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    <subfield code="a">UFOs ("Unidentified Falling Objects") are expected to be one of the major known performance limitation of the LHC. In this MD, the production mechanism and the dynamics of UFOs at the injection kicker magnets (MKIs) and the tune kicker magnets (MKQs) were studied. This was done by pulsing the MKIs and MKQs on a gap in the partly filled machine.  During the MD, in total 58 UFO-type beam loss patterns were observed directly after pulsing the MKIs. None were observed after pulsing the MKQs, which provides important input for possible mitigation strategies. The temporal and spatial distribution of the UFO events could be determined by using a dedicated BLM Study Buffer, the implications for the UFO dynamics are discussed.</subfield>
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    <subfield code="u">http://cds.cern.ch/record/1421594/files/CERN-ATS-Note-2012-018 MD.pdf</subfield>
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    <subfield code="a">MD on UFOs at MKIs and MKQs</subfield>
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    <subfield code="a">10.1111/j.1745-3933.2012.01221.x</subfield>
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    <subfield code="u">http://export.arxiv.org/oai2</subfield>
    <subfield code="d">2015-06-03</subfield>
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    <subfield code="a">Evidence for ultra-fast outflows in radio-quiet AGNs: III - location and energetics</subfield>
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    <subfield code="c">10 Jan 2012</subfield>
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    <subfield code="a">Comments: 5 pages, 3 figures, accepted for publication in MNRAS</subfield>
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    <subfield code="a">Comments: 5 pages, 3 figures, accepted for publication in MNRAS</subfield>
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    <subfield code="a">Using the results of a previous X-ray photo-ionization modelling of blue-shifted Fe K absorption lines on a sample of 42 local radio-quiet AGNs observed with XMM-Newton, in this letter we estimate the location and energetics of the associated ultra-fast outflows (UFOs). Due to significant uncertainties, we are essentially able to place only lower/upper limits. On average, their location is in the interval ~0.0003-0.03pc (~10^2-10^4 r_s) from the central black hole, consistent with what is expected for accretion disk winds/outflows. The mass outflow rates are constrained between ~0.01-1 M_{\odot} yr^{-1}, corresponding to >5-10% of the accretion rates. The average lower-upper limits on the mechanical power are log\dot{E}_K~42.6-44.6 erg s^{-1}. However, the minimum possible value of the ratio between the mechanical power and bolometric luminosity is constrained to be comparable or higher than the minimum required by simulations of feedback induced by winds/outflows. Therefore, this work demonstrates that UFOs are indeed capable to provide a significant contribution to the AGN cosmological feedback, in agreement with theoretical expectations and the recent observation of interactions between AGN outflows and the interstellar medium in several Seyferts galaxies.</subfield>
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    <subfield code="a">Reeves, J N</subfield>
    <subfield code="u">Keele University</subfield>
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    <subfield code="a">Braito, V</subfield>
    <subfield code="u">Leicester University</subfield>
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    <subfield code="a">Ramirez, J M</subfield>
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    <subfield code="a">On the X-ray low- and high-velocity outflows in AGNs</subfield>
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    <subfield code="c">24 Oct 2011</subfield>
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    <subfield code="a">Comments: Accepted for publication as a Letter to the Editor in Monthly Notices of the Royal Astronomical Society Letters</subfield>
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    <subfield code="a">Comments: Accepted for publication as a Letter to the Editor in Monthly Notices of the Royal Astronomical Society Letters</subfield>
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    <subfield code="a">An exploration of the relationship between bolometric luminosity and outflow velocity, for two classes of X-ray outflows in a large sample of active galactic nuclei has been performed. We find that line radiation pressure could be one physical mechanism that might accelerate the gas we observe in warm absorber, v~100-1000 km/s, and on comparable but less stringent grounds the ultra-fast outflows (UFOs), v~0.03-0.3c. If comparable with the escape velocity of the system; the first is naturally located at distances of the dusty torus, ~ 1 pc, and the second at sub-parsec scales, ~ 0.01 pc, in accordance with large set of observational evidence existing in the literature. The presentation of this relationship might give us key clues for our understanding of the different physical mechanisms acting in the center of galaxies, the feedback process and its impact on the evolution of the host galaxy.</subfield>
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    <subfield code="a">10.1088/0004-637X/742/1/44</subfield>
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    <subfield code="a">Evidence for ultra-fast outflows in radio-quiet AGNs: II - detailed photo-ionization modeling of Fe K-shell absorption lines</subfield>
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    <subfield code="c">2011</subfield>
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    <subfield code="a">Comments: Accepted for publication in ApJ</subfield>
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    <subfield code="a">Comments: Accepted for publication in ApJ</subfield>
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    <subfield code="a">X-ray absorption line spectroscopy has recently shown evidence for previously unknown Ultra-fast Outflows (UFOs) in radio-quiet AGNs. In the previous paper of this series we defined UFOs as those absorbers with an outflow velocity higher than 10,000km/s and assessed the statistical significance of the associated blueshifted FeK absorption lines in a large sample of 42 local radio-quiet AGNs observed with XMM-Newton. In the present paper we report a detailed curve of growth analysis and directly model the FeK absorbers with the Xstar photo-ionization code. We confirm that the frequency of sources in the radio-quiet sample showing UFOs is >35%. The outflow velocity distribution spans from \sim10,000km/s (\sim0.03c) up to \sim100,000km/s (\sim0.3c), with a peak and mean value of \sim42,000km/s (\sim0.14c). The ionization parameter is very high and in the range log\xi 3-6erg s^{-1} cm, with a mean value of log\xi 4.2 erg s^{-1} cm. The associated column densities are also large, in the range N_H\sim10^{22}-10^{24} cm^{-2}, with a mean value of N_H\sim10^{23} cm^{-2}. We discuss and estimate how selection effects, such as those related to the limited instrumental sensitivity at energies above 7keV, may hamper the detection of even higher velocities and higher ionization absorbers. We argue that, overall, these results point to the presence of extremely ionized and possibly almost Compton thick outflowing material in the innermost regions of AGNs. This also suggests that UFOs may potentially play a significant role in the expected cosmological feedback from AGNs and their study can provide important clues on the connection between accretion disks, winds and jets.</subfield>
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    <subfield code="b">&lt;p class="articleHeader"> &lt;!--HTML-->After more than two months since its stop in December, the LHC is slowly coming back from its hibernation - even if the temperature of the magnets in the tunnel has actually been getting lower and lower in recent days. The tunnel has been crowded with hundreds of people, busy with maintenance activities and preparations for the restart. The end of most activities (and the access to the tunnel) is scheduled for 21 February. On this date, the Operations team will take back ownership of the machine from the Programmed Stops Coordination team and push forward the preparations for the beam.&lt;/p> &lt;p> &amp;nbsp;&lt;/p> &lt;p> The cool-down of all LHC sectors (left floating at around 80 K during the Christmas break) restarted three weeks ago. At present, more than half of the machine is at nominal cryogenic temperature and the completion of the cool-down is expected by 27 February. As soon as a sector is cold, the Electrical Quality Assurance (ElQA) team starts the high-voltage qualification of the superconducting circuits, to check insulation and instrumentation integrity. These qualifications were initiated on the first Sector available (Sector 23) during the Charmonix workshop week, and have since been carried out on three other Sectors (Sectors 56,&amp;nbsp; 67 and 78) without any non-conformity being found.&lt;/p> &lt;p> &lt;br /> Once the circuits have undergone the high-voltage qualification, the powering tests of the superconducting circuits begin. These tests officially started on 10 February, after the validation and preparation of the first sector. To minimize the impact on the activities requiring access to the tunnel (which will continue for a few more days), the powering tests are only being performed during the evening and at night, to cope with the safety constraints. These tests aim at pushing the performance of all LHC circuits to their operational level. The tests involve injecting current through the superconducting circuits while checking the correct behaviour of the protection mechanisms, an essential element for the safe operation of the machine. After operating at 3.5 TeV for two years, the LHC is entering another domain, with the main dipole and quadrupole circuits powered at a different current level for operation at 4 TeV.&lt;/p> &lt;p> &lt;br /> Apart from some small issues and debugging (also of the new tools used this year to improve the performance in test execution), as at the beginning of each restart after a long stop, the tests are progressing well. All superconducting circuits should be commissioned during the first week of March. A few days of machine check-out will then drive us to the first beam, planned for 14 March.&lt;/p> &lt;p style="text-align: right;"> &lt;em>Mirko Pojer for the LHC Team&lt;/em>&lt;/p> &lt;hr /> &lt;p style="text-align: center;"> &lt;strong>LHC performance workshop summary&lt;/strong>&lt;/p> &lt;p> &lt;em>The Chamonix workshop last week reviewed the performance of the LHC in 2011 and discussed plans for 2012 and beyond. Among other things, we can look forward to the LHC running at 4 TeV during 2012.&lt;/em>&lt;/p> &lt;p> &lt;b>A critical review of 2011&lt;/b>&lt;/p> &lt;p> The performance of the machine was examined during the workshop, identifying possible improvements to critical systems such as beam instrumentation and machine protection. The high-intensity beams that the LHC collided last year have raised issues around the ring including beam-induced heating of some hardware, and problematic vacuum spikes. The present understanding of these problems and possible solutions were presented.