[467] | 1 | \documentclass{JINST} |
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| 2 | \usepackage[pdftex]{graphicx} |
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[474] | 3 | \graphicspath{{figures/}} |
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[467] | 4 | \usepackage[figuresright]{rotating} |
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[473] | 5 | %\usepackage{graphicx} |
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| 6 | %\usepackage[T1]{fontenc} |
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[467] | 7 | \usepackage{eurosym} |
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[473] | 8 | %\usepackage{rotating} |
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| 9 | %\usepackage[dvips]{color} |
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[467] | 10 | |
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[473] | 11 | |
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[467] | 12 | %used explicitly in the text |
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| 13 | \newcommand{\refTab}[1]{Tab.~\ref{#1}} |
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| 14 | \newcommand{\refFig}[1]{Fig.~\ref{#1}} |
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| 15 | \newcommand{\refSec}[1]{Sec.~\ref{#1}} |
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| 16 | |
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| 17 | |
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| 18 | |
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| 19 | |
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[473] | 20 | \title{PARISROC, a Photomultiplier Array Integrated Readout Chip.} |
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[467] | 21 | % |
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| 22 | |
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[473] | 23 | \author{S. Conforti$^a$, Second Author$^b$\thanks{Corresponding |
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[467] | 24 | author.}~ and Third Author$^b$\\ |
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[473] | 25 | \llap{$^a$}Laboratoire de l'Accélérateur Linéaire, IN2P3-CNRS, Université Paris-Sud 11, |
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| 26 | Bât. 200, 91898 Orsay Cedex, France\\ |
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[467] | 27 | \llap{$^b$}Name of Institute,\\ |
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| 28 | Address, Country\\ |
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[473] | 29 | E-mail: \email{conforti@lal.in2p3.fr}} |
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[467] | 30 | |
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| 31 | |
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| 32 | |
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| 33 | |
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| 34 | \abstract{ |
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[473] | 35 | PARISROC is a complete read |
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| 36 | out chip, in AMS SiGe 0.35 \begin{math}\mu{}\end{math}m technology |
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[477] | 37 | \cite{Genolini:2008uc} |
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[473] | 38 | %[1] |
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| 39 | , for photomultipliers array. It allows triggerless acquisition for |
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| 40 | next generation neutrino experiments and it belongs to an R\&D program |
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| 41 | funded by French national agency for research (ANR) called |
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| 42 | PMm2: "`Innovative electronics for photodetectors array |
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| 43 | used in High Energy Physics and Astroparticles"' |
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[477] | 44 | \cite{PMm2Site:2006} |
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[473] | 45 | %[2] |
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| 46 | (ref.ANR-06-BLAN-0186). The ASIC integrates 16 independent and auto |
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| 47 | triggered channels with variable gain and provides charge and time |
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| 48 | measurement by a 12-bit ADC and a 24-bit Counter. The charge |
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| 49 | measurement should be performed from 1 up to 300 pe with a good |
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| 50 | linearity. The time measurement allowed to a coarse time with a 24-bit |
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| 51 | counter at 10 MHz and a fine time on a 100ns ramp to achieve a |
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| 52 | resolution of 1 ns. The ASIC sends out only the relevant data through |
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| 53 | network cables to the central data storage. |
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[467] | 54 | }%end of abstract |
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| 55 | |
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| 56 | %\pacs{13.30.a,14.20.Dh,14.60.Pq,26.65.t+,29.40.Gx,29.40.Ka,29.40.Mc,95.55.Vj,95.85.Ry, |
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| 57 | %97.60.Bw} |
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| 58 | |
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[473] | 59 | %\submitto{Journal of Instrumentation} |
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[467] | 60 | |
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| 61 | \keywords{Keyword1; Keyword2; Keyword3} |
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| 62 | |
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| 63 | \begin{document} |
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| 64 | %use BST file provided by SPIRES for JHEP and modify it to forbid "to lower case" title |
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| 65 | \bibliographystyle{Campagne} |
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[476] | 66 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
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[473] | 67 | \section{Introduction} |
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| 68 | \label{sec:Intro} |
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[476] | 69 | %%%%%%%%%%%%%%%%%%%%%% |
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[473] | 70 | The PMm2 project: "`Innovative electronics for |
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| 71 | photodetectors array used in High Energy Physics and |
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[477] | 72 | Astroparticles"' \cite{PMm2Site:2006} |
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[473] | 73 | %[2] |
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| 74 | proposes to segment the large surface of photodetection in macro |
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| 75 | pixel consisting of an array of 16 photomultipliers connected to an |
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| 76 | autonomous front-end electronics () and powered by a common High |
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| 77 | Voltage. These large detectors are used in next generation proton decay |
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| 78 | and neutrino experiment (i.e. the post-SuperKamiokande detectors as |
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| 79 | those that will take place in megaton size water tanks) and will |
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| 80 | require very large surfaces of photo detection and a large volume of |
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| 81 | data. The micro-electronics group's (OMEGA from the LAL at Orsay) |
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| 82 | purpose is the front-end electronics conception and |
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[477] | 83 | realization. This R\&D \cite{PMm2Site:2006} |
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[473] | 84 | %[2] |
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| 85 | involves three French laboratories (LAL Orsay, LAPP Annecy, IPN |
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| 86 | Orsay) and ULB Bruxells for the DAQ. It is funded for three years by |
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| 87 | the French National Agency for Research (ANR) under the reference |
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| 88 | ANR-06-BLAN-0186. |
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[468] | 89 | |
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| 90 | |
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[473] | 91 | LAL Orsay is in charge of the design and tests of the readout chip |
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| 92 | named PARISROC which stands for Photomultiplier ARrray Integrated in |
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| 93 | Si-Ge Read Out Chip. |
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[468] | 94 | |
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[474] | 95 | \begin{figure}[!htbp] |
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[473] | 96 | \begin{center} |
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[474] | 97 | \includegraphics[width=0.7\columnwidth,height=6cm]{img1.jpg} |
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[473] | 98 | \caption{Principal of PMm2 proposal for megaton scale Cerenkov water |
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| 99 | tank.} |
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| 100 | \label{fig:1} |
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| 101 | \end{center} |
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| 102 | \end{figure} |
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[467] | 103 | |
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[473] | 104 | The detectors such as SuperKamiokande, are large tanks covered by a |
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| 105 | significant number of large photomultipliers (20"), |
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| 106 | the next generation neutrino experiments will require a bigger surface |
