Proton Synchrotron Division

Total Page:16

File Type:pdf, Size:1020Kb

Proton Synchrotron Division Proton Synchrotron Division Introduction Following the celebration of the 40th anniversary of the PS at the end of 1999, the synchrotron this year entered its fifth decade of operation as CERN’s workhorse accelerator. The Division was once again fully occupied supplying its usual multitude of beams to the users, nevertheless finding time to work on other exciting subjects not directly linked to today’s beams, and including essential R&D aimed at the very long- term future of CERN. Nowhere else in CERN does one find such a diversity of topics being studied and machines being operated, which is what makes the Division so attractive. In April the ISOLDE technical team was welcomed into the Division, it having been decided by the CERN management that PS would be a more logical home for ISOLDE operation and development than its former home, EP Division. Then at the end of the year a group of RF experts from SL Division was also welcomed into the Division. Since it was no longer necessary to coax the best performance from LEP’s superconducting cavities after the closure of that machine, this team will become the nucleus for the construction of the new CTF3 test facility. The highlights of the year with regard to beams were the commissioning of the Antiproton Decelerator (AD) and the start-up of the neutron Time-Of-Flight (nTOF) facility. Both had been eagerly awaited by the physicists, who obtained exactly what they were expecting, although perhaps with just a slight delay. The year also saw the end of a decade of electrons/positrons in the PS for LEP, and the best run ever for heavy ions. This latter run was scheduled originally as the last, but it has now been agreed that ions will come back again in 2002/3, and of course later for the LHC. Work continued on improving the proton beam needed in the future by the LHC, and during this time a new intensity record was established for protons in the PS, and extracted from it. In summary, the year 2000 was an excellent one for the PS and for the Division. Operation Operating statistics for the different particle beams in the PS Complex in 2000 are presented in the tables below. Proton Synchrotron Division 185 Operational statistics for lepton operation in 2000 Total number of hours scheduled for lepton operation, including expt. areas 6787 h Total number of hours achieved for lepton operation 6573 h Hours scheduled for lepton production for SPS/LEP, including setting up in PS 5242 h Hours achieved for lepton production for SPS/LEP 5041 h Electrons supplied to SPS/LEP 1.50 × 1017 Positrons supplied to SPS/LEP 1.38 × 1017 Operational statistics for proton operation in 2000 Total number of hours scheduled for proton operation 6477 h Hours scheduled for setting-up and machine development 441 h Hours scheduled for proton production for SPS 4038 h Hours achieved for proton production for SPS 3832 h Protons produced for SPS (at PSB extraction) 1.76 × 1019 Protons produced for SPS (at PS extraction) 1.59 × 1019 Protons for machine studies (at PSB extraction) 1.99 × 1018 Protons for AD (at PSB extraction) 2.62 × 1018 Protons for East Hall test beams (at PSB extraction) 7.74 × 1017 Hours scheduled for ISOLDE operation 3224 h Hours achieved for ISOLDE operation 3136 h Protons supplied by PSB for ISOLDE operation 8.73 × 1019 Operational statistics for Pb-ion operation in 2000 Hours scheduled for ion production for SPS 1184 h Hours achieved for ion production for SPS 1138 h Total charges of Pb53+ ions for SPS (at PSB extraction) 1.91 × 1016 Total charges of Pb53+ ions for SPS (at PS extraction) 1.4 × 1016 Operational statistics for AD operation in 2000 Hours scheduled for AD operation for physics 1482 h Hours achieved for AD operation for physics 1272 h The Proton Run from March to September The PS Complex started up at the beginning of March as usual, following the annual shutdown. The LPI machine was the first into action, but the proton Linac 2, the PS Booster and the PS itself were not far behind. Leptons were injected into the PS on 13 March with the protons following soon after. However, it quickly became apparent that there were some timing or synchronization difficulties affecting all machines. These problems were soon traced to an unforeseen instability in the TG8 timing units, which had been modified during the shutdown; the PS Complex has about 250 of them. When laboratory tests revealed that the problem could not be resolved easily, it was decided to go back to the old hardware/software