&lt;/p> &lt;p> One of the big successes of 2011 was the squeeze - the reduction of the beam size at the interaction point - that was pushed in the latter part of the year. Squeezing even further in 2012 might be possible in combination with the use of tighter collimator settings. This could give a peak luminosity of around 6x10&lt;sup>33&lt;/sup> cm&lt;sup>-2&lt;/sup>s&lt;sup>-1&lt;/sup> compared with a maximum of 3.6x10&lt;sup>33&lt;/sup> cm&lt;sup>-2&lt;/sup>s&lt;sup>-1&lt;/sup> in 2011.&lt;/p> &lt;p> &lt;b>&lt;strong>Possibilities for 2012&lt;/strong>&lt;/b>&lt;/p> &lt;p> Steve Myers, CERN&amp;#39;s Director for Accelerators and Technology, presented a summary of the workshop recommendations for the 2012 run. In brief, the LHC should operate at 4 TeV, with the key priorities being: delivering enough luminosity (of the order of 15 fb&lt;sup>-1&lt;/sup>) to ATLAS and CMS to allow them to independently discover or exclude the Higgs; the proton-lead ion run; and a machine development programme that targets operation after the long technical shutdown. A run extension was not ruled out if necessary to meet the target integrated luminosity.&lt;/p> &lt;p> Machine availability should be improved in 2012 thanks to a number of mitigation measures taken during the Christmas stop. These include a number of measures aimed at reducing the effects of radiation on the electronics situated in the LHC tunnel.&lt;/p> &lt;p> &lt;b>&lt;strong>Plans for the long shutdown of 2013/2014&lt;/strong>&lt;/b>&lt;/p> &lt;p> The total length of the long shutdown (LS1) for the LHC is provisionally around 20 months. The main focus will be the splice consolidation work, which involves opening every magnet interconnect in the ring, and measuring carefully the resistance of each joint in the cables which carry the current between the dipoles and quadrupoles in the arcs of the LHC. It is currently estimated that 15% of the splices will be re-done; shunts and clamps will be installed across each splice. The aim is to definitively exclude the possibility of a repeat of the incident of 19 September 2008 at the highest energies expected at the LHC.&lt;/p> &lt;p> Besides this, each of the LHC experiments has extensive programs of maintenance and upgrades. Some of the key LHC systems (cryogenics, vacuum, quench protection, electrical distribution, cooling, ventilation, access and RF) will undergo major maintenance and improvements.&lt;/p> &lt;p> &lt;b>&lt;strong>The machine after LS1&lt;/strong>&lt;/b>&lt;/p> &lt;p> After LS1, a large number of re-training quenches of the LHC dipoles will be required in order to reach the nominal energy of 7 TeV per beam. Therefore, the beam energy in the first years after LS1 is expected to be around 6.5 TeV. The planned injector upgrades will not have been deployed at this stage, but the injector performance still looks capable of supplying sufficient beam quality to enable the LHC to reach the design luminosity of 1x10&lt;sup>34&lt;/sup> cm&lt;sup>-2&lt;/sup>s&lt;sup>-1&lt;/sup>. Potential limitations to post-LS1 performance (quenches, radiation to electronics, UFOs) were also considered.&lt;/p> &lt;p> &lt;b>&lt;strong>Future projects&lt;/strong>&lt;/b>&lt;/p> &lt;p> Prospects for the LHC Injector Upgrade project and its principal client, the High-Luminosity LHC (HL-LHC), were also considered. Tentatively scheduled to start operation around 2023, HL-LHC aims to provide an ambitious 200 to 300 inverse femtobarns per year. An examination of the challenges of the HL-LHC included a look at the state of R&amp;D for the new magnets required for the high-luminosity interaction regions.&lt;/p> &lt;p> There was also an entertaining look at the even more distant future. Possible future projects under consideration include the Large Hadron electron Collider (LHeC), which involves colliding 60 GeV electrons with 7 TeV protons, and the High Energy LHC (HE-LHC), in which the beam energy of the LHC is increased from 7 to 16.5 TeV. Serious technological challenges exist for both these options.&lt;/p> &lt;hr /> &lt;p> Steve Myers, CERN Director for Accelerators and Technology, and Sergio Bertolucci, CERN Director for Research, discuss the Chamonix workshop:&lt;/p> &lt;p> &lt;script language="javascript" src="/insertplayer.js" type="text/javascript">&lt;/script>&lt;script type="text/javascript"> var flash_video_player=get_video_player_path(); insert_player_for_external('Video/Public/Movies/2012/CERN-MOVIE-2012-011/CERN-MOVIE-2012-011-0753-kbps-640x360-25-fps-audio-64-kbps-44-kHz-stereo', 'mms://mediastream.cern.ch/MediaArchive/Video/Public/Movies/2012/CERN-MOVIE-2012-011/CERN-MOVIE-2012-011-0480-kbps-512x288-25-fps-audio-128-kbps-48-kHz-stereo.wmv', 'false', 480, 360, 'https://mediastream.cern.ch/MediaArchive/Video/Public/Movies/2012/CERN-MOVIE-2012-011/CERN-MOVIE-2012-011-posterframe-640x360-at-10-percent.jpg', '1423359', true, 'Video/Public/Movies/2012/CERN-MOVIE-2012-011/CERN-MOVIE-2012-011-0600-kbps-maxH-360-25-fps-audio-128-kbps-48-kHz-stereo.mp4'); &lt;/script>&lt;/p></subfield>
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    <subfield code="b">&lt;p> &lt;!--HTML-->&lt;/p> &lt;p class="articleHeader"> Apr&amp;egrave;s un arr&amp;ecirc;t de plus de deux mois, le LHC se r&amp;eacute;veille doucement de son hibernation - m&amp;ecirc;me si la temp&amp;eacute;rature des aimants dans le tunnel est de plus en plus basse. Le tunnel a &amp;eacute;t&amp;eacute; pris d&amp;rsquo;assaut par des centaines de personnes, occup&amp;eacute;es par la maintenance et la pr&amp;eacute;paration pour le red&amp;eacute;marrage. La fin de la plupart des activit&amp;eacute;s (et de l&amp;#39;acc&amp;egrave;s au tunnel) est pr&amp;eacute;vue pour le 21 f&amp;eacute;vrier. &amp;Agrave; cette date, le groupe Op&amp;eacute;rations reprendra possession de la machine, apr&amp;egrave;s l&amp;#39;&amp;eacute;quipe de Coordination des arr&amp;ecirc;ts techniques, et avancera dans la pr&amp;eacute;paration du faisceau.&lt;/p> &lt;p> &amp;nbsp;&lt;/p> &lt;p> Le refroidissement de tous les secteurs du LHC (qui &amp;eacute;taient &amp;agrave; environ 80 K pendant la pause de No&amp;euml;l) a red&amp;eacute;marr&amp;eacute; il y a trois semaines. &amp;Agrave; l&amp;#39;heure actuelle, plus de la moiti&amp;eacute; de la machine est &amp;agrave; la temp&amp;eacute;rature cryog&amp;eacute;nique nominale, et l&amp;#39;ach&amp;egrave;vement du refroidissement est pr&amp;eacute;vu d&amp;#39;ici au 27 f&amp;eacute;vrier. D&amp;egrave;s qu&amp;#39;un secteur est froid, l&amp;#39;&amp;eacute;quipe d&amp;rsquo;Assurance de la qualit&amp;eacute; &amp;eacute;lectrique (ElQA) commence la qualification &amp;agrave; haute tension des circuits supraconducteurs, pour v&amp;eacute;rifier l&amp;#39;int&amp;eacute;grit&amp;eacute; de l&amp;#39;isolation et de l&amp;#39;instrumentation. Elle a commenc&amp;eacute; ces qualifications pendant la semaine de r&amp;eacute;union de Chamonix sur le premier secteur disponible (secteur 23), et a depuis r&amp;eacute;alis&amp;eacute; trois autres secteurs (secteurs 56, 67 et 78), sans constater aucune non-conformit&amp;eacute;.&lt;br /> &lt;br /> Une fois que les circuits sont qualifi&amp;eacute;s &amp;agrave; haute tension par l&amp;#39;&amp;eacute;quipe ElQA, les tests d&amp;rsquo;alimentation des circuits supraconducteurs commencent. Ces tests ont donc commenc&amp;eacute; le vendredi 10, apr&amp;egrave;s validation et pr&amp;eacute;paration du premier secteur. Pour minimiser l&amp;#39;impact sur les activit&amp;eacute;s n&amp;eacute;cessitant un acc&amp;egrave;s au tunnel (toujours en cours pour quelques jours), les tests en puissance sont &amp;agrave; pr&amp;eacute;sent effectu&amp;eacute;s seulement durant la soir&amp;eacute;e et la nuit, pour satisfaire les exigences de s&amp;eacute;curit&amp;eacute;. Les tests visent &amp;agrave; pousser les circuits du LHC &amp;agrave; leur niveau op&amp;eacute;rationnel en leur injectant du courant et en s&amp;rsquo;assurant en m&amp;ecirc;me temps du comportement conforme des m&amp;eacute;canismes de protection, &amp;eacute;l&amp;eacute;ments essentiels pour le bon fonctionnement de la machine. Apr&amp;egrave;s les deux ann&amp;eacute;es d&amp;#39;op&amp;eacute;ration &amp;agrave; 3,5 TeV, le LHC entrera dans un autre domaine. En effet, les circuits dip&amp;ocirc;les et quadrip&amp;ocirc;les principaux seront aliment&amp;eacute;s par un courant plus &amp;eacute;lev&amp;eacute; pour un fonctionnement &amp;agrave; 4 TeV.&lt;br /> &lt;br /> Hormis quelques petits probl&amp;egrave;mes (principalement au niveau des logiciels et des nouveaux outils utilis&amp;eacute;s cette ann&amp;eacute;e pour am&amp;eacute;liorer la performance dans l&amp;#39;ex&amp;eacute;cution des tests), comme nous le constatons au d&amp;eacute;but de chaque red&amp;eacute;marrage apr&amp;egrave;s un long arr&amp;ecirc;t, les essais sont en bonne voie et tous les circuits supraconducteurs devraient &amp;ecirc;tre mis en service au cours de la premi&amp;egrave;re semaine de mars. Quelques jours de contr&amp;ocirc;le de la machine nous conduiront au premier faisceau, pr&amp;eacute;vu pour le 14 mars.&lt;/p> &lt;p style="text-align: right;"> &lt;em>Mirko Pojer pour l&amp;#39;&amp;eacute;quipe du LHC&lt;/em>&lt;/p> &lt;hr /> &lt;p style="text-align: center;"> &lt;strong>R&amp;eacute;sum&amp;eacute; de l&amp;#39;atelier sur les performances du LHC&lt;/strong>&lt;/p> &lt;p> &lt;em>L&amp;rsquo;atelier de Chamonix, qui s&amp;rsquo;est tenu la semaine derni&amp;egrave;re, a permis d&amp;#39;analyser les performances du LHC en 2011 et de discuter des projets pour 2012 et au-del&amp;agrave;. En particulier, nous nous r&amp;eacute;jouissons &amp;agrave; la perspective d&amp;rsquo;une exploitation du LHC &amp;agrave; 4 TeV durant l&amp;rsquo;ann&amp;eacute;e 2012.&lt;/em>&lt;/p> &lt;p> &lt;b>Un regard critique sur l&amp;rsquo;ann&amp;eacute;e 2011&lt;/b>&lt;/p> &lt;p> Lors de l&amp;rsquo;atelier, on s&amp;rsquo;est attach&amp;eacute; &amp;agrave; examiner les performances de la machine en d&amp;eacute;terminant les am&amp;eacute;liorations qui pourraient &amp;ecirc;tre apport&amp;eacute;es &amp;agrave; des syst&amp;egrave;mes critiques, tels que l&amp;rsquo;instrumentation de faisceau et la protection de la machine. Les collisions de faisceaux &amp;agrave; haute intensit&amp;eacute; r&amp;eacute;alis&amp;eacute;es l&amp;rsquo;ann&amp;eacute;e derni&amp;egrave;re au LHC ont mis en &amp;eacute;vidence certains aspects &amp;agrave; prendre en compte le long de l&amp;rsquo;anneau, notamment l&amp;rsquo;&amp;eacute;chauffement de certains mat&amp;eacute;riels d&amp;ucirc; aux faisceaux, et des pics de vide probl&amp;eacute;matiques. On a pr&amp;eacute;sent&amp;eacute; l&amp;rsquo;&amp;eacute;tat actuel des connaissances sur ces probl&amp;egrave;mes et avanc&amp;eacute; des solutions possibles.&lt;/p> &lt;p> La compression du faisceau (r&amp;eacute;duction de la taille du faisceau au point d&amp;rsquo;interaction), obtenue vers la fin de l&amp;rsquo;ann&amp;eacute;e, fut l&amp;rsquo;une des grandes r&amp;eacute;ussites de 2011. Il sera peut-&amp;ecirc;tre possible de comprimer encore davantage le faisceau en 2012 gr&amp;acirc;ce &amp;agrave; un param&amp;eacute;trage plus serr&amp;eacute; des collimateurs. On pourrait ainsi obtenir une luminosit&amp;eacute; de cr&amp;ecirc;te d&amp;rsquo;environ 6 x 10&lt;sup>33&lt;/sup> cm&lt;sup>-2&lt;/sup>s&lt;sup>-1&lt;/sup>, contre un maximum de 3,6 x 10&lt;sup>33&lt;/sup> cm&lt;sup>-2&lt;/sup>s&lt;sup>-1&lt;/sup> en 2011.