<?xml version="1.0" encoding="ISO-8859-1"?><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance">
<front>
<journal-meta>
<journal-id>1562-3823</journal-id>
<journal-title><![CDATA[Revista Boliviana de Física]]></journal-title>
<abbrev-journal-title><![CDATA[Revista Boliviana de Física]]></abbrev-journal-title>
<issn>1562-3823</issn>
<publisher>
<publisher-name><![CDATA[Sociedad Boliviana de Física]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S1562-38232012000400011</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[Remote control and telescope auto-alignment system for multiangle lidar under development at CEILAP, Argentina]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Pallotta]]></surname>
<given-names><![CDATA[Juan V.]]></given-names>
</name>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Ristori]]></surname>
<given-names><![CDATA[Pablo]]></given-names>
</name>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Otero]]></surname>
<given-names><![CDATA[Lidia]]></given-names>
</name>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Gonzalez]]></surname>
<given-names><![CDATA[Francisco]]></given-names>
</name>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Dworniczak]]></surname>
<given-names><![CDATA[Juan Carlos]]></given-names>
</name>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[D’Elia]]></surname>
<given-names><![CDATA[Raul]]></given-names>
</name>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Pawelko]]></surname>
<given-names><![CDATA[Ezequiel]]></given-names>
</name>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Quel]]></surname>
<given-names><![CDATA[Eduardo]]></given-names>
</name>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Argentina B1603ALO Villa Martelli - Buenos Aires UMI-IFAECI-CNRS 3351]]></institution>
<addr-line><![CDATA[ ]]></addr-line>
</aff>
<aff id="A02">
<institution><![CDATA[,Argentina ITeDA (CNEA - CONICET - UNSAM) ]]></institution>
<addr-line><![CDATA[Buenos Aires ]]></addr-line>
<country>Argentina</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>00</month>
<year>2012</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>00</month>
<year>2012</year>
</pub-date>
<volume>20</volume>
<numero>20</numero>
<fpage>30</fpage>
<lpage>32</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.bo/scielo.php?script=sci_arttext&amp;pid=S1562-38232012000400011&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.bo/scielo.php?script=sci_abstract&amp;pid=S1562-38232012000400011&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.bo/scielo.php?script=sci_pdf&amp;pid=S1562-38232012000400011&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="en"><p><![CDATA[At CEILAP (CITEDEF-CONICET), a multiangle Raman lidar is under development to monitor aerosol extinction in the frame of the CTA (Cherenkov Telescope Array) Project. This is an initiative to build the next generation of ground-based instruments to collect very high energy gamma-ray radiation. It will serve as an open observatory for a wide astrophysics community and will explore the Universe in depth in Very High Energy (> 10 GeV) gamma-rays. The atmospheric conditions are is a major interest for CTA, and this instrument plays a major role measuring the atmospheric optical depth. The reception system is made by six 40 cm in diameter Newtonian telescopes, totally exposed to the hard environmental condition during the shifts. These working conditions could produce misalignments between laser and telescopes, losing the required overlap. To avoid that, a telescope controlled by a self-alignment system is under development to solve this problem. This is performed by PC software running from the acquisition module which is connected via ethernet to a microcontroller. This paper, describes the self-alignment method and hardware work in progress.]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[multiangle lidar]]></kwd>
<kwd lng="en"><![CDATA[Raman]]></kwd>
<kwd lng="en"><![CDATA[CTA observatory]]></kwd>
