, M-1$. Let $I(x^p)$ be their
 Fortunatly, it is quite simple to reduce the number of parameters to
 only $\theta$. Let $x^p$ be the coordinates of pixels in a segment of
 size $M$. Thus, $x^p = 0, 1, \ldots, M-1$. Let $I(x^p)$ be their

-intensity. Firstly, we "remove" the slope by computing :
+intensity. Firstly, we "remove" the slope by computing:

 
 \[I^{corr}(x^p) = I(x^p) - a.x^p - b\]
 
 Since linear equation coefficients are searched, a classical least
 
 \[I^{corr}(x^p) = I(x^p) - a.x^p - b\]
 
 Since linear equation coefficients are searched, a classical least

-square method can be used to determine $a$ and $b$ :
+square method can be used to determine $a$ and $b$:

 
 \[a = \frac{covar(x^p,I(x^p))}{var(x^p)} \]
 
 
 \[a = \frac{covar(x^p,I(x^p))}{var(x^p)} \]
 

-Assuming an overlined symbol means an average, then :
+Assuming an overlined symbol means an average, then:

 
 \[b = \overline{I(x^p)} - a.\overline{{x^p}}\]
 
 
 \[b = \overline{I(x^p)} - a.\overline{{x^p}}\]
 


@@ -258,22 +427,22 @@ Let $A$ be the amplitude of $I^{corr}$, i.e.
 
 \[A = \frac{max(I^{corr}) - min(I^{corr})}{2}\]
 
 
 \[A = \frac{max(I^{corr}) - min(I^{corr})}{2}\]
 

-Then, the least square method to find $\theta$ is reduced to search the minimum of :
+Then, the least square method to find $\theta$ is reduced to search the minimum of:

 
 \[\sum_{i=0}^{M-1} \left[ cos(2\pi f.i + \theta) - \frac{I^{corr}(i)}{A} \right]^2\]
 
 
 \[\sum_{i=0}^{M-1} \left[ cos(2\pi f.i + \theta) - \frac{I^{corr}(i)}{A} \right]^2\]
 

-It is equivalent to derivate this expression and to solve the following equation :
+It is equivalent to derivate this expression and to solve the following equation:

 
 \begin{eqnarray*}
 2\left[ cos\theta \sum_{i=0}^{M-1} I^{corr}(i).sin(2\pi f.i) + sin\theta \sum_{i=0}^{M-1} I^{corr}(i).cos(2\pi f.i)\right] \\
 - A\left[ cos2\theta \sum_{i=0}^{M-1} sin(4\pi f.i) + sin2\theta \sum_{i=0}^{M-1} cos(4\pi f.i)\right]   = 0
 \end{eqnarray*}
 
 
 \begin{eqnarray*}
 2\left[ cos\theta \sum_{i=0}^{M-1} I^{corr}(i).sin(2\pi f.i) + sin\theta \sum_{i=0}^{M-1} I^{corr}(i).cos(2\pi f.i)\right] \\
 - A\left[ cos2\theta \sum_{i=0}^{M-1} sin(4\pi f.i) + sin2\theta \sum_{i=0}^{M-1} cos(4\pi f.i)\right]   = 0
 \end{eqnarray*}
 

-Several points can be noticed :
+Several points can be noticed:

 \begin{itemize}
 \item As in the spline method, some parts of this equation can be
   computed before the acquisition loop. It is the case of sums that do
 \begin{itemize}
 \item As in the spline method, some parts of this equation can be
   computed before the acquisition loop. It is the case of sums that do

-  not depend on $\theta$ :
+  not depend on $\theta$:

 
 \[ \sum_{i=0}^{M-1} sin(4\pi f.i), \sum_{i=0}^{M-1} cos(4\pi f.i) \] 
 
 
 \[ \sum_{i=0}^{M-1} sin(4\pi f.i), \sum_{i=0}^{M-1} cos(4\pi f.i) \] 
 


@@ -283,7 +452,7 @@ computed.
 \item The simplest method to find the good $\theta$ is to discretize
   $[-\pi,\pi]$ in $nb_s$ steps, and to search which step leads to the
   result closest to zero. By the way, three other lookup tables can
 \item The simplest method to find the good $\theta$ is to discretize
   $[-\pi,\pi]$ in $nb_s$ steps, and to search which step leads to the
   result closest to zero. By the way, three other lookup tables can

-  also be computed before the loop :
+  also be computed before the loop:

 
 \[ sin \theta, cos \theta, \]
 
 
 \[ sin \theta, cos \theta, \]
 


@@ -293,8 +462,8 @@ computed.
 