&lt;/p> &lt;p> &lt;b>&lt;strong>Possibilit&amp;eacute;s pour 2012&lt;/strong>&lt;/b>&lt;/p> &lt;p> Steve Myers, directeur des acc&amp;eacute;l&amp;eacute;rateurs et de la technologie du CERN, a pr&amp;eacute;sent&amp;eacute; un r&amp;eacute;sum&amp;eacute; des recommandations formul&amp;eacute;es durant l&amp;rsquo;atelier pour la p&amp;eacute;riode d&amp;rsquo;exploitation de 2012. En bref, le LHC devrait &amp;ecirc;tre exploit&amp;eacute; &amp;agrave; 4 TeV, les priorit&amp;eacute;s essentielles &amp;eacute;tant les suivantes : fournir &amp;agrave; ATLAS et CMS une luminosit&amp;eacute; suffisante (de l&amp;rsquo;ordre de 15 fb&lt;sup>-1&lt;/sup>) qui leur permette, ind&amp;eacute;pendamment l&amp;rsquo;une de l&amp;rsquo;autre, soit de d&amp;eacute;couvrir le Higgs, soit de l&amp;rsquo;exclure ; r&amp;eacute;aliser l&amp;rsquo;exploitation proton-ion plomb ; et lancer le programme de d&amp;eacute;veloppement de la machine ax&amp;eacute; sur l&amp;rsquo;exploitation apr&amp;egrave;s le long arr&amp;ecirc;t technique. Il n&amp;rsquo;est pas exclu de prolonger l&amp;rsquo;exploitation pour pouvoir atteindre la luminosit&amp;eacute; int&amp;eacute;gr&amp;eacute;e vis&amp;eacute;e.&lt;/p> &lt;p> En 2012, la disponibilit&amp;eacute; de la machine devrait &amp;ecirc;tre am&amp;eacute;lior&amp;eacute;e gr&amp;acirc;ce &amp;agrave; un certain nombre de mesures d&amp;rsquo;att&amp;eacute;nuation prises pendant l&amp;rsquo;arr&amp;ecirc;t technique de fin d&amp;rsquo;ann&amp;eacute;e, dont certaines visaient &amp;agrave; r&amp;eacute;duire les effets des rayonnements sur l&amp;rsquo;&amp;eacute;lectronique situ&amp;eacute;e dans le tunnel du LHC.&lt;/p> &lt;p> &lt;b>&lt;strong>Projets pour le long arr&amp;ecirc;t de 2013-2014&lt;/strong>&lt;/b>&lt;/p> &lt;p> La dur&amp;eacute;e totale du long arr&amp;ecirc;t (LS1) du LHC est fix&amp;eacute;e provisoirement &amp;agrave; 20 mois environ. Les &amp;eacute;quipes concentreront leurs efforts sur la consolidation des connexions &amp;eacute;lectriques. Il s&amp;rsquo;agira d&amp;rsquo;ouvrir chacune des interconnexions d&amp;rsquo;aimants le long de l&amp;rsquo;anneau et de mesurer avec soin la r&amp;eacute;sistance de chaque connexion transportant le courant entre le dip&amp;ocirc;le et les quadrip&amp;ocirc;les des arcs du LHC. &amp;Agrave; ce jour, on estime que 15 % des connexions devront &amp;ecirc;tre refaites ; des d&amp;eacute;rivations et des brides de serrage seront install&amp;eacute;es au niveau de chaque connexion. Le but est d&amp;rsquo;exclure de mani&amp;egrave;re d&amp;eacute;finitive le risque que se reproduise l&amp;rsquo;incident survenu le 19 septembre 2008 aux &amp;eacute;nergies les plus &amp;eacute;lev&amp;eacute;es pr&amp;eacute;vues pour le LHC.&lt;/p> &lt;p> Parall&amp;egrave;lement, chacune des exp&amp;eacute;riences LHC a un vaste programme de travaux de maintenance et d&amp;rsquo;am&amp;eacute;lioration, lesquels seront importants pour certains des syst&amp;egrave;mes essentiels du LHC (cryog&amp;eacute;nie, vide, syst&amp;egrave;me de protection contre les transitions r&amp;eacute;sistives, distribution &amp;eacute;lectrique, refroidissement, ventilation, acc&amp;egrave;s et RF).&lt;/p> &lt;p> &lt;b>&lt;strong>La machine apr&amp;egrave;s le long arr&amp;ecirc;t technique&lt;/strong>&lt;/b>&lt;/p> &lt;p> Apr&amp;egrave;s le long arr&amp;ecirc;t technique (LS1), les dip&amp;ocirc;les du LHC devront de nouveau &amp;ecirc;tre entra&amp;icirc;n&amp;eacute;s, dans le cadre d&amp;rsquo;une vaste campagne, &amp;agrave; subir des transitions r&amp;eacute;sistives afin de parvenir &amp;agrave; l&amp;rsquo;&amp;eacute;nergie nominale de 7 TeV par faisceau. Aussi, l&amp;rsquo;&amp;eacute;nergie de faisceau dans les premi&amp;egrave;res ann&amp;eacute;es qui suivront le LS1 devrait-elle se situer aux environs de 6,5 TeV. Les am&amp;eacute;liorations pr&amp;eacute;vues pour le syst&amp;egrave;me d&amp;rsquo;injection n&amp;rsquo;auront alors pas encore &amp;eacute;t&amp;eacute; r&amp;eacute;alis&amp;eacute;es, mais la performance du syst&amp;egrave;me devrait permettre d&amp;rsquo;offrir une qualit&amp;eacute; de faisceau suffisante pour que la luminosit&amp;eacute; nominale du LHC atteigne 1 x 10&lt;sup>34&lt;/sup> cm&lt;sup>-2&lt;/sup>s&lt;sup>-1&lt;/sup>. Il a en outre &amp;eacute;t&amp;eacute; question des aspects susceptibles de limiter la performance apr&amp;egrave;s le LS1 (transitions r&amp;eacute;sistives, effets des rayonnements sur l&amp;rsquo;&amp;eacute;lectronique, UFO).&lt;/p> &lt;p> &lt;b>&lt;strong>Projets futurs&lt;/strong>&lt;/b>&lt;/p> &lt;p> &lt;span id="cke_bm_161S" style="display: none;">&amp;nbsp;&lt;/span>&lt;span id="cke_bm_162S" style="display: none;">&amp;nbsp;&lt;/span>&lt;span id="cke_bm_163S" style="display: none;">&amp;nbsp;&lt;/span>&lt;span id="cke_bm_164S" style="display: none;">&amp;nbsp;&lt;/span>&lt;span id="cke_bm_165S" style="display: none;">&amp;nbsp;&lt;/span>Les perspectives pour le projet d&amp;rsquo;am&amp;eacute;lioration des injecteurs du LHC (LIU) et son principal client, le LHC haute luminosit&amp;eacute; (HL-LHC), ont &amp;eacute;galement &amp;eacute;t&amp;eacute; examin&amp;eacute;es. Le HL-LHC, dont le d&amp;eacute;but de l&amp;rsquo;exploitation a provisoirement &amp;eacute;t&amp;eacute; fix&amp;eacute; aux environs de 2023, a pour ambition de fournir 200 &amp;agrave; 300 fb&lt;sup>-1&lt;/sup> par an. On a pass&amp;eacute; en revue les d&amp;eacute;fis que pr&amp;eacute;sentera le projet HL-LHC et on a notamment fait le point sur l&amp;#39;&amp;eacute;tat d&amp;#39;avancement de la R&amp;D pour les nouveaux aimants destin&amp;eacute;s aux r&amp;eacute;gions d&amp;rsquo;interaction haute luminosit&amp;eacute;.&lt;/p> &lt;p> On a &amp;eacute;galement &amp;eacute;voqu&amp;eacute; de fa&amp;ccedil;on informelle l&amp;rsquo;avenir encore plus lointain. Parmi les futurs projets envisageables figurent le Grand collisionneur hadron-&amp;eacute;lectron (LHeC), qui ferait entrer en collision des &amp;eacute;lectrons de 60 GeV avec des protons de 7 TeV, et le LHC haute &amp;eacute;nergie (HE-LHC), dans lequel l&amp;rsquo;&amp;eacute;nergie de faisceau du LHC serait port&amp;eacute;e de 7 &amp;agrave; 16,5 TeV. Ces options pr&amp;eacute;sentent toutes les deux de s&amp;eacute;rieux d&amp;eacute;fis technologiques.&lt;/p> &lt;hr /> &lt;p> Steve Myers, directeur des acc&amp;eacute;l&amp;eacute;rateurs et de la technologie au CERN, et Sergio Bertolucci, directeur de la recherche au CERN, font le point sur l&amp;#39;atelier de Chamonix (en anglais) :&lt;span id="cke_bm_165E" style="display: none;">&amp;nbsp;&lt;/span>&lt;span id="cke_bm_164E" style="display: none;">&amp;nbsp;&lt;/span>&lt;span id="cke_bm_163E" style="display: none;">&amp;nbsp;&lt;/span>&lt;span id="cke_bm_162E" style="display: none;">&amp;nbsp;&lt;/span>&lt;span id="cke_bm_161E" style="display: none;">&amp;nbsp;&lt;/span>&lt;/p> &lt;script language="javascript" src="/insertplayer.js" type="text/javascript">&lt;/script>&lt;script type="text/javascript"> var flash_video_player=get_video_player_path(); insert_player_for_external('Video/Public/Movies/2012/CERN-MOVIE-2012-011/CERN-MOVIE-2012-011-0753-kbps-640x360-25-fps-audio-64-kbps-44-kHz-stereo', 'mms://mediastream.cern.ch/MediaArchive/Video/Public/Movies/2012/CERN-MOVIE-2012-011/CERN-MOVIE-2012-011-0480-kbps-512x288-25-fps-audio-128-kbps-48-kHz-stereo.wmv', 'false', 480, 360, 'https://mediastream.cern.ch/MediaArchive/Video/Public/Movies/2012/CERN-MOVIE-2012-011/CERN-MOVIE-2012-011-posterframe-640x360-at-10-percent.jpg', '1423359', true, 'Video/Public/Movies/2012/CERN-MOVIE-2012-011/CERN-MOVIE-2012-011-0600-kbps-maxH-360-25-fps-audio-128-kbps-48-kHz-stereo.mp4'); &lt;/script></subfield>
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    <subfield code="b">&lt;!--HTML--> &lt;p class="articleHeader"> On a relatively warm Thursday morning in Chamonix (-7 Celsius) the workshop looked at what things would be like after the upcoming long shutdown (LS1 -&amp;nbsp; 2013/14). A large number of re-training&amp;nbsp; quenches of the LHC dipoles will be required in order to reach the nominal energy of 7 TeV so the beam energy in the first years after LS1 is expected to be around 6.5 TeV. The planned injector upgrades will not have been deployed at this stage, but the injector performance still looks capable of supplying sufficient beam quality to enable the LHC to reach the design luminosity of 1x10&lt;sup>34&lt;/sup> cm&lt;sup>-2&lt;/sup>s&lt;sup>-1&lt;/sup>.&lt;/p> &lt;p> &amp;nbsp;&lt;/p> &lt;p> A lot has been learned operating at 3.5 TeV over the last couple of years and many improvements have been made in the magnet powering and protection systems. The prospects for post-LS1 machine availability are encouraging. Potential limitations to post-LS1 performance (quenches, radiation to electronics, UFOs) were also considered.&lt;/p> &lt;p> The evening was spent considering the more dim and distant future and the prospects for the LHC Injector Upgrade project and its client, the High-Luminosity LHC (HL-LHC), tentatively scheduled to start operating around 2023. The goals of the HL-LHC are ambitious (200 - 300 inverse femtobarns per year) and the demands on the upgraded injectors reflect this. The devil is in the detail but it&amp;#39;s clear a lot of work remains to be done.&lt;/p></subfield>
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    <subfield code="b">&lt;!--HTML--> &lt;p class="articleHeader"> &amp;Agrave; Chamonix, il faisait un peu moins froid ce jeudi (-7&amp;deg; C). Les discussions ont port&amp;eacute; sur ce qui nous attend apr&amp;egrave;s le long arr&amp;ecirc;t &amp;agrave; venir (LS1, en 2013-2014). Les dip&amp;ocirc;les du LHC devront de nouveau &amp;ecirc;tre entra&amp;icirc;n&amp;eacute;s, dans le cadre d&amp;rsquo;une vaste campagne, &amp;agrave; subir des transitions r&amp;eacute;sistives afin de parvenir &amp;agrave; l&amp;rsquo;&amp;eacute;nergie nominale de 7 TeV, de sorte que l&amp;rsquo;&amp;eacute;nergie du faisceau dans les premi&amp;egrave;res ann&amp;eacute;es qui suivront le long arr&amp;ecirc;t LS1 devrait se situer aux environs de 6,5 TeV. Les am&amp;eacute;liorations pr&amp;eacute;vues pour le syst&amp;egrave;me d&amp;rsquo;injection n&amp;rsquo;auront alors pas encore &amp;eacute;t&amp;eacute; r&amp;eacute;alis&amp;eacute;es, mais la performance du syst&amp;egrave;me devrait permettre d&amp;rsquo;offrir une qualit&amp;eacute; de faisceau suffisante pour que la luminosit&amp;eacute; nominale du LHC atteigne 1x10&lt;sup>34 &lt;/sup>cm&lt;sup>-2&lt;/sup>s&lt;sup>-1&lt;/sup>.&lt;/p> &lt;p> &amp;nbsp;&lt;/p> &lt;p> On a beaucoup appris lors de l&amp;rsquo;exploitation &amp;agrave; 3,5 TeV ces deux derni&amp;egrave;res ann&amp;eacute;es et un grand nombre d&amp;rsquo;am&amp;eacute;liorations a &amp;eacute;t&amp;eacute; apport&amp;eacute; aux syst&amp;egrave;mes de protection et d&amp;rsquo;alimentation des aimants. Les perspectives pour la disponibilit&amp;eacute; de la machine apr&amp;egrave;s le long arr&amp;ecirc;t LS1 sont encourageantes. Il a en outre &amp;eacute;t&amp;eacute; question des aspects susceptibles de limiter la performance apr&amp;egrave;s le long arr&amp;ecirc;t LS1 (transitions r&amp;eacute;sistives, effets des rayonnements sur l&amp;rsquo;&amp;eacute;lectronique, UFO).&lt;/p> &lt;p> En soir&amp;eacute;e, les participants ont envisag&amp;eacute; l&amp;rsquo;avenir plus lointain et les perspectives pour le projet d&amp;rsquo;am&amp;eacute;lioration des injecteurs du LHC (LIU) et son client, le LHC haute luminosit&amp;eacute; (HL-LHC), dont le d&amp;eacute;but de l&amp;rsquo;exploitation a provisoirement &amp;eacute;t&amp;eacute; fix&amp;eacute; aux environs de 2023. Les objectifs du projet HL-LHC sont ambitieux (200 &amp;agrave; 300 fb&lt;sup>-1&lt;/sup> par an) ; les exigences requises pour l&amp;rsquo;am&amp;eacute;lioration des injecteurs en sont la cons&amp;eacute;quence. Le diable est dans les d&amp;eacute;tails, et une chose est s&amp;ucirc;re : il reste encore beaucoup &amp;agrave; faire.&lt;/p> &lt;p> &amp;nbsp;&lt;/p></subfield>