<kwd lng="en"><![CDATA[aerosols]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[ <p align="center"><font size="4" face="Verdana"><strong>Remote control and telescope auto-alignment system for   multiangle lidar under development at CEILAP, Argentina</strong></font></p>     <p align="center">&nbsp;</p>     <p align="center"><strong><font size="3" face="Verdana">Juan   V. Pallotta, Pablo Ristori, Lidia Otero, Francisco Gonzalez, Juan Carlos   Dworniczak, Raul D’Elia, Ezequiel Pawelko, Eduardo Quel.</font></strong></p>     <p align="center"><strong><font size="2" face="Verdana">CEILAP   (CITEDEF-CONICET), UMI-IFAECI-CNRS 3351</font></strong></p>     <p align="center"><strong><font size="2" face="Verdana">Juan   B. de La Salle 4397, B1603ALO Villa Martelli – Buenos Aires, Argentina. E-mail:   jpallotta@citedef.gob.ar</font></strong></p>     <p align="center"><strong><font size="2" face="Verdana">Alberto   Etchegoyen</font></strong></p>     <p align="center"><strong><font size="2" face="Verdana">ITeDA   (CNEA – CONICET - UNSAM)</font></strong></p>     <p align="center"><strong><font size="2" face="Verdana">Av.   Gral. Paz 1499 - 1650 San Martín – Buenos Aires, Argentina.</font><font size="2" face="Verdana"></font></strong></p><hr>     <p><font size="2" face="Verdana">At CEILAP (CITEDEF-CONICET), a   multiangle Raman lidar is under development to monitor aerosol extinction in   the frame of the CTA (Cherenkov Telescope Array) Project. This is an initiative   to build the next generation of ground-based instruments to collect very high   energy gamma-ray radiation. It will serve as an open observatory for a wide   astrophysics community and will explore the Universe in depth in Very High   Energy (&gt; 10 GeV) gamma-rays. The atmospheric conditions are is a major   interest for CTA, and this instrument plays a major role measuring the   atmospheric optical depth.</font></p>     <p><font size="2" face="Verdana">The reception system is made by six   40 cm in diameter Newtonian telescopes, totally exposed to the hard   environmental condition during the shifts. These working conditions could   produce misalignments between laser and telescopes, losing the required   overlap. To avoid that, a telescope controlled by a self-alignment system is   under development to solve this problem. This is performed by PC software   running from the acquisition module which is connected via ethernet to a   microcontroller. This paper, describes the self-alignment method and hardware   work in progress.</font></p>     ]]></body>
<body><![CDATA[<p><font size="2" face="Verdana"><b>Key words: </b>multiangle lidar, Raman, CTA observatory, aerosols.</font></p><hr>     <p><font size="2" face="Verdana"><b>INTRODUCTION</b></font></p>     <p><font size="2" face="Verdana">The Cherenkov Telescope Array   Consortium (CTA) contemplates the design, construction and the operation of two   observatories for the detection of gamma-ray produced by extraterrestrial   sources at energies range between 1010 eV to 1014 eV. These observatories will be deployed at each   hemisphere for full sky-map coverage. Each Observatory will consist of a   telescope array sensitive to the atmospheric generated Cherenkov radiation that   will improve the performance of the actual detectors. The objectives proposed   for CTA will be attained using an array of multiple telescopes distributed over   a surface of 1 km2, located at sites with excellent optical and   atmospheric conditions at a height of 2000 to 3500 mts above the sea level. The   comprehension of the atmospheric conditions during the measurements is   extremely important for the CTA Observatory. In fact, the atmosphere acts as   the first detector at which the air showers are developed. The array of   detectors observe the gamma ray induced cascades by measuring the Cherenkov   light produced by their charged particles moving above the speed of light of   the surrounding atmosphere. The emitted light is attenuated from the source to   the telescope due to molecular, aerosol and cloud extinction. Lidars play a   leading role in monitoring of sky conditions, by both detecting the overall   cloud coverage and measuring the atmospheric opacity due to aerosol and clouds   over the Observatory. The location of this astronomical facility will be   selected after a careful study of the preselected zones, regarding the latitude,   altitude, the atmospheric conditions, and the available local infrastructure.   