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| 107 | of photo detection and thus more photomultipliers. As a consequence the |
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[477] | 108 | total cost has an important relief \cite{Genolini:2008uc}. |
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[473] | 109 | \begin{itemize} |
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| 110 | \item A smaller number of electronics, thanks to the 16 PMTs macropixel with |
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| 111 | a common electronics, even if it induces more electronic channels; |
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| 112 | \item A common High Voltage for the 16 PMTs so a reduced number of |
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| 113 | underwater cables, cables that are also used to brought the DATA to |
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| 114 | the surface; |
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| 115 | \item The front-end closed to the PMTs that allow a suppression of |
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| 116 | underwater connector. |
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| 117 | \end{itemize} |
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[467] | 118 | |
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[473] | 119 | The general principle of PMm2 project is that the ASIC and a FPGA |
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| 120 | manage the dialog between the PMTs and the surface controller (\refFig{fig:2}). |
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| 121 | |
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| 122 | \begin{center} |
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[474] | 123 | \begin{figure}[!!htbp] |
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| 124 | \includegraphics[width=0.7\columnwidth,height=6cm]{img2.jpg} |
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[473] | 125 | \caption{Principle of the PMm2 project.} |
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| 126 | \label{fig:2} |
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| 127 | \end{figure} |
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| 128 | \end{center} |
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| 129 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
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| 130 | \section{PARISROC architecture} |
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| 131 | \label{sec:PARISROCArchi} |
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| 132 | The ASIC Parisroc is composed of 16 analogue channels managed by a |
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| 133 | common digital part (\refFig{fig:3}). |
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| 134 | |
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[467] | 135 | \begin{center} |
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[474] | 136 | \begin{figure}[!htbp] |
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| 137 | \includegraphics[width=0.7\columnwidth,height=6cm]{img3.jpg} |
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[473] | 138 | \caption{PARISROC global schematic.} |
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| 139 | \label{fig:3} |
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| 140 | \end{figure} |
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[467] | 141 | \end{center} |
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| 142 | |
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[473] | 143 | Each analogue channel is made of a low noise preamplifier with |
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| 144 | variable and adjustable gain. The variable gain is common for all |
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| 145 | channels and it can change from 8 to 1 on 4 bits. The gain is also |
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| 146 | tuneable channel by channel to adjust the input detector's gain, up to |
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| 147 | a factor 4 to an accuracy of 7\% with 8 bits. |
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[468] | 148 | |
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[473] | 149 | The preamplifier is followed by a slow channel for the charge |
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| 150 | measurement in parallel with a fast channel for the trigger output. |
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[468] | 151 | |
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[473] | 152 | The slow channel is made by a slow shaper followed by an analogue |
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| 153 | memory with a depth of 2 to provide a linear charge measurement up to |
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| 154 | 50~pC; this charge is converted by a 12-bits Wilkinson ADC. One follower |
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| 155 | OTA is added to deliver an analogue multiplexed charge measurement. |
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[468] | 156 | |
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[473] | 157 | The fast channel consists in a fast shaper (15~ns) followed by 2 low |
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| 158 | offset discriminators to auto-trig down to 50~fC. The thresholds are |
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| 159 | loaded by 2 internal 10-bit DACs common for the 16 channels and an |
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| 160 | individual 4bit DAC for one discriminator. The 2 discriminator outputs |
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| 161 | are multiplexed to provide only 16 trigger outputs. Each output trigger |
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| 162 | is latched to hold the state of the response until the end of the clock |
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| 163 | cycle. It is also delayed to open the hold switch at the maximum of the |
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| 164 | slow shaper. An "`OR"' of the 16 trigger gives a 17th output. |
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| 165 | |
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| 166 | |
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| 167 | For each channel, a fine time measurement is made by an analogue |
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| 168 | memory with depth of 2 which samples a 12-bit ramp, common for all |
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| 169 | channels, at the same time of the charge. This time is then converted |
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| 170 | by a 12 bit Wilkinson ADC. |
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| 171 | |
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| 172 | The two ADC discriminators have a common ramp, of 8/10/12 bits, as |
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| 173 | threshold to convert the charge and the fine time. In addition a bandgap bloc provides all voltage references. |
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| 174 | |
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| 175 | \begin{center} |
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[474] | 176 | \begin{figure}[!htbp] |
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| 177 | \includegraphics[width=0.7\columnwidth,height=6cm]{img4.jpg} |
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[473] | 178 | \caption{PARISROC Layout.} |
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| 179 | \label{fig:4} |
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| 180 | \end{figure} |
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| 181 | \end{center} |
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| 182 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
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| 183 | \subsection{Analogue Channel description and simulations} |
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| 184 | \label{ssec:AnalogChannel} |
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| 185 | %%%%%%%%%%%%%%%%%%%%%%%%%%% |
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| 186 | \refFig{fig:5} represents, in a schematic way, the detail of one channel analogue |
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| 187 | part. |
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| 188 | |
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| 189 | \begin{center} |
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[474] | 190 | \begin{figure}[!htbp] |
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| 191 | \includegraphics[width=0.7\columnwidth,height=6cm]{img5.jpg} |
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[473] | 192 | \caption{PARISROC one channel analogue part schematic.} |
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| 193 | \label{fig:5} |
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| 194 | \end{figure} |
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| 195 | \end{center} |
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| 196 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
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| 197 | \subsection{Preamplifier} |
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| 198 | \label{ssec:Preamplifier} |
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| 199 | %%%%%%%%%%%%%%%%%%%%%%%%%%% |
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| 200 | The input preamplifier is a low noise preamplifier with variable gain |
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| 201 | thanks to the switched input ($C_{in}$) and feedback ($C_f$) capacitors that |
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| 202 | can be adjusted (\refFig{fig:6}). |
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| 203 | |
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| 204 | This gain can vary changing $C_{in}$, which is |
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| 205 | common to the 16 channels, over 4 bits and $C_{f}$, to adjust preamplifier |
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| 206 | gain channel by channel. This adjustment allows correction of the PMT |
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| 207 | gain dispersion due to a use of a common HV. |
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| 208 | |