 \end{itemize}
 
 
 \end{itemize}
 

-Finally, the whole summarizes in an algorithm (called LSQ in the following) in two parts, one before and one during the acquisition loop :
-\begin{algorithm}[h]
+Finally, the whole summarizes in an algorithm (called LSQ in the following) in two parts, one before and one during the acquisition loop:
+\begin{algorithm}[htbp]

 \caption{LSQ algorithm - before acquisition loop.}
 \label{alg:lsq-before}
 
 \caption{LSQ algorithm - before acquisition loop.}
 \label{alg:lsq-before}
 


@@ -315,7 +484,7 @@ Finally, the whole summarizes in an algorithm (called LSQ in the following) in t
    }
 \end{algorithm}
 
    }
 \end{algorithm}
 

-\begin{algorithm}[ht]
+\begin{algorithm}[htbp]

 \caption{LSQ algorithm - during acquisition loop.}
 \label{alg:lsq-during}
 
 \caption{LSQ algorithm - during acquisition loop.}
 \label{alg:lsq-during}
 


@@ -380,7 +549,7 @@ Finally, the whole summarizes in an algorithm (called LSQ in the following) in t
 
 \subsubsection{Comparison}
 
 
 \subsubsection{Comparison}
 

-We compared the two algorithms on the base of three criterions :
+We compared the two algorithms on the base of three criteria:

 \begin{itemize}
 \item precision of results on a cosinus profile, distorted with noise,
 \item number of operations,
 \begin{itemize}
 \item precision of results on a cosinus profile, distorted with noise,
 \item number of operations,


@@ -399,12 +568,12 @@ discretization correspond to an error of 0.15nm on the lever
 deflection, which is smaller than the best precision they achieved,
 i.e. 0.3nm.
 
 deflection, which is smaller than the best precision they achieved,
 i.e. 0.3nm.
 

-For each test, we add some noise to the profile : each group of two
+For each test, we add some noise to the profile: each group of two

 pixels has its intensity added to a random number picked in $[-N,N]$
 (NB: it should be noticed that picking a new value for each pixel does
 not distort enough the profile). The absolute error on the result is
 evaluated by comparing the difference between the reference and
 pixels has its intensity added to a random number picked in $[-N,N]$
 (NB: it should be noticed that picking a new value for each pixel does
 not distort enough the profile). The absolute error on the result is
 evaluated by comparing the difference between the reference and

-computed phase, out of $2\pi$, expressed in percents. That is : $err =
+computed phase, out of $2\pi$, expressed in percents. That is: $err =

 100\times \frac{|\theta_{ref} - \theta_{comp}|}{2\pi}$.
 
 Table \ref{tab:algo_prec} gives the maximum and average error for the two algorithms and increasing values of $N$.
 100\times \frac{|\theta_{ref} - \theta_{comp}|}{2\pi}$.
 
 Table \ref{tab:algo_prec} gives the maximum and average error for the two algorithms and increasing values of $N$.