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    <subfield code="b">&lt;!--HTML-->&lt;!--HTML--> &lt;p class="articleHeader" style="text-align: justify;"> The LHC is enjoying a confluence of twos. This morning (Friday 5 August) we passed 2 inverse femtobarns delivered in 2011; the peak luminosity is now just over 2 x10&lt;sup>33&lt;/sup> cm&lt;sup>-2&lt;/sup>s&lt;sup>-1&lt;/sup>; and recently fill 2000 was in for nearly 22 hours and delivered around 90 inverse picobarns, almost twice 2010&amp;#39;s total.&lt;/p> &lt;p style="text-align: justify;"> &amp;nbsp;&lt;/p> &lt;p style="text-align: justify;"> In order to increase the luminosity we can increase of number of bunches, increase the number of particles per bunch, or decrease the transverse beam size at the interaction point. The beam size can be tackled in two ways: either reduce the size of the injected bunches or squeeze harder with the quadrupole magnets situated on either side of the experiments. Having increased the number of bunches to 1380, the maximum possible with a 50 ns bunch spacing, a one day meeting in Crozet decided to explore the other possibilities.&lt;/p> &lt;p style="text-align: justify;"> The size of the beams coming from the injectors has been reduced to the minimum possible. This has brought an increase in the peak luminosity of about 50% and the 2 x 10&lt;sup>33&lt;/sup> cm&lt;sup>-2&lt;/sup>s&lt;sup>-1&lt;/sup> level has now been passed. The next stage is to adiabatically increase the bunch intensity with the all out maximum being around 1.6 x 10&lt;sup>11&lt;/sup> protons per bunch. The mechanics of squeezing further are reasonably complicated and this possibility has been shelved until after the next technical stop.&lt;/p> &lt;p style="text-align: justify;"> The higher peak luminosity has given some impressive production rates and we are seeing over 6 inverse picobarn an hour at the start of a fill. However, recently operational efficiency has been hit and fills have been lost. These difficulties have been caused by electrical network glitches, the effects of radiation on electronics, vacuum spikes, and UFOs, among other things. Some of these are clearly related to high intensity and high luminosity; it might be said that we are victims of our own success. Nevertheless on 2 August the LHC managed 90 inverse picobarns in one day.&lt;/p></subfield>
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    <subfield code="b">&lt;p> &lt;!--HTML-->&lt;!--HTML-->&lt;/p> &lt;p class="articleHeader" style="text-align: justify;"> Le LHC semble actuellement en mode 2. Ce matin (vendredi 5 ao&amp;ucirc;t), nous avons en effet pass&amp;eacute; la barre des 2 femtobarns inverses produits en 2011 ; le pic de luminosit&amp;eacute; est maintenant &amp;agrave; un peu plus de 2 x10&lt;sup>33&lt;/sup> cm&lt;sup>-2&lt;/sup>s&lt;sup>-1&lt;/sup> ; et le r&amp;eacute;cent remplissage 2000 a dur&amp;eacute; pr&amp;egrave;s de 22 heures et a produit environ 90 picobarns inverses, soit presque deux fois le total atteint en 2010.&lt;/p> &lt;p style="text-align: justify;"> &amp;nbsp;&lt;/p> &lt;p style="text-align: justify;"> Si nous souhaitons accro&amp;icirc;tre la luminosit&amp;eacute;, nous pouvons augmenter le nombre de paquets, augmenter le nombre de particules par paquet, ou r&amp;eacute;duire la dimension transversale des faisceaux au point d&amp;rsquo;interaction. La taille du faisceau peut &amp;ecirc;tre modifi&amp;eacute;e de deux mani&amp;egrave;res : soit en r&amp;eacute;duisant la taille des paquets inject&amp;eacute;s, soit en comprimant davantage le faisceau &amp;agrave; l&amp;rsquo;aide des aimants quadripolaires situ&amp;eacute;s de part et d&amp;rsquo;autre des exp&amp;eacute;riences.&amp;nbsp; Le nombre de paquets ayant d&amp;eacute;j&amp;agrave; &amp;eacute;t&amp;eacute; port&amp;eacute; &amp;agrave; 1 380 - le maximum possible avec un intervalle entre paquets de 50 ns - il a &amp;eacute;t&amp;eacute; d&amp;eacute;cid&amp;eacute;, lors d&amp;rsquo;une r&amp;eacute;union tenue &amp;agrave; Crozet, d&amp;rsquo;explorer les autres possibilit&amp;eacute;s.&lt;/p> &lt;p style="text-align: justify;"> La taille des faisceaux provenant des injecteurs a &amp;eacute;t&amp;eacute; r&amp;eacute;duite &amp;agrave; son minimum. Cela a entra&amp;icirc;n&amp;eacute; une hausse d&amp;#39;environ 50% de la luminosit&amp;eacute; de cr&amp;ecirc;te et le niveau de 2 x 1033 cm-2 s-1 a &amp;eacute;t&amp;eacute; d&amp;eacute;pass&amp;eacute;. La prochaine &amp;eacute;tape consiste en une augmentation adiabatique de l&amp;rsquo;intensit&amp;eacute; du faisceau jusqu&amp;rsquo;&amp;agrave; un maximum d&amp;#39;environ 1,6 x 1011 protons par paquet. Les techniques permettant une compression plus grande sont relativement complexes et cette possibilit&amp;eacute; a &amp;eacute;t&amp;eacute; mise de c&amp;ocirc;t&amp;eacute; en attendant le prochain arr&amp;ecirc;t technique.&lt;/p> &lt;p style="text-align: justify;"> La luminosit&amp;eacute; de cr&amp;ecirc;te plus &amp;eacute;lev&amp;eacute;e a entra&amp;icirc;n&amp;eacute; une production impressionnante : plus de 6 pb-1 ont pu &amp;ecirc;tre mesur&amp;eacute;s en d&amp;eacute;but de remplissage. Cependant, l&amp;rsquo;efficacit&amp;eacute; op&amp;eacute;rationnelle de la machine a r&amp;eacute;cemment &amp;eacute;t&amp;eacute; perturb&amp;eacute;e et des injections de particules ont &amp;eacute;t&amp;eacute; perdues. Ces difficult&amp;eacute;s sont dues, entre autres, &amp;agrave; des d&amp;eacute;faillances du r&amp;eacute;seau &amp;eacute;lectrique, aux effets du rayonnement sur les syst&amp;egrave;mes &amp;eacute;lectroniques, &amp;agrave; des irr&amp;eacute;gularit&amp;eacute;s dans le syst&amp;egrave;me de vide ou aux UFO. Elles sont, pour certaines d&amp;rsquo;entre elles, directement li&amp;eacute;es aux hauts niveaux d&amp;rsquo;intensit&amp;eacute; et de luminosit&amp;eacute; ; nous sommes, en quelque sorte, victimes de notre propre succ&amp;egrave;s. Le 2 ao&amp;ucirc;t, le LHC est tout de m&amp;ecirc;me parvenu &amp;agrave; produire 90 pb-1 en une seule journ&amp;eacute;e, et affiche un total de 1,9 fb-1 pour l&amp;rsquo;ensemble de l&amp;rsquo;ann&amp;eacute;e en cours.&lt;/p></subfield>
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    <subfield code="b">&lt;!--HTML--> &lt;p class="articleHeader">The last technical stop finished on Friday 8 July, but the machine returned to its pre-stop performance level over a week later.&lt;/p> &lt;p>&amp;nbsp;&lt;/p> &lt;div class="phlwithcaption"> &lt;div class="imageScale">&lt;a target="_blank" href="https://lhc-statistics.web.cern.ch/LHC-Statistics/">&lt;img height="216" width="300" alt="" src="http://cds.cern.ch/record/1368917/files/LHC_Report(2)_image.png?subformat=icon" />&lt;/a>&lt;/div> &lt;p>Efficiency of LHC fills between 16 July and 20 July, 2011.&lt;/p> &lt;/div> &lt;p>The cryogenics team had the entire ring cold by Saturday morning and the usual post-technical stop tests with circulating beams started soon after. Unfortunately, they were interrupted by a major perturbation to CERN&amp;rsquo;s electrical network caused by an impressive thunderstorm that swept over the Pays de Gex. There were major knock-on effects, including the loss of cooling to the cryogenics and an inevitable recovery period once normal service had been re-established. The beams were circulating again by Tuesday afternoon and the post-technical stop checks continued, beefed up with further tests to address a number of issues related to the power cut.&amp;nbsp;&lt;/p> &lt;p>Before the stop, the LHC had managed to get 1380 bunches per beam into collisions and the plan was to ramp back up relatively quickly to this level via fills with 48, 264, and 840 bunches per beam. 48 and 264 bunches passed off reasonably smoothly. However, 840 bunches proved more difficult with three consecutive fills lost at high energy due to UFOs.  &lt;br /> &lt;br /> UFOs are a &lt;a target="_blank" href="http://cdsweb.cern.ch/journal/CERNBulletin/2011/24/News%20Articles/1357318">regular feature&lt;/a> of operation and they sometimes appear in bursts around one hour after the injection process. Usually these UFOs generate losses below the dump threshold, but following the stop they were stronger than usual. Operations opted to wait at 450 GeV for an hour to let the UFOs pass before ramping and this allowed for three fills - one with 840 bunches and two with 1092 bunches - that led the way back to physics with 1380 bunches. The evening of Monday 18 June saw a 1380 bunch fill go into 'Stable beams' with an initial luminosity of between 1.4 and 1.5 x10&lt;sup>33&lt;/sup> cm&lt;sup>-2&lt;/sup>s&lt;sup>-1&lt;/sup> &amp;ndash; another new record. The UFOs have since quieted down.&lt;/p> &lt;p>With 1380 nominal bunches, the LHC is now dealing with around half design intensity. There are ongoing issues with UFOs, the effects of radiation on electronics, vacuum activity and so on. Mitigating these effects and learning to live with high intensity is all part of the process, and the current aim is to re-establish stable conditions and realize the potential of the machine to deliver some serious integrated luminosity.&lt;/p> &lt;p>&amp;nbsp;&lt;/p> &lt;p>&amp;nbsp;&lt;/p> &lt;p>&amp;nbsp;&lt;/p></subfield>
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    <subfield code="b">&lt;!--HTML--> &lt;p class="articleHeader">Le dernier arr&amp;ecirc;t technique a pris fin le vendredi 8 juillet, mais il aura fallu une semaine pour que la machine retrouve son niveau de performance d&amp;rsquo;avant arr&amp;ecirc;t.&lt;/p> &lt;p>&amp;nbsp;&lt;/p> &lt;div class="phlwithcaption"> &lt;div class="imageScale">&lt;a target="_blank" href="https://lhc-statistics.web.cern.ch/LHC-Statistics/">&lt;img height="216" width="300" alt="" src="http://cds.cern.ch/record/1368917/files/LHC_Report(2)_image.png?subformat=icon" />&lt;/a>&lt;/div> &lt;p>Statistiques sur l'exploitation du LHC entre le 16 et le 20 juillet 2011.&lt;/p> &lt;/div> &lt;p>L&amp;rsquo;&amp;eacute;quipe responsable de la cryog&amp;eacute;nie avait remis &amp;agrave; froid la totalit&amp;eacute; de l&amp;rsquo;anneau samedi matin, et les tests avec faisceaux en circulation qui font habituellement suite &amp;agrave; un arr&amp;ecirc;t technique ont d&amp;eacute;but&amp;eacute; peu apr&amp;egrave;s. Ils ont malheureusement &amp;eacute;t&amp;eacute; interrompus par une importante perturbation sur le r&amp;eacute;seau &amp;eacute;lectrique du CERN due &amp;agrave; un violent orage qui s&amp;rsquo;est abattu sur le Pays de Gex. Cet orage a eu des r&amp;eacute;percussions importantes, notamment une perte de refroidissement au niveau du syst&amp;egrave;me cryog&amp;eacute;nique et une in&amp;eacute;vitable p&amp;eacute;riode de reprise une fois la situation revenue &amp;agrave; la normale. Mardi apr&amp;egrave;s-midi, les faisceaux circulaient de nouveau et les v&amp;eacute;rifications se sont poursuivies, compl&amp;eacute;t&amp;eacute;es par de nouveaux tests destin&amp;eacute;s &amp;agrave; contr&amp;ocirc;ler un certain nombre d&amp;rsquo;aspects li&amp;eacute;s &amp;agrave; la coupure d&amp;rsquo;&amp;eacute;lectricit&amp;eacute;.