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| 209 | \begin{center} |
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[474] | 210 | \begin{figure}[!htb] |
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| 211 | \includegraphics[width=0.7\columnwidth,height=6cm]{img6.jpg} |
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[473] | 212 | \caption{PARISROC preamplifier schematic.} |
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| 213 | \label{fig:6} |
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| 214 | \end{figure} |
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| 215 | \end{center} |
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| 216 | |
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| 217 | The preamplifier is designed as a voltage |
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| 218 | preamplifier in p-type Cascode structure to allow the acquisition of a |
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| 219 | fast input signal with a large dynamic range. |
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| 220 | |
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| 221 | The input transistor is a PMOS in common source |
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| 222 | configuration: $W = 800~\mu$m; $L = 0.35~\mu$m; the big input transistor is |
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| 223 | chosen to keep the preamplifier noise contribution low and to achieve a |
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| 224 | high gm. It supplies the output (the drain terminal) to the input |
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| 225 | terminal (source terminal) of the second stage transistor: $W = 100~\mu$m; |
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| 226 | $L = 0.35~\mu$m; the output transistor must be small to reach preamplifier |
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| 227 | high speed performances. The utility of the cascode preamplifier is in |
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| 228 | the large input impedance of the common source (with also the |
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| 229 | characteristic of Current Buffer) and better frequency response of a |
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| 230 | common Gate. An output buffer stage is designed in order to adapt the |
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| 231 | output impedance to the loaded impedance. The input dc level is high |
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| 232 | (about 2.6~V) while the output dc level is low (about 1~V). Because of |
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| 233 | the single side structure of preamplifier, it is hard to use the |
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| 234 | external reference voltage to set the dc operating point; the idea is |
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| 235 | to use an OTA as the dc feedback amplifier. |
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| 236 | |
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| 237 | In \refFig{fig:7} are shown preamplifier's output waveforms |
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| 238 | for fixed gain and different input signal (left panel) and for fixed |
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| 239 | input signal and different preamplifier gain (right panel). |
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| 240 | |
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[467] | 241 | \begin{center} |
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[474] | 242 | \begin{figure}[!htbp] |
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| 243 | \begin{tabular}{rl} |
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| 244 | \includegraphics[width=0.5\columnwidth,height=6cm]{img7a.jpg} & |
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| 245 | \includegraphics[width=0.5\columnwidth,height=6cm]{img7b.jpg} |
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| 246 | \end{tabular} |
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| 247 | caption{Simulated preamplifier output waveforms for different input |
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[473] | 248 | signals with fixed gain (left panel) and for fixed input |
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| 249 | signal at different gain (different input capacitor values (right |
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| 250 | panel).} |
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| 251 | \label{fig:7} |
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| 252 | \end{figure} |
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[467] | 253 | \end{center} |
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| 254 | |
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[473] | 255 | The input signal, used in simulation, is a triangle signal with 4.5~ns |
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| 256 | rise and fall time and 5~ns of duration as shown in \refFig{fig:8}. This current |
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| 257 | signal is sent to an external resistor (50~Ohms) and varies from 0 to 5~mA |
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| 258 | in order to simulate a PMT charge from 0 to 50~pC which represents 0 |
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| 259 | to 300 photo-electrons when the PM gain is $10^{6}$. |
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[467] | 260 | |
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[473] | 261 | \begin{center} |
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[474] | 262 | \begin{figure}[!htbp] |
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| 263 | \includegraphics[width=0.7\columnwidth,height=6cm]{img8.jpg} |
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[473] | 264 | \caption{Simulation input signal.} |
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| 265 | \label{fig:8} |
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| 266 | \end{figure} |
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| 267 | \end{center} |
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[467] | 268 | |
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[473] | 269 | The \refFig{fig:9} displays the input dynamic range allowed to the preamplifier |
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| 270 | linearity performance. \refTab{tab:1} lists the residuals obtained for different |
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| 271 | gains and shows a good linearity (better than $\pm 1\%$). |
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[467] | 272 | |
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[473] | 273 | \begin{center} |
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[474] | 274 | \begin{figure}[!htbp] |
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| 275 | \includegraphics[width=0.7\columnwidth,height=6cm]{img9.jpg} |
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[473] | 276 | \caption{Preamplifier linearity.} |
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| 277 | \label{fig:9} |
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| 278 | \end{figure} |
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| 279 | \end{center} |
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[467] | 280 | |
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| 281 | |
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[473] | 282 | \begin{table} |
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| 283 | \centering |
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| 284 | \caption{TO BE COMPLETED} |
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| 285 | \label{tab:1} |
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| 286 | \begin{tabular}{|c|c|c|c|} |
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| 287 | \hline |
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| 288 | $G_{pa}$ & $V_{out-max}$ & $Qi_{max}/n_{pe}$ & Residuals (\%) \\ |
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| 289 | \hline |
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| 290 | 8 & 1.394~V & 40~pC/250~pe & -0.6 to 0.2 \\ |
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| 291 | 4 & 0.841~V & 48~pC/300~pe & -0.1 to 0.3 \\ |
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| 292 | 2 & 0.417~V & 48~pC/300~pe & -0.2 to 0.3 \\ |
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| 293 | \hline |
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| 294 | \end{tabular} |
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| 295 | \end{table} |
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[467] | 296 | |
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| 297 | |
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[473] | 298 | |
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| 299 | The \refFig{fig:10} displays the preamplifier noise with an |
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| 300 | rms value of 13~fC and a Signal to Noise ratio of $\approx 12$. |
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| 301 | \refTab{tab:2} summarizes the results obtained. |
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[467] | 302 | |
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[473] | 303 | \begin{center} |
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[474] | 304 | \begin{figure}[!htbp] |
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| 305 | \includegraphics[width=0.7\columnwidth,height=6cm]{img10.jpg} |
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[473] | 306 | \caption{Preamplifier noise simulation; $G_{pa}=8$; $C_{in}=4$~pF and |
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| 307 | $C_{f}=0.5$~pF.} |
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| 308 | \end{figure} |
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| 309 | \label{fig:10} |
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| 310 | \end{center} |
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[467] | 311 | |
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[473] | 312 | \begin{table} |
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| 313 | \centering |
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| 314 | \caption{TO BE COMPLETED} |
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| 315 | \label{tab:2} |