@@ -446,7 +615,7 @@ largely beyond the worst experimental ones.
 
 \begin{figure}[ht]
 \begin{center}
 
 \begin{figure}[ht]
 \begin{center}

-  \includegraphics[width=9cm]{intens-noise20-spl}
+  \includegraphics[width=\columnwidth]{intens-noise20}

 \end{center}
 \caption{Sample of worst profile for N=10}
 \label{fig:noise20}
 \end{center}
 \caption{Sample of worst profile for N=10}
 \label{fig:noise20}


@@ -454,7 +623,7 @@ largely beyond the worst experimental ones.
 
 \begin{figure}[ht]
 \begin{center}
 
 \begin{figure}[ht]
 \begin{center}

-  \includegraphics[width=9cm]{intens-noise60-lsq}
+  \includegraphics[width=\columnwidth]{intens-noise60}

 \end{center}
 \caption{Sample of worst profile for N=30}
 \label{fig:noise60}
 \end{center}
 \caption{Sample of worst profile for N=30}
 \label{fig:noise60}


@@ -466,25 +635,126 @@ to numbers of pixels $M$. For LSQ, it also depends on $nb_s$ and for
 SPL on $N = k\times M$, i.e. the number of interpolated points. 
 
 We assume that $M=20$, $nb_s=1024$, $k=4$, all possible parts are
 SPL on $N = k\times M$, i.e. the number of interpolated points. 
 
 We assume that $M=20$, $nb_s=1024$, $k=4$, all possible parts are

-already in lookup tables and only arithmetic operations (+, -, *, /)
-are taken account. Translating the two algorithms in C code, we obtain
-about 400 operations for LSQ and 1340 (plus the unknown for $atan$)
-for SPL. Even if the result is largely in favor of LSQ, we can notice
-that executing the C code (compiled with \tt{-O3}) of SPL on an
-2.33GHz Core 2 Duo only takes 6.5µs in average, which is under our
-desing goals. The final decision is thus driven by the third criterion.\\
-
-The Spartan 6 used in our architecture has hard constraint : it has no
-floating point units. Thus, all computations have to be done with
-integers. 
+already in lookup tables and a limited set of operations (+, -, *, /,
+$<$, $>$) is taken account. Translating the two algorithms in C code, we
+obtain about 430 operations for LSQ and 1550 (plus few tenth for
+$atan$) for SPL. This result is largely in favor of LSQ. Nevertheless,
+considering the total number of operations is not really pertinent for
+an FPGA implementation: it mainly depends on the type of operations
+and their
+ordering. The final decision is thus driven by the third criterion.\\
+
+The Spartan 6 used in our architecture has a hard constraint: it has no built-in
+floating  point  units.   Obviously,  it  is  possible  to   use  some  existing
+"black-boxes"  for double  precision  operations.  But they  have  a quite  long
+latency. It is much simpler to  exclusively use integers, with a quantization of
+all double  precision values. Obviously,  this quantization should  not decrease
+too much the  precision of results. Furthermore, it should not  lead to a design
+with  a huge  latency because  of operations  that could  not complete  during a
+single or few clock cycles. Divisions  are in this case and, moreover, they need
+a varying  number of  clock cycles  to complete. Even  multiplications can  be a
+problem:  DSP48 take  inputs of  18  bits maximum.  For larger  multiplications,
+several DSP must be combined, increasing the latency.
+
+Nevertheless, the hardest constraint does not come from the FPGA characteristics
+but from the algorithms. Their VHDL  implentation will be efficient only if they
+can be fully (or near) pipelined. By the way, the choice is quickly done: only a
+small  part of  SPL  can be.   Indeed,  the computation  of spline  coefficients
+implies to solve  a tridiagonal system $A.m =  b$. Values in $A$ and  $b$ can be
+computed from  incoming pixels intensity  but after, the back-solve  starts with
+the  lastest  values,  which  breaks  the  pipeline.  Moreover,  SPL  relies  on
+interpolating far more points than profile size. Thus, the end of SPL works on a
+larger amount of data than the beginning, which also breaks the pipeline.
+
+LSQ has  not this problem: all parts  except the dichotomial search  work on the
+same  amount  of  data, i.e.  the  profile  size.  Furthermore, LSQ  needs  less
+operations than SPL, implying a  smaller output latency. Consequently, it is the
+best candidate for phase  computation. Nevertheless, obtaining a fully pipelined
+version supposes that  operations of different parts complete  in a single clock
+cycle. It is  the case for simulations but it completely  fails when mapping and
+routing the design  on the Spartan6. By the way,  extra-latency is generated and
+there must be idle times between two profiles entering into the pipeline.
+
+%%Before obtaining the least bitstream, the crucial question is: how to
+%%translate the C code the LSQ into VHDL ?
+
+
+%\subsection{VHDL design paradigms}
+
+\section{Experimental tests}
+
+In this section we explain what  we have done yet. Until now, we could not perform
+real experiments  since we just have  received the FGPA  board. Nevertheless, we
+will include real experiments in the final version of this paper.