At the Southern hemisphere, Argentina is one of the candidate countries for the installation of the CTA Observatory.   The places proposed are “El Leoncito”, located in San Juan state and “El   CASLEO”, in Salta.</font></p>     <p><font size="2" face="Verdana"><b>LIDAR HARDWARE</b></font></p>     <p><font size="2" face="Verdana">LIDAR telescope is planned to be   mounted on a steerable frame, and moved using two DC servomotors, reading its   position by two relative encoders.</font></p>     <p><font size="2" face="Verdana"><img width=215 height=163 id="Imagen 1" src="/img/revistas/rbf/v20n20/v20n20a11-image001.png"></font></p>     <p><font size="2" face="Verdana">Figure 1. A preliminary sketch of the multiangle lidar   under construction.</font></p>     <p><font size="2" face="Verdana">Movements are handled by a microcontroller that communicates with   the lidar PC through an ethernet connection. Each LIDAR is equipped with a   Nd:Yag laser, that generates laser pulses at 355, 532 and 1064 nm at a   repetition rate of 50 Hz and a pulse energy of ~20 mJ @ 355 nm. The   backscattered light is collected by six Newtonian telescopes with 40 cm   diameter, 1 m focal length. A multiwavelength   spectrometer separates the backscattered wavelengths and concentrates the light   into several Hamamatsu H6780 photomultipliers. A Licel TR20-160 module is used   to digitalize and store the lidar profiles</font></p>     <p><font size="2" face="Verdana">This lidar has special requirements:</font></p>     <p><font size="2" face="Verdana">&#149; It has to be   able to be operated remotely. The lidar operator may not have an a priori   knowledge on lidar techniques.</font></p>     ]]></body>
<body><![CDATA[<p><font size="2" face="Verdana">&#149;Telescopes,   mechanics and electronics, will be exposed during nighttime to extreme   environmental conditions (wind burst, temperature span, etc.), which could   produce lidar misalignments</font></p>     <p><font size="2" face="Verdana">These are the main reasons that   encourage the development of a fully automatic alignment system is to keep the   telescopes aligned during the acquisition period.</font></p>     <p><font size="2" face="Verdana"><b>LIDAR COMUNICATIONS</b></font></p>     <p><font size="2" face="Verdana">The lidar system under development   has two operational modes: <i>local mode </i>and <i>remote mode</i>. <i>Local   mode </i>was developed for maintenance procedures. The presence of a lidar   technician is required on site to perform hardware improvements and specific   tests. <i>Remote mode </i>was programmed to perform shift operations. In this   case the lidar will be remotely operated and monitored from the control center.   The lidar computer was designed to communicate with control center server   wirelessly via a WiFi link, creating a local lidar network under the TCP/IP   protocol.</font></p>     <p><font size="2" face="Verdana"><img width=283 height=195 id="Imagen 2" src="/img/revistas/rbf/v20n20/v20n20a11-image002.png"></font></p>     <p><font size="2" face="Verdana">Figure 2. A general schematic layout of the lidar communication   system. If remote mode is set, the shifter can monitor and control all the   operations.</font></p>     <p><font size="2" face="Verdana">At the link endpoints, several processes communicate with   each other to send/receive control and monitoring messages.</font></p>     <p><font size="2" face="Verdana">LIDAR   SOFTWARE</font></p>     <p><font size="2" face="Verdana">A more detailed view of the process at each lidar PC can be   seen on Figure 3. Each computer works under Linux operating system and all the   software was developed in C/C++. A socket-based IPC (Inter Process   Communication) was programed to communicate the local with the remote process.   To increase their efficiency, each process is totally independent, and   communicates to the other via control messages.</font></p>     <p><font size="2" face="Verdana"><img width=307 height=199 id="Imagen 3" src="/img/revistas/rbf/v20n20/v20n20a11-image003.png"></font></p>     ]]></body>