configuration for each of 186 Proton Synchrotron Division the 250 units. Thanks to a big effort from the Controls group this change was made in less than a week, and the delivery of beam to users was not delayed. LEP began operation on 3 April, and the East Hall beams were delivered as planned a week later. ISOLDE was also scheduled to begin operation then, and for ISOLDE this start-up was an important one as it was their first as part of PS Division. All went as planned and the PSB beams at 1.0 and 1.4 GeV, with nominal intensity up to 3 × 1013 protons/pulse, were sent to the ISOLDE target by mid-April. ISOLDE started by using the GPS target station, but one of the big priorities for the first half of 2000 was to complete the commissioning of the second separator (the HRS). This is important if 400 shifts of beam time are to be delivered to the ISOLDE users per year, as promised. This important milestone was passed at the end of May when the first scheduled HRS physics run took place. The SPS proton physics programme was scheduled to start a week after Easter, but this did not mean that the SPS was idle until then. The PS had to supply a number of specialized Machine Development (MD) beams to the SPS machine physicists as part of the preparation of the SPS for LHC. On 2 May, the SPS began fixed- target physics operation with protons. This operation normally uses the standard five-turn proton extraction at 14 GeV from the PS. However this year, the SPS scheduled a two-week physics run to test some components of LHC detectors. These tests required the SPS to extract beam at 450 GeV, with the LHC-style 25 ns bunch spacing. As this bunch spacing is established in the PS, it was decided to perform this test run using a test version of the LHC beam in the PS, instead of the standard SPS proton beam. This mode of operation was extremely successful and will probably be repeated for similar runs in the future. AD commissioning started on time although there had been a serious vacuum leak on a stochastic cooling kicker, and some alignment and vacuum problems with the electron cooler. However, this did not stop the AD team making excellent progress, and the goal of decelerating antiprotons to 100 MeV/c using both stochastic and electron cooling was successfully achieved by July. The AD requires two beams from the PS. First the machine is set up using 3.5 GeV/c protons, which are injected in the ‘wrong’ direction around the AD machine (i.e. they circulate anticlockwise). This has the advantage that the AD can be optimized for deceleration with a relatively intense proton beam rather than with low-intensity antiprotons. However, the beam cooling systems do not work in this mode. Therefore, the transverse emittance of the 3.5 GeV beam has to be very delicately controlled in the PSB and the PS, to allow subsequent deceleration in the AD. Then, to produce antiprotons, the AD needs a high-intensity 26 GeV proton beam incident on the antiproton production target. This beam is produced by injecting four PSB bunches into half of the PS circumference and then compressing them into a quarter of the circumference, just before ejection from the PS. This new scheme was made operational during the PS start-up and 1.5 × 1013 protons at 26 GeV were available for antiproton production for AD right from the start. Every 12 weeks or so, the PS main power supply needs some regular maintenance because it is rotating machinery (and is now more than 30 years old). A 10-hour technical stop was scheduled for 7 June, in the shadow of which other interventions were carried out, including a large amount of scheduled (and unscheduled) vacuum work on Linac 2, the PSB and the PS. All the PS Complex water stations were also stopped for routine maintenance and inspection. In spite of the large amount of work carried out, all the beams were back again by early evening. For the PS, this was simply a continuation of what had been already operational: protons for SPS, leptons for SPS/LEP, slow extracted beams for DIRAC and the other East Hall experiments, the AD production beam, and a number of MD beams for both PS and SPS studies. At the Proton Synchrotron Division 187 Booster, the ISOLDE programme at the GPS station was in full swing and, throughout June and July, the commissioning tests of the HRS continued. During June, a lot of effort was put into completing the commissioning of the AD machine, in order to meet the re-scheduled deadline for starting AD physics on 10 July. By 14 July, the ASACUSA team was able to announce that it had made ‘a complete scan of a 597 nm resonance’.