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| 316 | \begin{tabular}{|c|c|c|} |
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| 317 | \hline |
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| 318 | RMS & SNR & $V_{out}(1 p.e)$ \\ |
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| 319 | \hline |
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| 320 | $468~\mu$V ($\approx 1/12$~p.e, $\approx 13$~fC ) & 11.6 & 5.43~mV\\ |
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| 321 | \hline |
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| 322 | \end{tabular} |
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| 323 | \end{table} |
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[467] | 324 | |
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[473] | 325 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
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| 326 | \subsection{Trigger output} |
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| 327 | \label{ssec:Trigger} |
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| 328 | %%%%%%%%%%%%%%%%%%%%%%%%%%% |
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| 329 | The PARISROC is a self-triggered device. The fast channel has been |
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| 330 | conceived for this purpose.The amplified signal flows in a fast shaper that is a CRRC filter with |
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| 331 | a time constant of 15~ns. Its high gain allows to send high signal to |
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| 332 | the discriminator and thus to trigger easily on 1/3 of photo-electron. |
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| 333 | It has a classical design: differential pair is followed by a buffer. |
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[467] | 334 | |
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[474] | 335 | \begin{figure}[!htbp] |
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[473] | 336 | \centering |
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[474] | 337 | \includegraphics[width=0.7\columnwidth,height=6cm]{img11.jpg} |
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[473] | 338 | \caption{Fast shaper schematics.} |
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| 339 | \label{fig:11} |
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| 340 | \end{figure} |
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[467] | 341 | |
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[473] | 342 | The \refFig{fig:12} represents the fast shaper output |
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| 343 | waveforms for a variable input signal. The \refTab{tab:3} lists the fast |
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| 344 | shaper principal characteristics obtained in simulation. |
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| 345 | |
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[474] | 346 | \begin{figure}[!htbp] |
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[473] | 347 | \centering |
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[474] | 348 | \begin{tabular}{rl} |
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| 349 | \includegraphics[width=0.5\columnwidth,height=6cm]{img12a.jpg} & |
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| 350 | \includegraphics[width=0.5\columnwidth,height=6cm]{img12b.jpg} |
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| 351 | \end{tabular} |
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[473] | 352 | \caption{Simulated fast shaper outputs ($G_{pa} = 8$ with input from 1-10~pe (left panel) |
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| 353 | and from 1/3~pe to 2~pe (right panel).} |
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| 354 | \label{fig:12} |
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| 355 | \end{figure} |
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| 356 | |
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| 357 | \begin{table} |
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| 358 | \centering |
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| 359 | \caption{To be completed} |
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| 360 | \label{tab:3} |
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| 361 | \begin{tabular}{|c|c|c|c|} |
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| 362 | \hline |
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| 363 | RMS & SNR & $V_{out}(1 p.e)$ & $T_p$ \\ |
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| 364 | \hline |
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| 365 | $2.36~\mu$V ($\approx 1/16$~p.e, $\approx 10$~fC ) & 16 & 37.85~mV & 8~ns\\ |
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| 366 | \hline |
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| 367 | \end{tabular} |
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| 368 | \end{table} |
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| 369 | |
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| 370 | The fast shaper (15~ns) is followed by a low |
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| 371 | offset discriminator to auto-trig down to 50~fC (1/3~pe at $10^6$ gain). |
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| 372 | |
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| 373 | |
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| 374 | The two discriminators can be used alone or |
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| 375 | simultaneously. Their outputs are multiplexed to ease the choice. Both |
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| 376 | are simple low offset comparators with the same schematic. The |
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| 377 | difference comes from the way to set the threshold. The first |
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| 378 | discriminator has the threshold sets by one 10-bit DAC, common to all |
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| 379 | 16 channels, and one 4-bit DAC for each channel. The second |
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| 380 | discriminator has the threshold sets by only the 10 bit common DAC. |
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| 381 | Each output trigger is latched to hold the state of the response in SCA |
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| 382 | channel. In \refFig{fig:13} are shown the triggers and the zoom of the triggers rise |
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| 383 | time in order to see the time walk of around 4~ns. |
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| 384 | |
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| 385 | |
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[474] | 386 | \begin{figure}[!htbp] |
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[473] | 387 | \centering |
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[474] | 388 | \begin{tabular}{rl} |
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| 389 | \includegraphics[width=0.5\columnwidth,height=6cm]{img13a.jpg}& |
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| 390 | \includegraphics[width=0.5\columnwidth,height=6cm]{img13b.jpg} |
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| 391 | \end{tabular} |
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[473] | 392 | \caption{Simulated trigger output (input charge from 0 to 10~p.e; |
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| 393 | threshold at 1/3~p.e). Zoom of trigger rise time on right |
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| 394 | pannel.} |
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| 395 | \label{fig:13} |
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| 396 | \end{figure} |
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| 397 | |
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| 398 | Each output trigger is latched to hold the |
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| 399 | state of the response in SCA channel. SCA channel is the also called |
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| 400 | "`Analogue memory"'. The SCA has a |
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| 401 | depth equal to two; this means that there are two T\&H for time |
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| 402 | measurement as well as for charge measurement. |
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| 403 | |
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[474] | 404 | \begin{figure}[!htbp] |
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[473] | 405 | \centering |
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[474] | 406 | \includegraphics[width=0.7\columnwidth,height=6cm]{img14.jpg} |
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[473] | 407 | \caption{SCA (switched capacitor array) scheme.} |
---|
| 408 | \label{fig:14} |
---|
| 409 | \end{figure} |
---|
| 410 | |
---|
| 411 | The voltage level of the signal coming from |
---|
| 412 | slow shaper or ramp TDC cell is memorised in the T\&H capacitor (500~fF) |
---|
| 413 | so "`Track \& Hold Cell"' allows |
---|
| 414 | to lock the capacitor value only when a calibrated trigger (from fast |
---|
| 415 | channel) occurs within the selected column. The SCA column is selected, read and erased by |
---|
| 416 | the digital part. |
---|
| 417 | |
---|
[474] | 418 | \begin{figure}[!htbp] |
---|
[473] | 419 | \centering |
---|
[474] | 420 | \includegraphics[width=0.7\columnwidth,height=6cm]{img15.jpg} |
---|
[473] | 421 | \caption{Operation of T\&H cell.} |
---|
| 422 | \label{fig:15} |
---|
| 423 | \end{figure} |
---|
| 424 | |
---|
| 425 | On \refFig{fig:15} is illustrated the T\&H cell mode of |
---|
| 426 | operation: when a signal arrives in the discriminator cell is detected |
---|
| 427 | and the output trigger signal is sent to the T\&H cell. |
---|
| 428 | The output trigger is delayed and calibrated before being sent. |
---|
| 429 | |
---|
| 430 | |
---|
| 431 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 432 | \subsection{Charge channel} |
---|
| 433 | \label{ssec:Charge} |
---|
| 434 | %%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 435 | The charge channel is the slow channel: the signal amplified by the |
---|
| 436 | variable gain preamplifier is sent to the slow shaper, a typical |