<body><![CDATA[<p><font size="2" face="Verdana"><b>Figure 3. A general diagram about   connections in both sides of the lidar system.</b></font></p>     <p><font size="2" face="Verdana">A brief description of each process   at both sides of the link is described below:</font></p>     <p><font size="2" face="Verdana"><b>Lidar PC side (client):</b></font></p>     <p><font size="2" face="Verdana"><b><i>adq</i></b>: Is the main process at the client (lidar) side. It   controls the acquisition timing, it communicates with the laser, it triggers   the Licel, it sends the acquired new file to the <i>plot </i>process, and, if   necessary, to the <i>alignment </i>process.</font></p>     <p><font size="2" face="Verdana"><b><i>plot</i></b>: Waits messages from the <i>adq </i>process, conformed   mainly by the new acquired file path and shows it on the display. <b><i>comToServ</i></b>:   This process handle all the messages from/to the client/server side.</font></p>     <p><font size="2" face="Verdana"><b><i>alignment</i></b>: This process receive the path to the acquired file   from <i>adq </i>and process this signal to obtain the alignment parameters to   determine the telescope position.</font></p>     <p><font size="2" face="Verdana"><b>Control PC side (server):</b></font></p>     <p><font size="2" face="Verdana"><b><i>mainServ</i></b>: Handle the communication between the shifter and the   client PC.</font></p>     <p><font size="2" face="Verdana"><b><i>plot</i></b>: Shows the lidar signal from the last saved file.</font></p>     <p><font size="2" face="Verdana"><b>MICROCONTROLLER-</b></font><font size="2" face="Verdana"><b>CONTROLLED TELESCOPES</b></font></p>     ]]></body>
<body><![CDATA[<p><font size="2" face="Verdana">The tilt angle of the telescopes is   driven by a set of stepper motors, handled by a RCM2200 Rabbit System   microcontroller. This is Z80 family-based high-performance 8 bit   microcontroller. It has a built-in Ethernet interface with an integrated TCP/IP   stack, making it a good choice for interconnectivity. This interface is used to   link the microcontroller with the lidar PC. The instruction set is based on the   original Z80 microprocessor, with some additional instructions.</font></p>     <p><font size="2" face="Verdana">The aims of the Rabbit   microcontroller algorithm is to decode the Ethernet information received from   the lidar PC <i>alignment </i>process, and to handle the signals to correct the   stepper motor drivers. The message from the lidar PC to the Rabbit   microcontroller has 3 parameters: motor to be controlled, direction and number   of steps. Therefore, the firmware of the Rabbit microcontroller is a “dummy   terminal” that only receives message and drives the motor. After that, it sends   an acknowledge message back to the <i>alignment </i>process.</font></p>     <p><font size="2" face="Verdana"><b>ALIGNMENT ALGORITHM</b></font></p>     <p><font size="2" face="Verdana">The alignment algorithm is a   cooperative procedure between the <i>adq </i>and the <i>alignment </i>processes,   both running on the lidar PC, and a firmware recorded in the Rabbit microcontroller.</font></p>     <p><font size="2" face="Verdana">When the alignment mode is set at the <i>adq </i>process, each path of the acquired file is sent to <i>alignment</i>.   Moreover, after saving a new file at the lidar PC, this file is transferred to   the control PC for a backup. A summarized procedure flowchart can be seen on   Figure 5.</font></p>     <p><font size="2" face="Verdana"><img width=307 height=216 id="Imagen 4" src="/img/revistas/rbf/v20n20/v20n20a11-image004.png"></font></p>     <p><font size="2" face="Verdana"><b>Figure 4. Communication Diagram   between the <i>acquisition </i>and the <i>alignment </i>processes. Both are   fully independent, and they communicate via the IPC socket, implemented under   C/C++.</b></font></p>     <p><font size="2" face="Verdana">The aim of the alignment algorithm   is to quantify the alignment state of the recently acquired file and to save it   with its tilt position in a table. After that, <i>alignment </i>tilts the   telescope to a new position and sends an acknowledge message to <i>acq</i>, to   trigger new acquisition.</font></p>     <p><font size="2" face="Verdana">The alignment state quantification   is obtained by accumulating the lidar signal over certain range, as it seen on   the next figure:</font></p>     <p><font size="2" face="Verdana"><img width=327 height=212 id="Imagen 5" src="/img/revistas/rbf/v20n20/v20n20a11-image005.png"></font></p>     ]]></body>