&lt;/p> &lt;p>Avant l&amp;rsquo;arr&amp;ecirc;t, le LHC avait r&amp;eacute;ussi &amp;agrave; fonctionner avec 1 380 paquets par faisceau et il &amp;eacute;tait pr&amp;eacute;vu de revenir relativement rapidement &amp;agrave; ce niveau gr&amp;acirc;ce &amp;agrave; des injections de 48, 264 puis 840 paquets par faisceau. Les injections &amp;agrave; 48 et 264 paquets se sont d&amp;eacute;roul&amp;eacute;es sans encombre. Le passage &amp;agrave; 840 paquets a toutefois &amp;eacute;t&amp;eacute; plus difficile, trois remplissages cons&amp;eacute;cutifs ayant &amp;eacute;t&amp;eacute; perdus &amp;agrave; haute &amp;eacute;nergie en raison de poussi&amp;egrave;res microscopiques (les UFO). &lt;br /> &lt;br /> Ces poussi&amp;egrave;res sont&lt;a target="_blank" href="http://cdsweb.cern.ch/journal/CERNBulletin/2011/24/News%20Articles/1357318"> habituelles de l&amp;rsquo;exploitation&lt;/a>. Elles apparaissent parfois en jets  environ une heure apr&amp;egrave;s le d&amp;eacute;but de l&amp;rsquo;injection. Habituellement, elles entra&amp;icirc;nent des d&amp;eacute;perditions de faisceau qui n&amp;rsquo;atteignent pas le seuil d&amp;eacute;clenchant l&amp;rsquo;arr&amp;ecirc;t du faisceau, mais cette fois-ci, elles ont &amp;eacute;t&amp;eacute; plus importantes que d&amp;rsquo;ordinaire. Il a &amp;eacute;t&amp;eacute; d&amp;eacute;cid&amp;eacute; de maintenir le faisceau &amp;agrave; 450 GeV pendant une heure avant de remonter en &amp;eacute;nergie, de mani&amp;egrave;re &amp;agrave; laisser les poussi&amp;egrave;res passer, ce qui a permis de r&amp;eacute;aliser trois injections (une avec 840 paquets et deux avec 1 092 paquets), qui ont de nouveau ouvert la voie &amp;agrave; une exploitation &amp;agrave; 1 380 paquets. Lundi 18 juin au soir, une injection &amp;agrave; 1 380 paquets a d&amp;eacute;bouch&amp;eacute; sur des &amp;laquo; faisceaux stables &amp;raquo; avec une luminosit&amp;eacute; initiale comprise entre 1,4 et 1,5 x 10&lt;sup>33&lt;/sup>cm&lt;sup>-2&lt;/sup>s&lt;sup>-1&lt;/sup> - un nouveau record. Depuis, les poussi&amp;egrave;res n&amp;rsquo;ont pas refait parler d&amp;rsquo;elles.&lt;/p> &lt;p>Avec 1 380 paquets nominaux, le LHC est &amp;agrave; pr&amp;eacute;sent &amp;agrave; mi-chemin de son intensit&amp;eacute; nominale. Certains aspects restent &amp;agrave; surveiller (poussi&amp;egrave;res microscopiques, effets des rayonnements sur l&amp;rsquo;&amp;eacute;lectronique, vide, etc). Att&amp;eacute;nuer ces effets et apprendre &amp;agrave; vivre avec de hautes intensit&amp;eacute;s fait partie du jeu ; l&amp;rsquo;objectif est actuellement de r&amp;eacute;tablir des conditions stables et d'atteindre au mieux le potentiel de luminosit&amp;eacute; int&amp;eacute;gr&amp;eacute;e de la machine.&amp;nbsp;&lt;/p></subfield>
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    <subfield code="b">&lt;!--HTML--> &lt;p>&lt;strong>1 Operational experience 2011&lt;/strong>&lt;/p> &lt;p>&lt;strong>1.1 Overview&lt;/strong>&lt;/p> &lt;p>Starting on a positive note, it is encouraging that, for the period of this report, the operation of CMS and its entire infrastructure at Point 5 was remarkably stable and efficient. No luminosity was lost due to failures of common systems or infrastructure. The major faults were two failures of rack ventilation turbines, a leak in a water pump in the endcap circuit and the first fast dump of the magnet since underground commissioning. As the rack ventilation units have two turbines, these single turbine failures were tolerated until the next possible access. The water pump survived until the end of the fill after which the circuit was switched to a reserve pump (which in principle is also possible &amp;ldquo;on the fly&amp;rdquo;). A faulty position controller of a cryo-valve serving the cryo-power leads caused a spontaneous closure of the valve leading to the fast dump of the magnet. In this case, CMS was lucky once again, since the incident happened on the first day of the May technical stop. The magnet was recovered in record time, just less than four days.&lt;/p> &lt;p>It would be a mistake to misinterpret the recent excellent technical performance, over-reliant on good fortune, as evidence that further consolidation and improvement are unnecessary.&lt;/p> &lt;p>&lt;strong>1.2 Short accesses&lt;/strong>&lt;/p> &lt;p>CMS subdetectors made regular use of access possibilities when LHC had to stop for technical reasons. Though only one access for HCAL was mission-critical for high quality data-taking, several components, in particular power supply systems, showed disturbingly high failure rates, which might become critical in case the frequency of LHC accesses drops.&lt;/p> &lt;p>&lt;strong>1.3 Major incidents&lt;/strong>&lt;/p> &lt;p>On 23&lt;sup>rd&lt;/sup> June, the LHC power network was hit by a lightning-induced failure of a pair of 18-kV substations. All cooling and ventilation was lost with the most severe consequence that the cold box stopped. Due to the investment in ride-through over the last year and an outstanding reaction from CMS subsystem and common-system field coordinators plus the TE, EN and PH department piquet teams, the CMS magnet was able to survive the incident at full field, saving what would otherwise have been an unnecessary on-off-on cycle.  Recent measurements of the residual resistance ratio of the high purity aluminium stabiliser of the solenoid conductor indicate that it remains prudent to minimise the number of on-off cycles, currently standing at 51, to 200-300.  The six-cycle maximum targeted for 2011 remains within reach.&lt;/p> &lt;p>The key features for minimising the impact of the 23&lt;sup>rd&lt;/sup> June incident were the electrical system filtering, the UPS, the high capacity of the reserve helium dewar and the rapid unloading of the cooling system to focus inherent remaining cooling capacity on the busbar circuit until the towers and chillers could be restarted. A first &amp;ldquo;post mortem&amp;rdquo; analysis showed that only minor damage was sustained. In particular only a single power supply in the UXC had to have communication re-established by hand, showing that the equipment in the UXC is robust and well-controlled remotely. The UPS coverage on the surface has to be improved, the observed failure of the ventilation can easily be prevented and some computers have to be better protected to simplify the restart.&lt;/p> &lt;p>&lt;strong>1.4 Cooling system&lt;/strong>&lt;/p> &lt;p>Since January, two substantial water leaks and 20 micro-leaks were detected. One of the big leaks was detected by the new leak detection system, all the rest by manual inspections. All but one (muon circuit) were in the rack circuit. Based on this observation, the cooling team intends to modify the joints in critical racks (mostly Tracker) where they are often hard to access. There were several unforeseen stoppages of cooling systems during maintenance of neighbouring ones, due to faulty procedures or interdependencies. No consequences for data-taking resulted, but these incidents confirm the need for a consolidation program, part of the upgrade work foreseen for the next shutdown. This will decouple the most critical circuits, in particular the magnet busbar circuit, which will be made completely independent to avoid inadvertent magnet ramp down.&lt;/p> &lt;p>Following the intensive investment in the fluorocarbon cooling plants during the 2010/&amp;rsquo;11 year-end stop and subsequent technical stops by the CMS Tracker teams, EN-CV-DC and CMS cooling coordination, it is very pleasing to note the very low leak rate of C&lt;sub>6&lt;/sub>F&lt;sub>14&lt;/sub> which is now being sustained. The teams successfully isolated the main remaining leak and implemented extensive measures to reduce the pressure transients suspected of causing such leaks.&lt;/p> &lt;p>&lt;strong>1.5 Beam Radiation Monitoring&lt;/strong>&lt;/p> &lt;p>The detector protection aspects of BRM are functioning with the required reliability. For the first time (during the LHC &amp;ldquo;UFO&amp;rdquo; event of 22&lt;sup>nd&lt;/sup> May), beam condition monitor signals reached a large fraction (93%) of the abort threshold. The redundancy of the systems will soon be improved by the inclusion of BCM1L (leakage current diamond detectors at &amp;plusmn;1.8 m) into the abort logic. The rapid increase in luminosity and bunch intensity has resulted in the large Beam Scintillation Counters reaching saturation and no longer being very useful as a background monitor for pp operation. The BSC upgrade is in the early planning phase with projected installation in 2014. A project kick-off workshop is planned for 22&lt;sup>nd&lt;/sup> July 2011. The BRM group is currently switching to BCM1F to provide background measurements, but the great potential of this single-crystal diamond monitor has not yet been realised, due to manpower shortages.&lt;/p> &lt;p>&lt;strong>2 Facilities for supporting operation, maintenance and upgrade&lt;/strong>&lt;/p> &lt;p>&lt;strong>2.1 Building 904&lt;/strong>&lt;/p> &lt;p>The commissioning of the CSC production line in Building 904 is progressing well. On 15&lt;sup>th&lt;/sup> June, gluing of the first cathode panel and winding of the first anode panel for the first ME4/2 CSC chamber were finished. Preparations for the RPC production line continue, with the order for climate-controlled rooms imminent. Gas distribution and the central cooling plant are progressing on schedule. The intention is to be ready to start RPC prototype construction in late autumn.  Meanwhile, the metallo-textile CMS storage tent behind building 904 is more than half-filled with installation tools from SX5 and the ISR.&lt;/p> &lt;p>&lt;strong>2.2 Point 5 Surface Assembly Building, SX5&lt;/strong>&lt;/p> &lt;p>The SX5 building is now almost completely cleared of installation tooling, which finally releases space to start the conversion into the future maintenance and repair centre of CMS. Technical specifications for the shell structure of the pixel laboratories in the SHL alcove will be issued shortly. The order for installation of a first floor (HCAL electronics lab) in the SL51 alcove has been placed and the next step will be to setup the radiation-protection zone perimeter on the floor of SX5 proper. This zone, which will house a workshop for activated detectors and a storage zone for activated components, will soon be fenced off by concrete blocks and equipped with access-controlled entry. Later the adjacent storage and working areas for subdetectors and infrastructure will be installed, with priority on the gas detector areas, as the muon detector projects have to give up the bulk of their remaining zones in ISR by the end of 2011.&lt;br /> &lt;br /> &lt;strong>3 Planning&lt;/strong>&lt;/p> &lt;p>&lt;strong>3.1 Long Shutdowns&lt;/strong>&lt;/p> &lt;p>The current baseline CERN planning envisages Long Shutdown 1 (LS1) starting at the end of 2012 and lasting 18 months, with Long Shutdown 2 (LS2) starting at the end of 2017, and having a duration driven by experiment requirements.  Variants on this planning are being considered and, although no decision will be taken for some months, CMS must make contingency plans to deal with the challenges that may result from the baseline and from alternative scenarios, which also helps inform our input to the decision-making process.  One particularly challenging option would be a delayed start of Long Shutdown 1 by four-five months and a delay (or creep) of LS2 until the end of 2018.  The duration of LS1 and the performance limits of the LHC thereafter are key ingredients of the planning process.  In this context the recent review recommendation that LHC collimator upgrades in the IR3 dispersion suppressors can be postponed for three years without affecting nominal performance at 7 TeV/beam is highly significant and should soon lead to a reliable estimate of the duration of LS1 (probably 20 months).  It is already clear that very careful planning and prioritisation will be necessary to fit all the required work into the available time. Technical Coordination will use this collaboration week to discuss possible scenarios in some detail. Underlying the planning process is the need to always have contingency plans in hand for unexpected LHC repairs of varying duration.