---|
| 437 | $\mathrm{CRRC}^2$ filter with variable peaking time. The |
---|
| 438 | peaking time can be set from 50~ns (default value) to 200~ns thanks to |
---|
| 439 | the switched feedback capacitors. |
---|
| 440 | |
---|
| 441 | On left part of \refFig{fig:16} are represented the slow shaper waveforms for |
---|
| 442 | different shaping times and the same input signal. The noise value (\refTab{tab:4} |
---|
| 443 | and right part of \refFig{fig:16}), from $980~\mu$V to $1.6$~mV (simulation results), foresee |
---|
| 444 | good noise performance. |
---|
| 445 | |
---|
[474] | 446 | \begin{figure}[!htbp] |
---|
[473] | 447 | \centering |
---|
[474] | 448 | \begin{tabular}{rl} |
---|
| 449 | \includegraphics[width=0.5\columnwidth,height=6cm]{img16a.jpg}& |
---|
| 450 | \includegraphics[width=0.5\columnwidth,height=6cm]{img16b.jpg} |
---|
| 451 | \end{tabular} |
---|
[473] | 452 | \caption{Slow shaper output waveforms simulation (left panel). Slow shaper |
---|
| 453 | output noise simulation (right panel).} |
---|
| 454 | \label{fig:16} |
---|
| 455 | \end{figure} |
---|
| 456 | |
---|
| 457 | \begin{table} |
---|
| 458 | \centering |
---|
| 459 | \caption{TO BE COMPLETED. $G_{pa} = 8$} |
---|
| 460 | \label{tab:4} |
---|
| 461 | \begin{tabular}{|c|c|c|c|} |
---|
| 462 | \hline |
---|
| 463 | Time constant & RMS & SNR & $V_{out}(1 p.e)$ \\ |
---|
| 464 | \hline |
---|
| 465 | 50~ns & \parbox[t]{20mm}{$1.68$~mV \\ $\approx 1/17$~p.e \\ $ \approx 9$~fC} |
---|
| 466 | & 11 |
---|
| 467 | & \parbox[t]{20mm}{$29$~mV \\ $T_p = 48$~ns } \\ |
---|
| 468 | 100~ns & \parbox[t]{20mm}{$1.26$~mV\\$\approx 1/12$~p.e \\ $ \approx 20$~fC} |
---|
| 469 | & 8 |
---|
| 470 | & \parbox[t]{20mm}{$15$~mV \\ $T_p = 78$~ns }\\ |
---|
| 471 | 200~ns & \parbox[t]{20mm}{$0.98$~mV\\$\approx 1/5$~p.e \\ $ \approx 32$~fC} |
---|
| 472 | & 5 |
---|
| 473 | & \parbox[t]{23mm}{$8$~mV \\ $ T_p = 141.5$~ns } \\ |
---|
| 474 | \hline |
---|
| 475 | \end{tabular} |
---|
| 476 | \end{table} |
---|
| 477 | |
---|
| 478 | The \refFig{fig:17} and \refTab{tab:5} illustrate the linearity performance for |
---|
| 479 | different time constants. Simulations show a good linearity with |
---|
| 480 | residuals from -0.5\% to 0.2\% at $T_p = 50$~ns, from |
---|
| 481 | -1\% to 0.3\% at $T_p =100$~ns and -0.7\% to 0.3\% at |
---|
| 482 | $T_p=200$~ns. |
---|
| 483 | |
---|
[474] | 484 | \begin{figure}[!htbp] |
---|
[473] | 485 | \centering |
---|
[474] | 486 | \includegraphics[width=0.7\columnwidth,height=6cm]{img17.jpg} |
---|
[473] | 487 | \caption{Slow shaper linearity simulation.} |
---|
| 488 | \label{fig:17} |
---|
| 489 | \end{figure} |
---|
| 490 | |
---|
| 491 | \begin{table} |
---|
| 492 | \centering |
---|
| 493 | \caption{TO BE COMPLETED} |
---|
| 494 | \label{tab:5} |
---|
| 495 | \begin{tabular}{|c|c|c|c|} |
---|
| 496 | \hline |
---|
| 497 | Time constante & $V_{out-max}$ & $Qi_{max}/n_{pe}$ & Residuals (\%) \\ |
---|
| 498 | \hline |
---|
| 499 | 50~ns & 1.437~V & 13~pC/80~pe & -0.5 to 0.2 \\ |
---|
| 500 | 100~ns & 1.493~V & 24~pC/150~pe & -1.0 to 0.3 \\ |
---|
| 501 | 200~ns & 1.385~V & 48~pC/300~pe & -0.7 to 0.3 \\ |
---|
| 502 | \hline |
---|
| 503 | \end{tabular} |
---|
| 504 | \end{table} |
---|
| 505 | |
---|
| 506 | The Slow shaper maximum value, therefore the charge value, is then |
---|
| 507 | memorized in the analogue memory, with a depth of 2, thanks to the |
---|
| 508 | delayed trigger. \refFig{fig:18} gives the simulated slow shaper and SCA |
---|
| 509 | signals. |
---|
| 510 | |
---|
[474] | 511 | \begin{figure}[!htbp] |
---|
[473] | 512 | \centering |
---|
[474] | 513 | \includegraphics[width=0.7\columnwidth,height=6cm]{img18.jpg} |
---|
[473] | 514 | \caption{Slow shaper \& SCA simulation.} |
---|
| 515 | \label{fig:18} |
---|
| 516 | \end{figure} |
---|
| 517 | This charge, stored as a voltage value, is then converted in digital |
---|
| 518 | value thanks to the 8/10/12 bit Wilkinson ADC. |
---|
| 519 | |
---|
| 520 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 521 | \subsection{Time measurement} |
---|
| 522 | \label{ssec:Timemeas} |
---|
| 523 | %%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 524 | For each channel, a fine time measurement is performed by the analogue |
---|
| 525 | memory with a depth of 2 which samples a 12 bit ramp (100~ns), common |
---|
| 526 | for all channels, at the same time of the charge. |
---|
| 527 | |
---|
| 528 | In \refFig{fig:19} is represented the TDC Ramp general schematic. The current, |
---|
| 529 | which flows in feedback, charges the capacitance $C_f$ when the switch is |
---|
| 530 | off. When the switch is turned off, $C_f$ discharges. Signals \verb|start\_ramp| and |
---|
| 531 | \verb|start\_ramp\_b| manage the switches. The rising signal starts the ramp |
---|
| 532 | and the falling signal stop the ramp (\refFig{fig:19}). |
---|
| 533 | |
---|
[474] | 534 | \begin{figure}[!htbp] |
---|
[473] | 535 | \centering |
---|
[474] | 536 | \begin{tabular}{rl} |
---|
| 537 | \includegraphics[width=0.5\columnwidth,height=6cm]{img19a.jpg}& |
---|
| 538 | \includegraphics[width=0.5\columnwidth,height=6cm]{img19b.jpg} |
---|
| 539 | \end{tabular} |
---|
[473] | 540 | \caption{TDC Ramp general schematic.} |
---|
| 541 | \label{fig:19} |
---|
| 542 | \end{figure} |
---|
| 543 | In order to avoid the large falling time of the ramp due to the $C_f$ |
---|
| 544 | discharge time and the problem of non linearity at the start and the |
---|
| 545 | end of ramp signal (\refFig{fig:20}), the real ramp is created from two |
---|
| 546 | ramps. |
---|
| 547 | |
---|
[474] | 548 | \begin{figure}[!htbp] |
---|
[473] | 549 | \centering |
---|
[474] | 550 | \includegraphics[width=0.7\columnwidth,height=6cm]{img20.jpg} |
---|
[473] | 551 | \caption{TDC Ramp.} |
---|
| 552 | \label{fig:20} |
---|
| 553 | \end{figure} |
---|
| 554 | |
---|
| 555 | The signal start ramp, coming from the digital |
---|
| 556 | part, enters in two delay cells. The two delayed signals create the |
---|
| 557 | first and second ramps. Commutating alternatively two switches the 100~ns ramp TDC is created |
---|
| 558 | (\refFig{fig:21} and \refFig{fig:22}). |
---|
| 559 | |
---|
[474] | 560 | \begin{figure}[!htbp] |
---|
[473] | 561 | \centering |
---|
[474] | 562 | \includegraphics[width=0.7\columnwidth,height=6cm]{img21.jpg} |
---|
[473] | 563 | \caption{TDC Ramp scheme.} |
---|
| 564 | \label{fig:21} |
---|
| 565 | \end{figure} |
---|
| 566 | |
---|
[474] | 567 | \begin{figure}[!htbp] |
---|
[473] | 568 | \centering |
---|
[474] | 569 | \includegraphics[width=0.7\columnwidth,height=6cm]{img22.jpg} |
---|
[473] | 570 | \caption{TDC Ramp simulation.} |
---|
| 571 | \label{fig:22} |
---|
| 572 | \end{figure} |
---|
| 573 | |
---|
| 574 | This time value, stored as a voltage value, is then converted in |
---|
| 575 | digital value tanks to the 8/10/12 bit Wilkinson ADC. |
---|
| 576 | |
---|
| 577 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 578 | \subsection{ADC ramp} |
---|
| 579 | \label{ssec:ADCramp} |
---|
| 580 | %%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 581 | In \refFig{fig:23} is represented the Ramp ADC general scheme. It is the |
---|
| 582 | same as TDC ramp one, the difference is in a variable current source |
---|
| 583 | which allows obtaining 8bit/10bit/12bit ADC according to the injected |
---|
| 584 | current. \refTab{tab:6} gives, for each ramp, the time duration to reach 3.3~V. |
---|
| 585 | |
---|
[474] | 586 | \begin{figure}[!htbp] |
---|
[473] | 587 | \centering |
---|
[474] | 588 | \includegraphics[width=0.7\columnwidth,height=6cm]{img23.jpg} |
---|
[473] | 589 | \caption{ADC ramp schematic.} |
---|
| 590 | \label{fig:23} |
---|
| 591 | \end{figure} |
---|
| 592 | |
---|
| 593 | \begin{table} |
---|
| 594 | \centering |
---|
| 595 | \caption{TO BE COMPLETED} |
---|
| 596 | \label{tab:6} |
---|
| 597 | \begin{tabular}{|l|l|} |
---|
| 598 | \hline |
---|
| 599 | Header 1 & Header 2 \\ |
---|
| 600 | 12 bit ADC & From 0.9~V to 3.3~V in $102.0~\mu{}$s \\ |
---|
| 601 | 10 bit ADC & From 0.9~V to 3.3~V in $25.6~\mu{}$s \\ |
---|
| 602 | \phantom{ }8 bit ADC & From 0.9~V to 3.3~V in $6.4~\mu{}$s \\ |
---|
| 603 | \hline |
---|
| 604 | \end{tabular} |
---|
| 605 | \end{table} |
---|
| 606 | |
---|
| 607 | Then the ADC ramp is compared thanks to a Discriminator to the voltage |
---|
| 608 | values, which corresponds to charge and fine time values, stored in the |
---|
| 609 | SCA. The digital converted DATA are then treated by the digital part. |
---|
| 610 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 611 | \subsection{Digital part} |
---|
| 612 | \label{ssec:Digital} |
---|
| 613 | %%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 614 | The digital part of PARISROC is built around 4 modules which are "`acquisition"', "`conversion"', "`readout"' and "`top manager"'. Actually, PARISROC is based on 2 memories. During acquisition, |
---|
| 615 | discriminated analog signals are stored into an analog memory (the SCA: |
---|
| 616 | switched capacitor array). The analog to digital conversion module |
---|
| 617 | converts analog charges and times from SCA into 12 bits digital values. |
---|
| 618 | These digital values are saved into registers (RAM). At the end of the |
---|
| 619 | cycle, the RAM is readout by an external system. The block diagram is |
---|
| 620 | given on \refFig{fig:24}. |
---|
| 621 | |
---|
| 622 | |
---|
[474] | 623 | \begin{figure}[!htbp] |
---|
[473] | 624 | \centering |
---|
[474] | 625 | \includegraphics[width=0.7\columnwidth,height=6cm]{img24.jpg} |
---|
[473] | 626 | \caption{Block diagram of the digital part.} |
---|
| 627 | \label{fig:24} |
---|
| 628 | \end{figure} |
---|
| 629 | |
---|
| 630 | This sequence is made thanks to the top manager module which controls |
---|
| 631 | the 3 other ones. When 1 or more channels are hit, it starts ADC |
---|
| 632 | conversion and then the readout of digitized data. The maximum cycle |
---|
| 633 | length is about $200~\mu$s. During |
---|
| 634 | conversion and readout, acquisition is never stopped. It means that |
---|
| 635 | discriminated analog signals can be stored in the SCA at any time of |
---|
| 636 | the sequence shown in on \refFig{fig:25}. |
---|
| 637 | |
---|
[474] | 638 | \begin{figure}[!htbp] |
---|
[473] | 639 | \centering |
---|
[474] | 640 | \includegraphics[width=0.7\columnwidth,height=6cm]{img25.jpg} |
---|
[473] | 641 | \caption{Top manager sequence.} |
---|
| 642 | \label{fig:25} |
---|
| 643 | \end{figure} |