<body><![CDATA[<p><font size="2" face="Verdana">Figure 5. After finishing the scanning process, the   microcontroller sets the telescope position to the one at wich the maximum   value was attained. This procedure tends to increase the lidar signal in a wide   dynamic range.</font></p>     <p><font size="2" face="Verdana">FIRST RESULTS</font></p>     <p><font size="2" face="Verdana">This algorithm was successfully tested, comparing the   vertical lidar signals obtained with the ones obtained by the MWRL lidar at   CEILAP (CITEDEF-CONICET). The test was done for a vertical fixed position, as   can be seen on Figure 4.</font></p>     <p><font size="2" face="Verdana">The CEILAP’s telescope was manually aligned to provide the   reference signal. The tested telescope was left intentionally misaligned to   test the optimization algorithm.</font></p>     <p><font size="2" face="Verdana"><img width=327 height=152 id="Imagen 6" src="/img/revistas/rbf/v20n20/v20n20a11-image006.png"></font></p>     <p><font size="2" face="Verdana"><b>Figure 4. Picture of the setup of   lidar intercomparison.</b></font></p>     <p><font size="2" face="Verdana">After turning on the alignment mode,   the algorithm exhibited good results, approaching the telescope's signal under   test to the reference lidar signal. The next figure shows the lidar signals   after the alignment process.</font></p>     <p><font size="2" face="Verdana"><img width=267 height=174 id="Imagen 7" src="/img/revistas/rbf/v20n20/v20n20a11-image007.png"></font></p>     <p><font size="2" face="Verdana">Figure 5. Picture of the lidar signals intercomparison after   alignment algorithm success.</font></p>     <p><font size="2" face="Verdana">The differences seen on the last   figure are due to the different distance to the laser source of the systems.   Figure 5 shows the long range agreement of the signals.</font></p>     ]]></body>
<body><![CDATA[<p><font size="2" face="Verdana"><b>CONCLUSIONS</b></font></p>     <p><font size="2" face="Verdana">The system is ready to be tested in   a slant path fixed angle. The lidar is actually being installed inside a   container to perform this new test. A new enhanced version of the controlled   telescope actuators is under construction. First measurements indicate that it   will be possible to achieve the expected auto-optimizations goals during the   scanning procedure. The new software for a multiangle lidar prototype is fully   operational.</font></p>     <p><font size="2" face="Verdana"><b>ACKNOWLEDGMENTS</b></font></p>     <p><font size="2" face="Verdana">Authors wish to thank JICA, ANCyPT,   the CITEFA main workshop’s technicians and José Luis Luque from the CEILAP   workshop for their support on this development.</font></p>     <p><font size="2" face="Verdana"><b>REFERENCES</b></font></p>     <!-- ref --><p><font size="2" face="Verdana">1.- Otero, L. A. <i>et al. </i>(2004).   First Aerosol Measurements with a Multiwavelength LIDAR System at Buenos Aires,   Argentina Proceedings of the Conference of the ILRC2004.</font>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=229460&pid=S1562-3823201200040001100001&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p><font size="2" face="Verdana">2.- http://www.digi.com/   http://www.cta-observatory.com/, <u>http://astrum.frm.utn.edu.ar/CTA-Argentina</u></font>/ <font size="2" face="Verdana">Licel programing examples and   documentation: http://www.licel.com/soft_tcp.html</font>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=229461&pid=S1562-3823201200040001100002&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --> ]]></body><back>
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<source><![CDATA[First Aerosol Measurements with a Multiwavelength LIDAR System at Buenos Aires: Argentina Proceedings of the Conference of the ILRC2004]]></source>
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</article>