 
 

+\subsection{VHDL implementation}

 
 
 
 

-\subsection{VHDL design paradigms}

 
 

-\subsection{VHDL implementation}
+% - ecriture d'un code en C avec integer
+% - calcul de la taille max en bit de chaque variable en fonction de la quantization.
+% - tests de quantization : équilibre entre précision et contraintes FPGA
+% - en parallèle : simulink et VHDL à la main
+
+
+From the LSQ algorithm, we have written a C program that uses only
+integer values. We use a very simple quantization by multiplying
+double precision values by a power of two, keeping the integer
+part. For example, all values stored in lut$_s$, lut$_c$, $\ldots$ are
+scaled by 1024.  Since LSQ also computes average, variance, ... to
+remove the slope, the result of implied euclidian divisions may be
+relatively wrong. To avoid that, we also scale the pixel intensities
+by a power of two. Futhermore, assuming $nb_s$ is fixed, these
+divisions have a knonw denominator. Thus, they can be replaced by
+their multiplication/shift counterpart. Finally, all other
+multiplications or divisions by a power of two have been replaced by
+left or right bit shifts. By the way, the code only contains
+additions, substractions and multiplications of signed integers, which
+is perfectly adapted to FGPAs.
+
+As said above, hardware constraints have a great influence on the VHDL
+implementation. Consequently, we searched the maximum value of each
+variable as a function of the different scale factors and the size of
+profiles, which gives their maximum size in bits. That size determines
+the maximum scale factors that allow to use the least possible RAMs
+and DSPs. Actually, we implemented our algorithm with this maximum
+size but current works study the impact of quantization on the results
+precision and design complexity. We have compared the result of the
+LSQ version using integers and doubles and observed that the precision
+of both were similar.
+
+Then we built two versions of VHDL codes: one directly by hand coding
+and the other with Matlab using the Simulink HDL coder
+feature~\cite{HDLCoder}. Although the approach is completely different
+we obtained VHDL codes that are quite comparable. Each approach has
+advantages and drawbacks.  Roughly speaking, hand coding provides
+beautiful and much better structured code while Simulink allows to
+produce a code faster.  In terms of throughput and latency,
+simulations shows that the two approaches are close with a slight
+advantage for hand coding.  We hope that real experiments will confirm
+that.
+
+\subsection{Simulation}
+
+Currently, we have only simulated our VHDL codes with GHDL and GTKWave (two free
+tools with linux).  Both approaches led to correct results.  At the beginning of
+our simulations, our  pipiline could compute a new phase each  33 cycles and the
+length of the  pipeline was equal to  95 cycles.  When we tried  to generate the
+corresponding bitsream  with ISE environment  we had many problems  because many
+stages required  more than the  10$n$s required by  the clock frequency.   So we
+needed to decompose  some part of the  pipeline in order to add  some cycles and
+simplify some parts between a clock top.
+% ghdl + gtkwave
+% au mieux : une phase tous les 33 cycles, latence de 95 cycles.
+% mais routage/placement impossible.
+\subsection{Bitstream creation}
+
+Currently both  approaches provide synthesable  bitstreams with ISE.   We expect
+that the  pipeline will  have a latency  of 112  cycles, i.e. 1.12$\mu$s  and it
+could accept new profiles of pixel each 48 cycles, i.e. 480$n$s.
+
+% pas fait mais prévision d'une sortie tous les 480ns avec une latence de 1120

 
 

-\section{Experimental results}

 \label{sec:results}
 
 
 \label{sec:results}