---|
| 644 | |
---|
| 645 | The first module in the sequence is the acquisition |
---|
| 646 | which is dedicated to charge and fine time measurements. It manages the |
---|
| 647 | SCA where charge and fine time are stored as a voltage like. It also |
---|
| 648 | integrates the coarse time measurement thanks to a 24-bit gray counter |
---|
| 649 | with a resolution of 100~ns. Each channel has a depth of 2 for the SCA |
---|
| 650 | and they are managed individually. Besides, SCA is treated like a FIFO |
---|
| 651 | memory: analog voltage can be written, read and erased from this |
---|
| 652 | memory. |
---|
| 653 | |
---|
| 654 | |
---|
[474] | 655 | \begin{figure}[!htbp] |
---|
[473] | 656 | \centering |
---|
[474] | 657 | \includegraphics[width=0.7\columnwidth,height=6cm]{img26.jpg} |
---|
[473] | 658 | \caption{SCA analogue voltage} |
---|
| 659 | \label{fig:26} |
---|
| 660 | \end{figure} |
---|
| 661 | |
---|
| 662 | Then, the conversion module converts analog values stored in |
---|
| 663 | the SCA (charge and fine time: cf. \`refFig{fig:26}) in digital ones thanks to a 12-bit |
---|
| 664 | Wilkinson ADC. The counter clock frequency is 40~MHz, it implies a |
---|
| 665 | maximum ADC conversion time of $103~\mu$s |
---|
| 666 | when it overflows. This module makes 32 conversions in 1 run (16 |
---|
| 667 | charges and 16 fine times). |
---|
| 668 | |
---|
| 669 | Finally, the readout module permits to empty all the registers |
---|
| 670 | to an external system. As it will only transfer hit channels, this |
---|
| 671 | module will tag each frame with its channel number: it works as a |
---|
| 672 | selective readout. The pattern used is composed of 4 data: 4-bit |
---|
| 673 | channel number, 24-bit coarse time, 12-bit charge and 12-bit fine time. |
---|
| 674 | The total length of one frame is 52 bits. The maximum readout time |
---|
| 675 | appears when all channels are hit. About 832 bits of data are |
---|
| 676 | transferred to the concentrator with a 10~MHz clock: the readout takes |
---|
| 677 | about $100~\mu$s with $1~\mu$s between 2 frames. |
---|
| 678 | |
---|
| 679 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 680 | \section{ASIC Laboratory tests} |
---|
| 681 | \label{sec:ASICLAbTest} |
---|
| 682 | %%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 683 | The PARISROC has been submitted in June 2008; a first batch of 6 ASICs |
---|
| 684 | has been produced and received in January 2009 (a second batch of 14 |
---|
| 685 | ASICs in May 2009. |
---|
| 686 | |
---|
| 687 | The ASIC test has been a critical step in the PARISROC planning due to |
---|
| 688 | the ASIC complexity.A dedicated test board has been designed and realized for this purpose |
---|
| 689 | (\refFig{fig:27}). Its role is to allow the characterization of the chip and the |
---|
| 690 | communication between photomultipliers and ASIC. This is possible |
---|
| 691 | thanks to a dedicated Labview program that allows sending the ASIC |
---|
| 692 | configuration (slow control parameters; ASIC parameters, etc) and |
---|
| 693 | receiving the output bits via a USB cable connected to the test board. |
---|
| 694 | The Labview is developed by LAL. |
---|
| 695 | |
---|
[474] | 696 | \begin{figure}[!htbp] |
---|
[473] | 697 | \centering |
---|
[474] | 698 | \includegraphics[width=0.7\columnwidth,height=6cm]{img27.jpg} |
---|
[473] | 699 | \caption{Test Board.} |
---|
| 700 | \label{fig:27} |
---|
| 701 | \end{figure} |
---|
| 702 | |
---|
| 703 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 704 | \subsection{General tests} |
---|
| 705 | \label{ssec:GeneralTest} |
---|
| 706 | %%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 707 | On \refFig{fig:28} is shown the Test Bench used in laboratory. It is composed by a |
---|
| 708 | test board, a signal generator, an oscilloscope, multimeters and PC to |
---|
| 709 | run labview program. |
---|
| 710 | |
---|
[474] | 711 | \begin{figure}[!htbp] |
---|
[473] | 712 | \centering |
---|
[474] | 713 | \includegraphics[width=0.7\columnwidth,height=6cm]{img28.jpg} |
---|
[473] | 714 | \caption{Test Bench.} |
---|
| 715 | \label{fig:28} |
---|
| 716 | \end{figure} |
---|
| 717 | |
---|
| 718 | The signal generator is a TEKTRONIX single |
---|
| 719 | channel function generator. It is used to create the input charge |
---|
| 720 | injected in the ASIC. The signal injected has the shaping as similar as |
---|
| 721 | possible to the PMT signal. On \refFig{fig:28} is represented the generator input |
---|
| 722 | signal and its characteristics. |
---|
| 723 | |
---|
[474] | 724 | \begin{figure}[!htbp] |
---|
[473] | 725 | \centering |
---|
[474] | 726 | \includegraphics[width=0.7\columnwidth,height=6cm]{img29.jpg} |
---|
| 727 | %%%% NOT USED \includegraphics[width=0.5\columnwidth,height=6cm]{img34.jpg} |
---|
[473] | 728 | \caption{Input signals} |
---|
| 729 | \label{fig:29} |
---|
| 730 | \end{figure} |
---|
| 731 | |
---|
| 732 | At the beginning all the standard electrical |
---|
| 733 | characteristics have been tested: DC levels, analogue output signals, |
---|
| 734 | the analogue part characteristics and then the pedestals, the DAC |
---|
| 735 | linearity, S\-curves (trigger efficiency as a function of the injected |
---|
| 736 | charge or the threshold), the ADC linearity. The first purpose is the |
---|
| 737 | comparison between simulation results and test measurements; most of |
---|
| 738 | them are in agreement with the ASIC characteristics, obtained in |
---|
| 739 | simulation. |
---|
| 740 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 741 | \subsection{Analogue tests} |
---|
| 742 | \label{ssec:AnalogueTest} |
---|
| 743 | %%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 744 | The DC level characterization is the first step in ASIC |
---|
| 745 | characterization; in particular the DC uniformity of the analogue part |
---|
| 746 | DC level for the different channels has to be measured. |
---|
| 747 | |
---|
| 748 | In \refFig{fig:30} are represented the preamplifier, slow |
---|
| 749 | shaper and fast shaper DC uniformity plots. The DC uniformity test has a small dispersion |
---|
| 750 | of 0.4\%, 0.1\% and 0.05\% respectively for the preamplifier, the slow |
---|
| 751 | shaper and the fast shaper (\refTab{tab:7}). |
---|
| 752 | |
---|
[474] | 753 | \begin{figure}[!htbp] |
---|
[473] | 754 | \centering |
---|
[474] | 755 | \begin{tabular}{c} |
---|
| 756 | \includegraphics[width=0.7\columnwidth,height=6cm]{img30a.jpg}\\ |
---|
| 757 | \includegraphics[width=0.7\columnwidth,height=6cm]{img30b.jpg}\\ |
---|
| 758 | \includegraphics[width=0.7\columnwidth,height=6cm]{img30c.jpg} |
---|
| 759 | \end{tabular} |
---|
[473] | 760 | \caption{DC uniformity.} |
---|
| 761 | \label{fig:30} |
---|
| 762 | \end{figure} |
---|
| 763 | |
---|
| 764 | \begin{table} |
---|
| 765 | \centering |
---|
| 766 | \caption{TO BE COMPLETED} |
---|
| 767 | \label{tab:7} |
---|
| 768 | \begin{tabular}{|l|c|c|c|} |
---|
| 769 | \hline |
---|
| 770 | DC level & RMS \\ |
---|
| 771 | Preamplifier & 3.8~mV (0.40~\%) \\ |
---|
| 772 | Slow shaper & 1.3~mV (0.10~\%) \\ |
---|
| 773 | Fast shaper & 1.0~mV (0.05\%) \\ |
---|
| 774 | \hline |
---|
| 775 | \end{tabular} |
---|
| 776 | \end{table} |
---|
| 777 | |
---|
| 778 | The second step is the analogue part output signals: Injecting a |
---|
| 779 | charge equivalent to 10~pe, and setting a preamplifier gain at 8, are |
---|
| 780 | observed and compared with simulation results all the output waveforms. |
---|
| 781 | |
---|
| 782 | There is a good agreement in preamplifier results ( \refFig{fig:31} and \refTab{tab:8}), the |
---|
| 783 | amplitude has the same value while time rise value has a difference of |
---|
| 784 | 3~ns. This difference is due to the output buffer placed in the test |
---|
| 785 | board. |
---|
| 786 | |
---|
[474] | 787 | \begin{figure}[!htbp] |
---|
[473] | 788 | \centering |
---|
[474] | 789 | \begin{tabular}{rl} |
---|
| 790 | \includegraphics[width=0.5\columnwidth,height=6cm]{img31a.jpg}& |
---|
| 791 | \includegraphics[width=0.5\columnwidth,height=6cm]{img31b.jpg} |
---|
| 792 | \end{tabular} |
---|
[473] | 793 | \caption{Measurement and simulation of the preamplifier output for |
---|
| 794 | an input charge of 10~pe.} |
---|
| 795 | \label{fig:31} |
---|
| 796 | \end{figure} |
---|
| 797 | |
---|
| 798 | \begin{table} |
---|
| 799 | \centering |
---|
| 800 | \caption{TO BE COMPLETED. Preamplifier parameters.... $G_{pa} = 8$. WHY not same parameters 1~pe and 10~p.e} |
---|
| 801 | \label{tab:8} |
---|
| 802 | \begin{tabular}{|l|c|c|} |
---|
| 803 | \hline |
---|
| 804 | & Measurement & Simulation \\ |
---|
| 805 | \hline |
---|
| 806 | Maximum voltage (10~pe) & 50.00~mV & 50.83~mV \\ |
---|
| 807 | Rise time (10~pe) & 7.78~ns & 4.79~ns \\ |
---|
| 808 | RMS noise & 1~mV & 0.47~mV \\ |
---|
| 809 | without USB cable & 0.66~mV & \\ |
---|
| 810 | Noise in pe & 0.2 & 0.086 \\ |
---|
| 811 | without USB cable & 0.132 & \\ |
---|
| 812 | Maximum voltage (1~pe) & 5.00~mV & 5.43~mV \\ |
---|
| 813 | SNR (1~pe ????) & 5 & 11.6 \\ |
---|
| 814 | without USB cable & 7.5 & \\ |
---|
| 815 | \hline |
---|
| 816 | \end{tabular} |
---|
| 817 | \end{table} |
---|
| 818 | |
---|
| 819 | The slow shaper waveforms are shown in \refFig{fig:32} while \refTab{tab:9} |
---|
| 820 | summarizes the results. The first differences appear: a different value |
---|
| 821 | in amplitude for slow shaper signal and fast shaper signal that is |
---|
| 822 | probably associate, also, to the Output Buffer. The second relevant |
---|
| 823 | difference is in noise value, in particular in slow shaper noise |
---|
| 824 | performance (\refTab{tab:9}). |
---|
| 825 | |
---|
[474] | 826 | \begin{figure}[!htbp] |
---|
[473] | 827 | \centering |
---|
[474] | 828 | \begin{tabular}{rl} |
---|
| 829 | \includegraphics[width=0.5\columnwidth,height=6cm]{img32a.jpg} |
---|
| 830 | \includegraphics[width=0.5\columnwidth,height=6cm]{img32b.jpg} |
---|
| 831 | \end{tabular} |
---|
[473] | 832 | \caption{Measurement and simulation of the slow shaper output for an |
---|
| 833 | input charge of 10~pe.} |
---|
| 834 | \label{fig:32} |
---|
| 835 | \end{figure} |
---|
| 836 | |
---|
| 837 | \begin{table} |
---|
| 838 | \centering |
---|
| 839 | \caption{TO BE COMPLETED. $G_{pa} = 8$ and $RC = 50$~ns.} |
---|
| 840 | \label{tab:9} |
---|
| 841 | \begin{tabular}{|l|c|c|} |
---|
| 842 | \hline |
---|
| 843 | & Measurement & Simulation \\ |
---|
| 844 | \hline |
---|