&lt;/p> &lt;p>&lt;strong>3.2 Year-end technical stops&lt;/strong>&lt;/p> &lt;p>The year-end technical stops are a potentially vital ingredient in the overall consolidation and upgrade plan as well as being essential for maintenance and repair.  Based on the many uncertainties in the current planning, Technical Coordination and the EAM team are paying particular attention to the options for the 2011/&amp;rsquo;12 and 2016/&amp;rsquo;17 year-end stops.  The first offers possibilities to start Phase 1 upgrade work, the second (suitably extended) may, in certain scenarios, be the only logical window for installation of the Phase 1 (four-layer, low mass) pixel tracker. A provisional decision on whether to open CMS in winter 2011/&amp;rsquo;12 will be taken in September, weighing the risks to physics performance in 2012 against the benefits in 2012 and beyond. Discussions of potential work packages and their preparatory work will continue during this CMS week.&lt;/p> &lt;p>&lt;strong>4 Magnet, Infrastructure and Common Systems Projects&lt;/strong>&lt;/p> &lt;p>Several common systems or infrastructure projects, centrally managed by Technical Coordination, are already in preparation, mostly for execution in LS1.&lt;/p> &lt;p>&lt;strong>4.1 Common Systems: Beampipe&lt;/strong>&lt;/p> &lt;p>The dimensions and tolerances of the new central beampipe, matching the Phase 1 Pixel Tracker upgrade, have been fixed and discussed in the LEB meetings. The final aperture calculation, vacuum simulation and mechanical stress investigations are ongoing.  The proposed inner diameter of the central beryllium cylinder is 43.4 mm and at &amp;plusmn; 1.45 m this flares into a conical part along &amp;eta; = 4.9. The metals aluminium, beryllium, and AlBeMet (a 38%/62% aluminium-beryllium alloy) are under investigation as an alternative, replacing stainless steel in the outer cones &amp;plusmn; 1.95 m and possibly also up to &amp;plusmn; 3.12 m.  AlBeMet has excellent mechanical properties, will become much less activated than stainless steel, but is subject to the same handling and surface protection regulations as beryllium. Final approval of the dimensions will be requested from the LMC in a few weeks, with a view to completing the design, holding an EDR and placing the order before the end of the year. The walls of the new 21.7-mm radius central pipe can be guaranteed to be initially placed clear of the virtual 17-mm radius cylinder joining the bores of the two TAS absorbers. However, time-dependent tolerances (such as cavern-floor movements) may lead to this condition being unsustainable over the potential three-four-year period between long shutdowns.  The actual position of the pipe wall can be verified in a few days via nuclear interaction tomography but it is advisable that the high-&amp;beta;* operation requested by TOTEM for total cross-section measurements be completed in the first year after LS1 to avoid the need for a lengthy and costly opening for beampipe re-positioning.&lt;/p> &lt;p>&lt;strong>4.2 Common systems: Magnet Cryogenics&lt;/strong>&lt;br /> &lt;br /> As mentioned in previous reports and in the Upgrade Technical Proposal, failure of one or both of the helium compressor pair in the surface cryo-plant is a critical single-point failure for CMS and urgent action is being taken to specify custom-built components which can reduce the impact of this failure from four-six months to one month. This vulnerability is rendered more urgent by the recent sudden failure of similar (but not identical) compressors in the LHC cryo-plants. The plan during LS1 is to implement the full redundancy for which provision was made in the design. A funding mechanism is being discussed in the appropriate CMS boards.&lt;/p> &lt;p>&lt;strong>4.3 Common systems: Radiation shielding&lt;/strong>&lt;/p> &lt;p>Easily deployed radiation shielding will be necessary to allow access to all parts of CMS, respecting the ALARA principle and minimising individual and collective dose to personnel. Recently a break-through has been made in the design of shielding for the region between the Tracker bulkhead and z = 10.7 m. It is foreseen to finalise the design over the summer, hold an EDR in autumn and starting production towards the end of the year.&lt;/p> &lt;p>&lt;strong>4.4 Endcap Muon: YE4&lt;/strong>&lt;/p> &lt;p>Although coordinated as part of the endcap muon upgrade, the YE4 shielding wall is an integral part of the overall CMS shielding strategy for nominal luminosity. It is designed to absorb radiation due to particles escaping from the forward shielding and reflecting back off the headwall. The first material was delivered to HMC-3, Taxila, Pakistan in April. Approval of the cutting scheme, quality control plan and inspection points was agreed in June, and material for the first sector cases in now being cut. Delivery to CERN is expected in early 2012, after which a second horizontal assembly will be done prior to filling the sectors with the shielding mixture. LS1 provides the only available window for underground assembly of the YE4s. A tooling-and-assembly EDR is planned for August 2011.&lt;/p> &lt;p>&lt;strong>4.5 Tracking: Pixel Luminosity Telescope&lt;/strong>&lt;/p> &lt;p>The PLT upgrade to the Beam Radiation Monitoring System has recently been thoroughly reviewed. The details of the review are still being analysed, but one can already congratulate all participants on the massive progress the project has made during the last six months. 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    <subfield code="b">&lt;!--HTML--> &lt;p class="articleHeader">The LHC has held the number of bunches per beam at 1092 over the last couple of weeks and has been delivering luminosity to the experiments at a healthy rate. The integrated luminosity total has already passed 1 inverse femtobarn (fb&lt;sup>-1&lt;/sup>), which was the overall goal for the year. There was a modest celebration in the CCC to mark the occasion. Modest celebrations are now on hold until the end of this year's run or the delivery of 5 fb&lt;sup>-1&lt;/sup>.&lt;/p> &lt;p>&amp;nbsp;&lt;/p> &lt;div class="phlwithcaption"> &lt;div class="imageScale">&lt;a target="_blank" href="http://cds.cern.ch/record/1360708/files/LHCReport_image.png">&lt;img width="300" height="230" alt="" src="http://cds.cern.ch/record/1360708/files/LHCReport_image.png?subformat=icon" />&lt;/a>&lt;/div> &lt;/div> &lt;p>LHCb is designed to perform different types of physics searches from those at ATLAS and CMS, and is limited to a peak luminosity of about 3x10&lt;sup>32&lt;/sup> cm&lt;sup>-2&lt;/sup>s&lt;sup>-1&lt;/sup>. If the beams were to be collided head-on in the LHCb detector, this figure would be exceeded. Therefore the beams are initially separated by a few microns in the vertical plane and then, as the beam intensity decays during a fill, this separation is gently reduced to keep the luminosity constant at the acceptable maximum. This technique is known as 'luminosity levelling' and has been used successfully to deliver around 0.36 fb&lt;sup>-1&lt;/sup> to LHCb in 2011, well on the way to their target of 1 fb&lt;sup>-1&lt;/sup> for the year.&amp;nbsp;&amp;nbsp;&lt;/p> &lt;p>As expected, high beam intensities have introduced a number of issues including: UFOs, the effect of radiation on the electronics installed in the LHC tunnel; and beam-induced heating of some accelerator components. Understanding, and where possible mitigating, these effects is ongoing, hence the more sedate pace in pushing the beam intensity recently. The operations team has successfully pushed up the number of bunches per beam to 1236 and they hope to make the step up to 1380, the final target of 2011,&amp;nbsp;before the start of&amp;nbsp;next machine development (MD) period, on 29 June.  The MD sessions will be followed by a 5-day technical stop, which will take us to 8 July when operation for physics will start again.&lt;/p> &lt;p>&amp;nbsp;&lt;/p></subfield>
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    <subfield code="b">&lt;p class="articleHeader">Le LHC a maintenu le nombre de paquets par faisceau &amp;agrave; 1092 au cours des deux derni&amp;egrave;res semaines, et a fourni de la luminosit&amp;eacute; aux exp&amp;eacute;riences sans d&amp;eacute;semparer. La luminosit&amp;eacute; int&amp;eacute;gr&amp;eacute;e totale a d&amp;eacute;j&amp;agrave; franchi la barre des 1 fb&lt;sup>-1 &lt;/sup>(femtobarn inverse), ce qui &amp;eacute;tait l&amp;rsquo;objectif global pour l&amp;rsquo;ann&amp;eacute;e 2011. L'&amp;eacute;v&amp;eacute;nement a modestement &amp;eacute;t&amp;eacute; c&amp;eacute;l&amp;eacute;br&amp;eacute; au CCC, et il faudra d&amp;eacute;sormais attendre la fin de l'exploitation 2011 - ou atteindre les 5 fb&lt;sup>-1&lt;/sup> - pour les prochaines r&amp;eacute;jouissances.&lt;/p> &lt;p>&amp;nbsp;&lt;/p> &lt;div class="phlwithcaption"> &lt;div class="imageScale">&lt;a target="_blank" href="http://cds.cern.ch/record/1360708/files/LHCReport_image.png">&lt;img width="300" height="230" alt="" src="http://cds.cern.ch/record/1360708/files/LHCReport_image.png?subformat=icon" />&lt;/a>&lt;/div> &lt;/div> &lt;p>LHCb est un d&amp;eacute;tecteur con&amp;ccedil;u pour diff&amp;eacute;rents types de recherches, de celle conduites &amp;agrave; ATLAS &amp;agrave; celles men&amp;eacute;es &amp;agrave; CMS, et peut recevoir une luminosit&amp;eacute; de cr&amp;ecirc;te maximale d&amp;rsquo;environ 3x10&lt;sup>32&lt;/sup> cm&lt;sup>-2&lt;/sup>s&lt;sup>-1&lt;/sup>. Si les faisceaux entraient en collision de mani&amp;egrave;re frontale dans LHCb, cette limite serait d&amp;eacute;pass&amp;eacute;e.  Par cons&amp;eacute;quent, les faisceaux sont d&amp;rsquo;abord s&amp;eacute;par&amp;eacute;s de quelques microns dans le plan vertical et, ensuite, pour s'adapter &amp;agrave; la d&amp;eacute;croissance de l&amp;rsquo;intensit&amp;eacute; du faisceau au cours de l'injection, cette s&amp;eacute;paration est r&amp;eacute;duite progressivement de fa&amp;ccedil;on &amp;agrave; toujours maintenir la luminosit&amp;eacute; au maximum acceptable.  Cette technique, connue sous le nom d&amp;rsquo;&amp;eacute;galisation de la luminosit&amp;eacute;, a bien fonctionn&amp;eacute; en 2011, lorsque la machine a livr&amp;eacute; quelque 0,36 fb&lt;sup>-1&lt;/sup> &amp;agrave; LHCb, lequel est donc tr&amp;egrave;s bien parti pour atteindre son objectif de 1 fb&lt;sup>-1&lt;/sup> pour la totalit&amp;eacute; de l&amp;rsquo;ann&amp;eacute;e.&lt;/p> &lt;p>Comme nous nous y attendions, les intensit&amp;eacute;s de faisceau &amp;eacute;lev&amp;eacute;es ont entra&amp;icirc;n&amp;eacute; un certain nombre de probl&amp;egrave;mes, notamment les &amp;laquo; objets tombants non identifi&amp;eacute;s &amp;raquo;, l&amp;rsquo;effet des rayonnements sur l&amp;rsquo;&amp;eacute;lectronique install&amp;eacute;e dans le tunnel du LHC, et l&amp;rsquo;&amp;eacute;chauffement de certains &amp;eacute;l&amp;eacute;ments de l&amp;rsquo;acc&amp;eacute;l&amp;eacute;rateur provoqu&amp;eacute; par les faisceaux. Les &amp;eacute;quipes s&amp;rsquo;efforcent de mieux comprendre et, dans la mesure du possible, d&amp;rsquo;att&amp;eacute;nuer ces effets, c&amp;rsquo;est pourquoi l&amp;rsquo;augmentation de l&amp;rsquo;intensit&amp;eacute; se poursuit actuellement &amp;agrave; un rythme plus calme. L'&amp;eacute;quipe des op&amp;eacute;rations a fait passer avec succ&amp;egrave;s le nombre de paquets par faisceaux &amp;agrave; 1236, et elle esp&amp;egrave;re passer le cap des 1380, objectif final pour l'ann&amp;eacute;e 2011, avant le d&amp;eacute;but de la prochaine phase de d&amp;eacute;veloppement machine (MD) qui commencera le 29 juin prochain.  Les sessions MD seront suivies d&amp;rsquo;un arr&amp;ecirc;t technique de 5 jours, ce qui nous am&amp;egrave;nera au 8 juillet, date de la reprise des op&amp;eacute;rations pour la physique.&lt;/p></subfield>