| 845 | Maximum Voltage (10~pe) & 117~mV & 290~mV \\ |
---|
| 846 | Rise time (10~pe) & 18.0~ns & 19.1~ns \\ |
---|
| 847 | RMS noise & 4.0~mV & 1.7~mV \\ |
---|
| 848 | Noise in pe & 0.3 & 0.08 \\ |
---|
| 849 | Maximum Voltage (1~pe) & 12~mV & 19~mV \\ |
---|
| 850 | SNR & 3 & 11 \\ |
---|
| 851 | \hline |
---|
| 852 | \end{tabular} |
---|
| 853 | \end{table} |
---|
| 854 | |
---|
| 855 | The Fast shaper results are shown in \refFig{fig:33} |
---|
| 856 | and \refTab{tab:10}. |
---|
[474] | 857 | \begin{figure}[!htb] |
---|
[473] | 858 | \centering |
---|
[474] | 859 | \begin{tabular}{rl} |
---|
| 860 | \includegraphics[width=0.5\columnwidth,height=6cm]{img33a.jpg} |
---|
| 861 | \includegraphics[width=0.5\columnwidth,height=6cm]{img33b.jpg} |
---|
| 862 | \end{tabular} |
---|
[473] | 863 | \caption{Measurement and simulation of the fast shaper output for an |
---|
| 864 | input charge of 1 pe.} |
---|
| 865 | \label{fig:33} |
---|
| 866 | \end{figure} |
---|
| 867 | |
---|
| 868 | |
---|
| 869 | \begin{table} |
---|
| 870 | \centering |
---|
| 871 | \caption{TO BE COMPLETED. $G_{pa} = 8$.} |
---|
| 872 | \label{tab:10} |
---|
| 873 | \begin{tabular}{|l|c|c|} |
---|
| 874 | \hline |
---|
| 875 | & Measurement & Simulation \\ |
---|
| 876 | \hline |
---|
| 877 | RMS noise & 2.5~mV & 2.4~mV \\ |
---|
| 878 | Noise in pe & 0.08 & 0.05 \\ |
---|
| 879 | Maximum Voltage (1~pe) & 30~mV & 42~mV \\ |
---|
| 880 | SNR & 12 & 18 \\ |
---|
| 881 | \hline |
---|
| 882 | \end{tabular} |
---|
| 883 | \end{table} |
---|
| 884 | Another important characteristic is the |
---|
| 885 | linearity. The output voltage in function of the input injected charge |
---|
| 886 | is plotted for the different analogue signals. \refFig{fig:34} gives few examples for |
---|
[477] | 887 | the preamplifier at different gains. \refTab{tab:11} summarizes the fit |
---|
[473] | 888 | results of these linearities. Good linearity performances are shown by |
---|
| 889 | residuals (better than $\pm 2~\%$) value but for a |
---|
| 890 | smaller dynamic range than simulation. |
---|
| 891 | |
---|
[474] | 892 | \begin{figure}[!htbp] |
---|
[473] | 893 | \centering |
---|
[474] | 894 | \begin{tabular}{c} |
---|
| 895 | \includegraphics[width=0.7\columnwidth,height=6cm]{img34a.jpg} |
---|
| 896 | \includegraphics[width=0.7\columnwidth,height=6cm]{img34b.jpg} |
---|
| 897 | \includegraphics[width=0.7\columnwidth,height=6cm]{img34c.jpg} |
---|
| 898 | \end{tabular} |
---|
[473] | 899 | \caption{Preamplifier linearity for different gains.} |
---|
| 900 | \label{fig:34} |
---|
| 901 | \end{figure} |
---|
| 902 | |
---|
| 903 | \begin{table} |
---|
| 904 | \centering |
---|
| 905 | \caption{TO BE COMPLETED} |
---|
| 906 | \label{tab:11} |
---|
| 907 | \begin{tabular}{|c|c|c|c|} |
---|
| 908 | \hline |
---|
| 909 | Preamplifier Gains & Maximum voltage & Charge/Nb of pe & Residuals \\ |
---|
| 910 | \hline |
---|
| 911 | 8 & 0.52~V & 12~pC / 78~pe & -1.0~\% to 0.8~\% \\ |
---|
| 912 | 4 & 0.64~V & 32~pC / 198~pe & -1.0~\% to 1.0~\% \\ |
---|
| 913 | 2 & 0.51~V & 50~pC / 312~pe & -2.0~\% to 1.5~\% \\ |
---|
| 914 | \hline |
---|
| 915 | \end{tabular} |
---|
| 916 | \end{table} |
---|
| 917 | |
---|
| 918 | |
---|
| 919 | \refFig{fig:35} represents an example of slow shaper |
---|
| 920 | linearity for a time constant of 50~ns and a preamplifier gain of 8 |
---|
| 921 | with residuals better than $pm 1~\%$. |
---|
| 922 | |
---|
[474] | 923 | \begin{figure}[!htbp] |
---|
[473] | 924 | \centering |
---|
[474] | 925 | \includegraphics[width=0.7\columnwidth,height=6cm]{img35.jpg} |
---|
[473] | 926 | \caption{Slow shaper linearity; $RC =50$~ns and $G_{pa}=8$.} |
---|
| 927 | \label{fig:35} |
---|
| 928 | \end{figure} |
---|
| 929 | |
---|
| 930 | \refFig{fig:36} gives an example of the fast shaper linearity until an injected |
---|
| 931 | charge of 10~pe. Residuals better than $ \pm 2~\%$ |
---|
| 932 | are obtained. |
---|
| 933 | |
---|
[474] | 934 | \begin{figure}[!htbp] |
---|
[473] | 935 | \centering |
---|
[474] | 936 | \includegraphics[width=0.7\columnwidth,height=6cm]{img36.jpg} |
---|
[473] | 937 | \caption{Fast shaper linearity up to 10~pe.} |
---|
| 938 | \label{fig:36} |
---|
| 939 | \end{figure} |
---|
| 940 | |
---|
| 941 | The preamplifier linearity in function of |
---|
| 942 | variable feedback capacitor value with an input charge of 10~pe and |
---|
| 943 | with residuals from $-2.5~\%$ to $1.4~\%$ is represented on \refFig{fig:37} . The gain |
---|
| 944 | adjustment linearity is nice at 2~\% on 8 bits. |
---|
| 945 | |
---|
[474] | 946 | \begin{figure}[!htbp] |
---|
[473] | 947 | \centering |
---|
[474] | 948 | \includegraphics[width=0.7\columnwidth,height=6cm]{img37.jpg} |
---|
[473] | 949 | \caption{Preamplifier linearity vs feedback capacitor value.} |
---|
| 950 | \label{fig:37} |
---|
| 951 | \end{figure} |
---|
| 952 | |
---|
| 953 | On \refFig{fig:38} is given the gain uniformity. For the |
---|
| 954 | different preamplifier gains is plotted the maximum voltage value for |
---|
| 955 | all channels in order to investigate the homogeneity among the whole |
---|
| 956 | chip, essential for a multichannels ASIC. Residual dispersion of 0.05~\%, |
---|
| 957 | 0.013~\% and 0.012~\% have respectively been obtained for gain 8, 4 and |
---|
| 958 | 2. |
---|
| 959 | |
---|
[474] | 960 | \begin{figure}[!htbp] |
---|
[473] | 961 | \centering |
---|
[474] | 962 | \includegraphics[width=0.7\columnwidth,height=6cm]{img38.jpg} |
---|
[473] | 963 | \caption{Gain uniformity for $G_{pa}=8, 4, 2$.} |
---|
| 964 | \label{fig:38} |
---|
| 965 | \end{figure} |
---|
| 966 | |
---|
| 967 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 968 | \subsection{DAC linearity} |
---|
| 969 | \label{ssec:DAClinearity} |
---|
| 970 | %%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 971 | The DAC linearity has been measured and it consists in measuring the |
---|
| 972 | voltage DAC ($V_{dac}$) amplitude obtained for different DAC register |
---|
| 973 | values. \refFig{fig:39} gives the evolution of $V_{dac}$ as a function of the register for the two |
---|
| 974 | DACs and residuals from $-0.1~\%$ to $0.1~\%$. |
---|
| 975 | |
---|
[474] | 976 | \begin{figure}[!htbp] |
---|
[473] | 977 | \centering |
---|
[474] | 978 | \begin{tabular}{rl} |
---|
| 979 | \includegraphics[width=0.5\columnwidth,height=6cm]{img39a.jpg}& |
---|
| 980 | \includegraphics[width=0.5\columnwidth,height=6cm]{img39b.jpg} |
---|
| 981 | \end{tabular} |
---|
[473] | 982 | \caption{DAC linearity; DAC1 and DAC2 respectively.} |
---|
| 983 | \label{fig:39} |
---|
| 984 | \end{figure} |
---|
| 985 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 986 | \subsection{Trigger output} |
---|
| 987 | \label{ssec:TriggerMeas} |
---|
| 988 | %%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 989 | The trigger output behavior was studied scanning the threshold for |
---|
| 990 | different injected charges. At first no charge was injected which |
---|
| 991 | corresponds to measure the fast shaper pedestal. The result is |
---|
| 992 | represented on \refFig{fig:40} for each channel. The S-curves |
---|
| 993 | are superimposed meaning good homogeneity. The spread |
---|
| 994 | is of one DAC count ($LSB DAC = 1.78$~mV) or 0.06~pe. |
---|
| 995 | |
---|
[474] | 996 | \begin{figure}[!htbp] |
---|
[473] | 997 | \centering |
---|
[474] | 998 | \includegraphics[width=0.7\columnwidth,height=6cm]{img40.jpg} |
---|
[473] | 999 | \caption{Pedestal S-curves for channel 1 to 16.} |
---|
| 1000 | \label{fig:40} |
---|
| 1001 | \end{figure} |
---|
| 1002 | |
---|
| 1003 | The trigger efficiency was then measured for a |
---|
| 1004 | fixed injected charge of 10~pe. On \refFig{fig:41} are represented the S-curves |
---|
| 1005 | obtained with 200 measurements of the trigger for all channels varying |
---|
| 1006 | the threshold. The homogeneity is proved by a spread of 7 DAC unit (0.4~pe) and a noise of 0.07 pe ($RMS =2.19$). |
---|
| 1007 | |
---|
[474] | 1008 | \begin{figure}[!htbp] |
---|
| 1009 | \centering |
---|
| 1010 | \begin{tabular}{rl} |
---|
| 1011 | \multicolumn{2}{c}{\includegraphics[width=0.5\columnwidth,height=6cm]{img41a.jpg}}\\ |
---|
| 1012 | \includegraphics[width=0.5\columnwidth,height=6cm]{img41b.jpg}& |
---|
| 1013 | \includegraphics[width=0.5\columnwidth,height=6cm]{img41c.jpg} |
---|
| 1014 | \end{tabular} |
---|
[473] | 1015 | \caption{Fast shaper and trigger (top panel); S-curves for input of 10~pe (left panel); |
---|
| 1016 | uniformity plot for channel 1 to 16 (right panel).} |
---|
| 1017 | \label{fig:41} |
---|
| 1018 | \end{figure} |
---|
| 1019 | |
---|
| 1020 | The trigger output is studied also by scanning |
---|
| 1021 | the threshold for a fixed channel and changing the injected charge. On \refFig{fig:42} |
---|
| 1022 | on the left panel is shown the trigger efficiency versus the DAC unit and on |
---|
| 1023 | the right panel is plotted the threshold versus the injected charge but only |
---|
| 1024 | until 0.5~pC. From these measurements a noise of 10~fC has been |
---|
| 1025 | extrapolated. Therefore the threshold is only possible above $10~\sigma$ of the noise due to the discriminator coupling |
---|
| 1026 | (\refFig{fig:43}). |
---|
| 1027 | |
---|
[474] | 1028 | \begin{figure}[!htbp] |
---|
[473] | 1029 | \centering |
---|
[474] | 1030 | \begin{tabular}{rl} |
---|
| 1031 | \includegraphics[width=0.5\columnwidth,height=6cm]{img42a.jpg} |
---|
| 1032 | \includegraphics[width=0.5\columnwidth,height=6cm]{img42b.jpg} |
---|
| 1033 | \end{tabular} |
---|
[473] | 1034 | \caption{Trigger efficiency vs DAC count up to 300~pe (left panel) and |
---|
| 1035 | until 3~pe (right panel).} |
---|
| 1036 | \label{fig:42} |
---|
| 1037 | \end{figure} |
---|
| 1038 | |
---|
[474] | 1039 | \begin{figure}[!htbp] |
---|
[473] | 1040 | \centering |
---|
[474] | 1041 | \includegraphics[width=0.7\columnwidth,height=6cm]{img43.jpg} |
---|
[473] | 1042 | \caption{Threshold vs injected charge up to 500~fC. It is shown the 1~p.e threshold for a PMT gain of $10^6$.} |
---|
| 1043 | \label{fig:43} |
---|
| 1044 | \end{figure} |
---|
| 1045 | |
---|
| 1046 | The trigger coupling illustrated in \refFig{fig:44} with the |
---|
| 1047 | injected charge in channel 1 and output signal observed in channel 2, |
---|
| 1048 | shows a coupling signal around 25~mV (10~fC). This coupling signal is |
---|
| 1049 | due, probably, to the input power supply ($V_{dd-pa}$ and $V_{ss}$). |
---|
| 1050 | |
---|
[474] | 1051 | \begin{figure}[!htbp] |
---|
| 1052 | \includegraphics[width=0.7\columnwidth,height=6cm]{img44.jpg} |
---|
[473] | 1053 | \caption{Trigger coupling signal.} |
---|
| 1054 | \label{fig:44} |
---|
| 1055 | \end{figure} |
---|
| 1056 | |
---|
| 1057 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 1058 | \subsection{ADC characterisation} |
---|
| 1059 | \label{ssec:ADCMeas} |
---|
| 1060 | %%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 1061 | The ADC performance has been studied alone and with the whole chain. Injecting to the |
---|
| 1062 | ADC input directly a DC voltage by the internal DAC, |
---|
| 1063 | in order to have a voltage level as stable as possible, were measured |
---|
| 1064 | the ADC values for all channels (\refFig{fig:45}). |
---|
| 1065 | |
---|
| 1066 | The measurement is repeated 10000 times for |
---|
| 1067 | each channel and in the first plot of the LabView front panel window (\refFig{fig:45}). The |
---|
| 1068 | minimal, maximal and mean values, over all acquisitions, for each |
---|
| 1069 | channel are plotted. In the second plot there is the rms charge value |
---|
| 1070 | versus channel number with a value in the range $[0.5, 1]$ ADC unit. |
---|
| 1071 | Finally the third plot shows an example of charge amplitude |
---|
| 1072 | distribution for a single channel: a spread of 5 ADC counts is |
---|
| 1073 | obtained. |
---|
| 1074 | |
---|
[474] | 1075 | \begin{figure}[!htbp] |
---|
[473] | 1076 | \centering |
---|
[474] | 1077 | \includegraphics[width=0.7\columnwidth,height=6cm]{img45.jpg} |
---|
[473] | 1078 | \caption{ADC measurements with DC input 1.45~V (middle scale).} |
---|
| 1079 | \label{fig:45} |
---|
| 1080 | \end{figure} |
---|
| 1081 | |
---|
| 1082 | The ADC is suited to a multichannel conversion |
---|
| 1083 | so the uniformity and linearity are studied in order to characterize |
---|
| 1084 | the ADC behaviour. On \refFig{fig:46} is represented the ADC transfer function for the |
---|
| 1085 | 10-bit ADC versus the input voltage level. All channels are represented |
---|
| 1086 | and have plots superimposed. |
---|
| 1087 | |
---|
[474] | 1088 | \begin{figure}[!htbp] |
---|
[473] | 1089 | \centering |
---|
[474] | 1090 | \includegraphics[width=0.7\columnwidth,height=6cm]{img46.jpg} |
---|
[473] | 1091 | \caption{10 bits ADC transfer function vs input charge.} |
---|
| 1092 | \label{fig:46} |
---|
| 1093 | \end{figure} |
---|
| 1094 | |
---|
| 1095 | The good homogeneity observed is confirmed by |
---|
| 1096 | the linear fit parameters comparison. In are plotted the slope and the |
---|
| 1097 | intercept distributions for all channels. The RMS slope value of 0.143 |
---|
| 1098 | and the RMS intercept value of 0.3 confirm the 10-bits ADC uniformity |
---|
| 1099 | (\refTab{tab:12}). |
---|
| 1100 | |
---|
[474] | 1101 | \begin{figure}[!htbp] |
---|
[473] | 1102 | \centering |
---|
[474] | 1103 | \begin{tabular}{rl} |
---|
| 1104 | \includegraphics[width=0.5\columnwidth,height=6cm]{img47a.jpg}& |
---|
| 1105 | \includegraphics[width=0.5\columnwidth,height=6cm]{img47b.jpg} |
---|
| 1106 | \end{tabular} |
---|
[473] | 1107 | \caption{Evolution of the fit parameters (slope on the |
---|
| 1108 | left panel and intercept on the right panel) as a function of the channel |
---|
| 1109 | number.} |
---|
| 1110 | \label{fig:47} |
---|
| 1111 | \end{figure} |
---|
| 1112 | |
---|
| 1113 | \begin{table} |
---|
| 1114 | \centering |
---|
| 1115 | \caption{TO BE COMPLETED. 10 bits ADC parameter fits.... 25 acquisitions per channel, $LSB = 1.06$~mV...} |
---|
| 1116 | \label{tab:12} |
---|
| 1117 | \begin{tabular}{|l|c|c|} |
---|
| 1118 | \hline |
---|
| 1119 | & Slope & Intercept \\ |
---|
| 1120 | Mean & 936.17 & 859.8 \\ |
---|
| 1121 | RMS & 0.14 & 0.3 \\ |
---|
| 1122 | \hline |
---|
| 1123 | \end{tabular} |
---|
| 1124 | \end{table} |
---|
| 1125 | |
---|
| 1126 | In \refFig{fig:48} are shown respectively the 12, 10 and 8 bits ADC |
---|
| 1127 | linearity plots with the 25 measurements made for each input voltage |
---|
| 1128 | level. The average ADC count value is plotted versus the input signal. |
---|
| 1129 | The residuals from $-1.5$ to $0.9$ ADC units for the 12-bits ADC; from $-0.5$ |
---|
| 1130 | to $0.4$ for the 10-bit ADC and from $-0.5$ to $0.5$ for the 8-bit ADC. This prove |
---|
| 1131 | the good ADC behaviour in terms of Integral non linearity. |
---|
| 1132 | |
---|
[474] | 1133 | \begin{figure}[!htbp] |
---|
| 1134 | \centering |
---|
| 1135 | \begin{tabular}{c} |
---|
| 1136 | \includegraphics[width=0.7\columnwidth,height=6cm]{img48a.jpg}\\ |
---|
| 1137 | \includegraphics[width=0.5\columnwidth,height=6cm]{img48b.jpg}\\ |
---|
| 1138 | \includegraphics[width=0.5\columnwidth,height=6cm]{img48c.jpg} |
---|
| 1139 | \end{tabular} |
---|
[473] | 1140 | \caption{12, 10, 8 bit ADC linearity.} |
---|
| 1141 | \label{fig:48} |
---|
| 1142 | \end{figure} |
---|
| 1143 | In terms of Differential non linearity, the |
---|
| 1144 | value from $-1.0$ to $0.65$ for the 10 bit ADC and from $-0.3$ to $0.2$ for the 8 |
---|
| 1145 | bit ADC, show us a good behaviour even if the plots are the results of |
---|
| 1146 | preliminary measurements. |
---|
| 1147 | |
---|
[474] | 1148 | \begin{figure}[!htb] |
---|
| 1149 | \centering |
---|
| 1150 | \begin{tabular}{rl} |
---|
| 1151 | \includegraphics[width=0.5\columnwidth,height=6cm]{img49a.jpg} |
---|
| 1152 | \includegraphics[width=0.5\columnwidth,height=6cm]{img49b.jpg} |
---|
| 1153 | \end{tabular} |
---|
[473] | 1154 | \caption{Differential non linearity.} |
---|
| 1155 | \label{fig:49} |
---|
| 1156 | \end{figure} |
---|
| 1157 | |
---|
| 1158 | Once the ADC performances have been tested |
---|
| 1159 | separately, the measurements are performed on the complete chain. The |
---|
| 1160 | results of the input signal autotriggered, held in the T\&H and |
---|
| 1161 | converted in the ADC are illustrated in where are plotted the 10-bit |
---|
| 1162 | ADC counts in function of the variable input charge (up to 50~pe). A |
---|
| 1163 | good linearity of $1.4~\%$ and a noise of 6 ADC units are obtained. In \refTab{tab:13} |
---|
| 1164 | are listed the setting value for measurements. |
---|
| 1165 | |
---|
| 1166 | \begin{table} |
---|
| 1167 | \centering |
---|
| 1168 | \caption{TO BE COMPELTED. $G_{pa}=14$ ($C_{in}=7$~pF , $C_f=0.5$~pF), |
---|
| 1169 | Slow shaper $RC=50$~ns, |
---|
| 1170 | DAC delay: $bit<0> = 1$ \& $bit<2> = 1$. |
---|
| 1171 | } |
---|
| 1172 | \label{tab:13} |
---|
| 1173 | \begin{tabular}{|l|c|c|c|} |
---|
| 1174 | \hline |
---|
| 1175 | Parameters & 12 bits ADC & 10 bits ADC & 8 bits ADC\\ |
---|
| 1176 | \hline |
---|
| 1177 | LSB & $0.27$ & $1.06$~mV & $4.26$~mV\\ |
---|
| 1178 | Min ADC count at 3~pe& $509$ & $132$ & $33$ \\ |
---|
| 1179 | Max ADC count at 50~pe & $3873$ & $989$ & $241$ \\ |
---|
| 1180 | Residuals in ADC units &$[21,54]$ & $[6,14]$ & $[2,3]$ \\ |
---|
| 1181 | \hline |
---|
| 1182 | \end{tabular} |
---|
| 1183 | \end{table} |
---|
| 1184 | |
---|
[474] | 1185 | \begin{figure}[!htbp] |
---|
[473] | 1186 | \centering |
---|
[474] | 1187 | \includegraphics[width=0.7\columnwidth,height=6cm]{img50.jpg} |
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[473] | 1188 | \caption{10 bit ADC linearity.} |
---|
| 1189 | \label{fig:50} |
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| 1190 | \end{figure} |
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| 1191 | |
---|
| 1192 | On \refFig{fig:51} is plotted the 8-bit linearity at $1.4~\%$ |
---|
| 1193 | and a noise of 1.53 ADC unit. In \refTab{tab:13} are listed the setting value for |
---|
| 1194 | measurements. |
---|
| 1195 | |
---|
[474] | 1196 | \begin{figure}[!htbp] |
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[473] | 1197 | \centering |
---|
[474] | 1198 | \includegraphics[width=0.7\columnwidth,height=6cm]{img51.jpg} |
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[473] | 1199 | \caption{8 bit ADC linearity.} |
---|
| 1200 | \label{fig:51} |
---|
| 1201 | \end{figure} |
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| 1202 | |
---|
| 1203 | On \refFig{fig:53} is plotted the 12-bit linearity |
---|
| 1204 | at $1.4~\%$ and a noise of 23.69 ADC unit. In \refTab{tab:13} are listed the setting |
---|
| 1205 | value for measurements. |
---|
| 1206 | |
---|
[474] | 1207 | \begin{figure}[!htbp] |
---|
| 1208 | \centering |
---|
| 1209 | \includegraphics[width=0.7\columnwidth,height=6cm]{img52.jpg} |
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[473] | 1210 | \caption{12 bit ADC linearity.} |
---|
| 1211 | \label{fig:52} |
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| 1212 | \end{figure} |
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| 1213 | |
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| 1214 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
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| 1215 | \section{Measurements with PMTs} |
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| 1216 | \label{sec:MeasWithPMT} |
---|
| 1217 | %%%%%%%%%%%%%%%%%%%%%%%%%%% |
---|
| 1218 | The first measurements with a photomultiplier at input are started in |
---|
| 1219 | IPNO at Orsay. |
---|
| 1220 | |
---|
[474] | 1221 | \begin{figure}[!htbp] |
---|
[473] | 1222 | \centering |
---|
[474] | 1223 | \includegraphics[width=0.7\columnwidth,height=6cm]{img53.jpg} |
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[473] | 1224 | \caption{TO BE COMPLETED} |
---|
| 1225 | \label{fig:53} |
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| 1226 | \end{figure} |
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| 1227 | |
---|
[467] | 1228 | \acknowledgments |
---|
| 1229 | %\begin{acknowledgments} |
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[473] | 1230 | This work, especially one of the author, is supported by the National Reasaerch Agency under contract ANR-06-BLAN-0186. |
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[467] | 1231 | %\end{acknowledgments} |
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[473] | 1232 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
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[467] | 1233 | \newpage |
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[473] | 1234 | %\section*{References} |
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[467] | 1235 | \bibliography{campagne} |
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| 1236 | \end{document} |
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| 1237 | |
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| 1238 | |
---|