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    <subfield code="b">&lt;!--HTML--> &lt;p class="articleHeader">On 29 May, yet another record was set as 1092 bunches per beam were injected into the LHC, hitting a peak luminosity of 1.26x10&lt;sup>33&lt;/sup> cm&lt;sup>-2&lt;/sup> s&lt;sup>-1&lt;/sup>. While running at 3.5 TeV each beam now packs a total energy of over 70 MJ &amp;ndash; equivalent to a TGV travelling at a 70 kph.&lt;/p> &lt;p>&amp;nbsp;&lt;/p> &lt;div class="phlwithcaption"> &lt;div class="imageScale">&lt;a href="http://cds.cern.ch/record/1357318/files/1105146_01-A4-at-144-dpi_image.jpg" target="_blank">&lt;img src="http://cds.cern.ch/record/1357318/files/1105146_01-A4-at-144-dpi_image.jpg?subformat=icon" alt="" />&lt;/a>&lt;/div> &lt;br /> Operators in the LHC Control Centre happily show off their display screens after succesfully injecting 1092 bunches injected into the machine for the first time.&amp;nbsp;&lt;/div> &lt;p>As the total beam intensity has been pushed up, the LHC has encountered a number of related problems, such as the so-called UFOs (Unidentified Falling Objects).  These are thought to be dust particles falling through the beam, causing localized beam loss. The losses can push nearby beam loss monitors over the threshold and dump the beam. This is more of an annoyance than a danger for the LHC, but UFOs do reduce the operational efficiency of the machine.&lt;/p> &lt;p>Despite this, the luminosity delivered to the experiments has steadily increased. On three occasions there have been over 40 inverse picobarns (pb&lt;sup>-1&lt;/sup>) delivered in a single fill. The total for the year, at the time of writing, stands at over 800 pb&lt;sup>-1&lt;/sup> or 0.80 inverse femtobarn (fb&lt;sup>-1&lt;/sup>) &amp;ndash; well on the way to the target for the year of 1 fb&lt;sup>-1&lt;/sup>. The program of the coming weeks is to push for even more luminosity, maximizing the total delivered to the experiments before the summer conferences.&lt;i>&lt;br /> &lt;/i>&lt;/p> &lt;hr /> &lt;script language="javascript" src="http://cdsweb.cern.ch/insertplayer.js" type="text/javascript">&lt;/script> &lt;script type="text/javascript"> var flash_video_player=get_video_player_path(); insert_player_for_external('Video/Public/Movies/2011/CERN-MOVIE-2011-079/CERN-MOVIE-2011-079-0753-kbps-640x360-25-fps-audio-64-kbps-44-kHz-stereo', 'mms://mediastream.cern.ch/MediaArchive/Video/Public/Movies/2011/CERN-MOVIE-2011-079/CERN-MOVIE-2011-079-0480-kbps-512x288-25-fps-audio-128-kbps-48-kHz-stereo.wmv', 'false', 480, 360, 'http://mediaarchive.cern.ch/MediaArchive/Video/Public/Movies/2011/CERN-MOVIE-2011-079/CERN-MOVIE-2011-079-posterframe-640x360-at-10-percent.jpg', '1354548', true); &lt;/script></subfield>
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    <subfield code="a">Unidentified falling objects (UFOs) are potentially a major luminosity limitation for nominal LHC operation. They are presumably micrometer sized dust particles which lead to fast beam losses when they interact with the beam. With large-scale increases and optimizations of the beam loss monitor (BLM) thresholds, their impact on LHC availability was mitigated from mid 2011 onwards. For higher beam energy and lower magnet quench limits, the problem is expected to be considerably worse, though. In 2011/12, the diagnostics for UFO events were significantly improved: dedicated experiments and measurements in the LHC and in the laboratory were made and complemented by FLUKA simulations and theoretical studies. The state of knowledge, extrapolations for nominal LHC operation and mitigation strategies are presented</subfield>
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    <subfield code="a">Comparison of ejection events in the jet and accretion disc outflows in 3C 111</subfield>
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    <subfield code="c">09 May 2012</subfield>
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    <subfield code="a">Comments: 9 pages, accepted for publication in MNRAS</subfield>
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    <subfield code="a">Comments: 9 pages, accepted for publication in MNRAS</subfield>
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    <subfield code="a">We present a comparison of the parameters of accretion disc outflows and the jet of the broad-line radio galaxy 3C 111 on sub-pc scales. We make use of published X-ray observations of ultra-fast outflows (UFOs) and new 43GHz VLBA images to track the jet knots ejection. We find that the superluminal jet coexists with the mildly relativistic outflows on sub-pc scales, possibly indicating a transverse stratification of a global flow. The two are roughly in pressure equilibrium, with the UFOs potentially providing additional support for the initial jet collimation. The UFOs are much more massive than the jet, but their kinetic power is probably about an order of magnitude lower, at least for the observations considered here. However, their momentum flux is equivalent and both of them are powerful enough to exert a concurrent feedback impact on the surrounding environment. A link between these components is naturally predicted in the context of MHD models for jet/outflow formation. However, given the high radiation throughput of AGNs, radiation pressure should also be taken into account. From the comparison with the long-term 2-10keV RXTE light curve we find that the UFOs are preferentially detected during periods of increasing flux. We also find the possibility to place the UFOs within the known X-ray dips-jet ejection cycles, which has been shown to be a strong proof of the disc-jet connection, in analogue with stellar-mass black holes. However, given the limited number of observations presently available, these relations are only tentative and additional spectral monitoring is needed to test them conclusively.</subfield>
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    <subfield code="a">Mike Lamont for the LHC Team</subfield>
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    <subfield code="a">... It’s a blooming miracle - a special LHC Report</subfield>
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    <subfield code="a">... C'est un pur miracle - spéciales "Dernières nouvelles du LHC"</subfield>
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    <subfield code="b">&lt;p class="articleHeader"> Wrestling a 27 km superconducting collider under control is not easy. Throw in high intensity beams and it can sometimes seem a continual, frustrating battle with the vagaries of a hugely complex problem space.&lt;/p> &lt;p> &amp;nbsp;&lt;/p> &lt;p> This problem space has been thoroughly explored over the last three or four years. The myriad of potential obstacles to smooth operation ranges from unidentified falling objects (UFOs), electron clouds, beam dynamics, radiation to electronics, vacuum instabilities, &amp;ldquo;transparent&amp;rdquo; software changes, Radio Frequency (RF) trips, electrical network glitches etc. etc. The huge extended systems, such as the beam loss monitors, cryogenics, and quench protection systems, have a phenomenal number of components that inevitably have occasional failures (there is, of course, a higher probability that these occur late Friday evening and over the weekend).&amp;nbsp;On the cryogenics front, cooling and keeping 36,000 tonnes of magnets at 1.9 K is a challenging prerequisite for everything else that follows.&lt;/p> &lt;p> Despite their complexity, we have very well behaved magnets and overall the machine is stable and magnetically reproducible. The magnets are well understood following a long and careful measurement campaign carried out during production. A sophisticated magnet model is even capable of dealing with the once feared dynamic effects. Together with the accuracy and stability of the power converters, our carefully optimized machine stays optimized. The injection, ramp and squeeze have been mastered and, as a general rule, injected beam makes it into collisions.&lt;/p> &lt;p> Exploitation of the LHC&amp;rsquo;s potential is helped by the presence of excellent beam instrumentation and powerful high-level software architecture. Together with some applied intelligence, these have allowed the development of tools (e.g. measurement and correction of optics, an on-line aperture model) which have opened the way to maximizing the performance of the machine. Most notably, accurate measurements of the aperture in the regions adjacent to the experiments have allowed us to reduce the beam size at the interaction points to unexpectedly low values. The better-than-expected aperture reflects good observance of tolerances during installation and very good alignment of all elements by the survey group.&lt;/p> &lt;p> The LHC has enjoyed from the start very good beam quality (both protons and ions)&amp;nbsp;from the injector complex. The bunch currents have been well above, and the beam sizes well below, the nominal values quoted in the design report. The production of beam in the LINAC, Booster, PS, and SPS is distinctly non-trivial and requires continual care and attention to maintain the beam parameters, however this diligence is reflected directly in delivered luminosity.&lt;/p> &lt;p> Naturally, a cautious approach marked the re-starting in November 2009 following recovery from the 2008 incident. This was most clearly reflected in the choice to run at an initial beam energy of 3.5 TeV. Having experienced first hand the destructiveness of magnetic energy, awareness of the damage potential of the beam to the machine has underpinned the operational approach and marked the subsequent evolution in beam intensity. The full and proper functioning of the extended machine protection system (MPS) has always been an absolute priority.&lt;/p> &lt;p> The MPS consists of a federation of inputs from various systems into a beam interlock system (BIS). When the BIS is triggered it provokes a beam dump within 3 to 4 turns (that is, in a few hundred millionths of a second). The MPS has worked flawlessly, always pulling a beam abort when called upon to do so.&lt;/p> &lt;p> In addition to the MPS, the beam drives a subtle interplay of the beam dump system, the collimation system and protection devices, all of which rely on a well-defined aperture, orbit and optics for guaranteed safe operation. Assuring this throughout high intensity operation remains paramount. Numerous interlocks are in place to ensure that posted limits are always respected.&lt;/p> &lt;p> One notable feature during LHC commissioning and operation is the collective ability of CERN teams to resolve problems. There is in-depth expertise and experience on all systems, including vacuum, collimation, RF, fast kicker magnets and so on. Serious issues, such as radiation to electronics, and the lack of redundancy in protection systems, are targeted rigorously as they become apparent.&amp;nbsp;&amp;nbsp;&lt;/p> &lt;p> Although precision and rigour are needed when dealing with the tightly synchronized choreography and the ever present dangers of magnetic and beam energy, an open and mostly friendly atmosphere pervades. A recent visitor to an 8:30 meeting noted the lack of defensiveness, and a willingness to directly engage a problem without needing to assign blame. There is amazing dedication from everybody involved. Problems that stop the operation of the machine happen anytime, with a slight preference for nighttime and the weekend. Despite this, there is unfailing support from all teams. Coming out of the technical stop this last weekend the Machine Protection and Electrical Integrity team worked until 5 in the morning on Saturday, and the control and timing teams were in from 2 to gone 6 on Sunday morning dealing with the effects of an innocent leap second.&lt;/p> &lt;p> Finally, trying to hold everything together across the accelerator complex is a talented, smart, moderately good-looking operations team who have necessarily developed an advanced sense of humour.&lt;/p> &lt;p> &lt;em>The LHC came out of a five-day technical stop on the evening of Friday 29 June. For real-time information on the operation of the machine, visit the &lt;a href="http://op-webtools.web.cern.ch/op-webtools/vistar/vistars.php" target="_blank">LHC Page 1&lt;/a> status page.&lt;/em>&lt;/p></subfield>
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    <subfield code="b">&lt;p class="articleHeader"> Parvenir &amp;agrave; dompter un collisionneur supraconducteur de 27 km n&amp;rsquo;est pas une mince affaire. Si de plus vous y injectez des faisceaux de haute intensit&amp;eacute;, vous vous trouverez aux prises avec les caprices d&amp;rsquo;un syst&amp;egrave;me d&amp;rsquo;une complexit&amp;eacute; extr&amp;ecirc;me.&lt;/p> &lt;p> &amp;nbsp;&lt;/p> &lt;p> Ce syst&amp;egrave;me hautement complexe a &amp;eacute;t&amp;eacute; explor&amp;eacute; de fond en comble au cours des trois ou quatre derni&amp;egrave;res ann&amp;eacute;es. Mille et un facteurs sont susceptibles de faire obstacle &amp;agrave; son bon fonctionnement : objets tombants non identifi&amp;eacute;s (UFO), nuages d&amp;rsquo;&amp;eacute;lectrons, dynamique du faisceau, effets des rayonnements sur l&amp;rsquo;&amp;eacute;lectronique, instabilit&amp;eacute;s du vide, modifications &amp;laquo; transparentes &amp;raquo; de logiciel, coupures de radiofr&amp;eacute;quence ou encore probl&amp;egrave;mes du r&amp;eacute;seau &amp;eacute;lectrique. Les gigantesques syst&amp;egrave;mes r&amp;eacute;partis, tels que les d&amp;eacute;tecteurs de perte de faisceau, la cryog&amp;eacute;nie et les syst&amp;egrave;mes de protection contre les transitions r&amp;eacute;sistives, sont constitu&amp;eacute;s d&amp;rsquo;un nombre ph&amp;eacute;nom&amp;eacute;nal d&amp;#39;&amp;eacute;l&amp;eacute;ments, qui ont in&amp;eacute;vitablement leurs d&amp;eacute;faillances occasionnelles (avec, bien &amp;eacute;videmment, une forte probabilit&amp;eacute; que celles-ci interviennent le vendredi en fin de soir&amp;eacute;e ou pendant le week-end). Du c&amp;ocirc;t&amp;eacute; de la cryog&amp;eacute;nie, refroidir et maintenir 36 000 tonnes d&amp;#39;aimants &amp;agrave; 1,9 K est un pr&amp;eacute;requis exigeant pour tout ce qui suit.&lt;/p> &lt;p> Malgr&amp;eacute; leur complexit&amp;eacute;, nos aimants se tiennent bien et, d&amp;rsquo;un point de vue g&amp;eacute;n&amp;eacute;ral, la machine est stable et pr&amp;eacute;sente une bonne reproductibilit&amp;eacute; du champ magn&amp;eacute;tique. Une longue campagne de mesures minutieuses, men&amp;eacute;e en p&amp;eacute;riode de production, nous a permis de bien comprendre le fonctionnement des aimants. Aujourd&amp;rsquo;hui, un mod&amp;egrave;le d&amp;rsquo;aimant tr&amp;egrave;s &amp;eacute;volu&amp;eacute; est m&amp;ecirc;me capable de g&amp;eacute;rer les effets dynamiques qui &amp;eacute;taient autrefois redout&amp;eacute;s. Gr&amp;acirc;ce &amp;agrave; la pr&amp;eacute;cision et &amp;agrave; la stabilit&amp;eacute; des convertisseurs de puissance, notre machine, qui a &amp;eacute;t&amp;eacute; optimis&amp;eacute;e avec soin, reste optimis&amp;eacute;e. L&amp;rsquo;injection, la mont&amp;eacute;e en &amp;eacute;nergie et la compression sont maintenant ma&amp;icirc;tris&amp;eacute;es et, en r&amp;egrave;gle g&amp;eacute;n&amp;eacute;rale, les faisceaux inject&amp;eacute;s arrivent &amp;agrave; entrer en collision.&lt;/p> &lt;p> L&amp;rsquo;exploitation des possibilit&amp;eacute;s qu&amp;rsquo;offre le LHC est facilit&amp;eacute;e par la pr&amp;eacute;sence d&amp;rsquo;une excellente instrumentation de faisceau et d&amp;rsquo;une puissante architecture de logiciels de haut niveau. Appliqu&amp;eacute;es avec intelligence, celles-ci ont permis de mettre au point des outils (par exemple pour la mesure et la correction de l&amp;rsquo;optique ou un mod&amp;egrave;le d&amp;rsquo;ouverture en ligne) gr&amp;acirc;ce auxquels la performance de la machine a &amp;eacute;t&amp;eacute; optimis&amp;eacute;e. Surtout, gr&amp;acirc;ce &amp;agrave; des mesures pr&amp;eacute;cises de l&amp;rsquo;ouverture dans les zones adjacentes aux exp&amp;eacute;riences, nous avons pu r&amp;eacute;duire &amp;agrave; des valeurs remarquablement basses les dimensions du faisceau aux points d&amp;rsquo;interaction. L&amp;rsquo;am&amp;eacute;lioration inesp&amp;eacute;r&amp;eacute;e de l&amp;rsquo;ouverture peut &amp;ecirc;tre mise sur le compte du respect des tol&amp;eacute;rances au cours de l&amp;rsquo;installation et d&amp;rsquo;un tr&amp;egrave;s bon alignement des &amp;eacute;l&amp;eacute;ments par le groupe M&amp;eacute;trologie.&lt;/p> &lt;p> Le LHC a b&amp;eacute;n&amp;eacute;fici&amp;eacute; d&amp;egrave;s le d&amp;eacute;part de l&amp;rsquo;excellente qualit&amp;eacute; du faisceau (de protons et d&amp;#39;ions) produit par le complexe d&amp;rsquo;injecteurs. Par rapport aux valeurs nominales pr&amp;eacute;vues dans le rapport de conception, l&amp;rsquo;intensit&amp;eacute; des paquets est bien plus grande et la taille des faisceaux est bien plus petite. La production du faisceau dans le LINAC, le Booster du PS, le PS et le SPS est loin d&amp;rsquo;&amp;ecirc;tre un jeu d&amp;rsquo;enfant et exige un soin et une attention de tous les instants pour maintenir les param&amp;egrave;tres du faisceau. Or, la luminosit&amp;eacute; obtenue en d&amp;eacute;pend directement.&lt;/p> &lt;p> Naturellement, apr&amp;egrave;s les travaux de remise en &amp;eacute;tat qui ont fait suite &amp;agrave; l&amp;rsquo;incident de 2008, le red&amp;eacute;marrage de novembre 2009 s&amp;rsquo;est fait sous le signe de la prudence. Cela s&amp;rsquo;est surtout traduit par le choix d&amp;rsquo;exploiter la machine &amp;agrave; une &amp;eacute;nergie de faisceau initiale de 3,5 TeV. Ayant fait l&amp;rsquo;exp&amp;eacute;rience directe de la destructivit&amp;eacute; de l&amp;rsquo;&amp;eacute;nergie stock&amp;eacute;e dans les aimants, nous &amp;eacute;tions aussi conscients du potentiel destructeur du faisceau pour la machine, ce qui nous a incit&amp;eacute;s &amp;agrave; opter pour le mode d&amp;rsquo;exploitation que nous avons choisi et a d&amp;eacute;termin&amp;eacute; l&amp;rsquo;&amp;eacute;volution ult&amp;eacute;rieure de l&amp;rsquo;intensit&amp;eacute; du faisceau. Pouvoir tirer pleinement parti du syst&amp;egrave;me de protection de la machine (MPS) a toujours &amp;eacute;t&amp;eacute; une priorit&amp;eacute;.&lt;br /> &lt;br /> Le MPS met &amp;agrave; contribution divers syst&amp;egrave;mes pour produire un m&amp;eacute;canisme de verrouillage du faisceau (BIS). Quand le BIS s&amp;rsquo;active, il provoque une &amp;eacute;jection du faisceau en 3 &amp;agrave; 4 tours (soit en quelques centaines de microsecondes). Le MPS fonctionne impeccablement, imposant un arr&amp;ecirc;t du faisceau chaque fois que cela est n&amp;eacute;cessaire.&lt;/p> &lt;p> Outre l&amp;rsquo;apport du MPS, le faisceau impose une interaction subtile entre le syst&amp;egrave;me d&amp;rsquo;&amp;eacute;jection du faisceau, le syst&amp;egrave;me de collimation et les dispositifs de protection, dont le bon fonctionnement repose sur une bonne d&amp;eacute;finition de l&amp;rsquo;ouverture, de l&amp;rsquo;orbite et de l&amp;rsquo;optique. Se plier &amp;agrave; ces exigences tout au long de l&amp;rsquo;exploitation haute intensit&amp;eacute; reste d&amp;#39;une importance capitale. De nombreux verrous ont &amp;eacute;t&amp;eacute; &amp;eacute;tablis pour faire en sorte que les limites d&amp;eacute;finies soient toujours respect&amp;eacute;es.&lt;/p> &lt;p> La mise en service et l&amp;#39;exploitation du LHC ont &amp;eacute;t&amp;eacute; marqu&amp;eacute;es par la capacit&amp;eacute; des &amp;eacute;quipes du CERN de r&amp;eacute;soudre ensemble les probl&amp;egrave;mes. Les &amp;eacute;quipes poss&amp;egrave;dent des comp&amp;eacute;tences tr&amp;egrave;s pouss&amp;eacute;es et une exp&amp;eacute;rience approfondie de leurs syst&amp;egrave;mes respectifs, en particulier dans le domaine du vide, de la collimation, de la radiofr&amp;eacute;quence et des aimants de d&amp;eacute;flexion rapide, pour n&amp;rsquo;en citer que quelques-uns. Les probl&amp;egrave;mes tels que les effets des rayonnements sur l&amp;rsquo;&amp;eacute;lectronique et le manque de redondance dans les syst&amp;egrave;mes de protection, sont cibl&amp;eacute;s avec la plus grande rigueur &amp;agrave; mesure qu&amp;rsquo;ils apparaissent.&lt;/p> &lt;p> Malgr&amp;eacute; la pr&amp;eacute;cision et la rigueur n&amp;eacute;cessaires pour r&amp;eacute;gler le ballet des faisceaux &amp;eacute;troitement synchronis&amp;eacute;s et les dangers permanents li&amp;eacute;s &amp;agrave; l&amp;rsquo;&amp;eacute;nergie stock&amp;eacute;e dans les aimants et &amp;agrave; l&amp;rsquo;&amp;eacute;nergie du faisceau, il r&amp;egrave;gne un esprit d&amp;#39;ouverture et une atmosph&amp;egrave;re le plus souvent amicale. R&amp;eacute;cemment, un visiteur ayant assist&amp;eacute; &amp;agrave; une de nos r&amp;eacute;unions de 8 h 30 relevait l&amp;rsquo;absence d&amp;rsquo;attitude d&amp;eacute;fensive et la volont&amp;eacute; de s&amp;rsquo;attaquer directement au probl&amp;egrave;me sans chercher &amp;agrave; bl&amp;acirc;mer quiconque. Le d&amp;eacute;vouement des uns et des autres est tout simplement impressionnant. Les probl&amp;egrave;mes entra&amp;icirc;nant un arr&amp;ecirc;t de l&amp;rsquo;exploitation peuvent survenir n&amp;rsquo;importe quand, avec une l&amp;eacute;g&amp;egrave;re pr&amp;eacute;f&amp;eacute;rence pour la nuit et les week-ends. Quoi qu&amp;rsquo;il en soit, toutes les &amp;eacute;quipes donnent le meilleur d&amp;rsquo;elles-m&amp;ecirc;mes en tout temps. Pour parachever l&amp;rsquo;arr&amp;ecirc;t technique du week-end dernier, l&amp;rsquo;&amp;eacute;quipe charg&amp;eacute;e de la protection des machines et de l&amp;rsquo;int&amp;eacute;grit&amp;eacute; &amp;eacute;lectrique a travaill&amp;eacute; jusqu&amp;rsquo;&amp;agrave; cinq heures samedi matin et les &amp;eacute;quipes responsables du contr&amp;ocirc;le et du cadencement &amp;eacute;taient au poste dimanche entre deux heures et six heures du matin pour g&amp;eacute;rer les effets d&amp;rsquo;une simple seconde intercalaire.&lt;br /> &lt;br /> Enfin, rien ne serait possible dans le complexe d&amp;rsquo;acc&amp;eacute;l&amp;eacute;rateurs sans la contribution d&amp;rsquo;une &amp;eacute;quipe d&amp;rsquo;op&amp;eacute;rateurs talentueux, intelligents et plut&amp;ocirc;t beaux, et qui ont bien s&amp;ucirc;r d&amp;ucirc; d&amp;eacute;velopper un sens de l&amp;rsquo;humour tr&amp;egrave;s pointu.&lt;/p> &lt;p> &lt;em>Le LHC a repris ses op&amp;eacute;rations le vendredi 29 juin, apr&amp;egrave;s un arr&amp;ecirc;t technique de cinq jours. Pour obtenir des informations en temps r&amp;eacute;el sur le fonctionnement de la machine, consultez la page&lt;/em>&lt;em>&amp;nbsp;&lt;a href="http://op-webtools.web.cern.ch/op-webtools/vistar/vistars.php" target="_blank">LHC 1&lt;/a>.&lt;/em>&lt;/p></subfield>
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