Recommended publications
  • Proton Driven Plasma Wakefield Acceleration in AWAKE
    Proton Driven Plasma Article submitted to journal Wakefield Acceleration in Subject Areas: AWAKE Plasma Wakefield Acceleration, 1 1 Proton Driven, Electron Acceleration E. Gschwendtner , M. Turner , **Author List Continues Next Page** Keywords: AWAKE, Plasma Wakefield Acceleration, Seeded Self Modulation In this article, we briefly summarize the experiments Author for correspondence: performed during the first Run of the Advanced Insert corresponding author name Wakefield Experiment, AWAKE, at CERN (European e-mail: [email protected] Organization for Nuclear Research). The final goal of AWAKE Run 1 (2013 - 2018) was to demonstrate that 10-20 MeV electrons can be accelerated to GeV- energies in a plasma wakefield driven by a highly- relativistic self-modulated proton bunch. We describe the experiment, outline the measurement concept and present first results. Last, we outline our plans for the future. 1 Continued Author List 2 E. Adli2,A. Ahuja1,O. Apsimon3;4,R. Apsimon3;4, A.-M. Bachmann1;5;6,F. Batsch1;5;6 C. Bracco1,F. Braunmüller5,S. Burger1,G. Burt7;4, B. Buttenschön8,A. Caldwell5,J. Chappell9, E. Chevallay1,M. Chung10,D. Cooke9,H. Damerau1, L.H. Deubner11,A. Dexter7;4,S. Doebert1, J. Farmer12, V.N. Fedosseev1,R. Fiorito13;4,R.A. Fonseca14,L. Garolfi1,S. Gessner1, B. Goddard1, I. Gorgisyan1,A.A. Gorn15;16,E. Granados1,O. Grulke8;17, A. Hartin9,A. Helm18, J.R. Henderson7;4,M. Hüther5, M. Ibison13;4,S. Jolly9,F. Keeble9,M.D. Kelisani1, S.-Y. Kim10, F. Kraus11,M. Krupa1, T. Lefevre1,Y. Li3;4,S. Liu19,N. Lopes18,K.V. Lotov15;16, M. Martyanov5, S.
    [Show full text]
  • The Large Hadron Collider Lyndon Evans CERN – European Organization for Nuclear Research, Geneva, Switzerland
    34th SLAC Summer Institute On Particle Physics (SSI 2006), July 17-28, 2006 The Large Hadron Collider Lyndon Evans CERN – European Organization for Nuclear Research, Geneva, Switzerland 1. INTRODUCTION The Large Hadron Collider (LHC) at CERN is now in its final installation and commissioning phase. It is a two-ring superconducting proton-proton collider housed in the 27 km tunnel previously constructed for the Large Electron Positron collider (LEP). It is designed to provide proton-proton collisions with unprecedented luminosity (1034cm-2.s-1) and a centre-of-mass energy of 14 TeV for the study of rare events such as the production of the Higgs particle if it exists. In order to reach the required energy in the existing tunnel, the dipoles must operate at 1.9 K in superfluid helium. In addition to p-p operation, the LHC will be able to collide heavy nuclei (Pb-Pb) with a centre-of-mass energy of 1150 TeV (2.76 TeV/u and 7 TeV per charge). By modifying the existing obsolete antiproton ring (LEAR) into an ion accumulator (LEIR) in which electron cooling is applied, the luminosity can reach 1027cm-2.s-1. The LHC presents many innovative features and a number of challenges which push the art of safely manipulating intense proton beams to extreme limits. The beams are injected into the LHC from the existing Super Proton Synchrotron (SPS) at an energy of 450 GeV. After the two rings are filled, the machine is ramped to its nominal energy of 7 TeV over about 28 minutes. In order to reach this energy, the dipole field must reach the unprecedented level for accelerator magnets of 8.3 T.
    [Show full text]
  • CERN Intersecting Storage Rings (ISR)
    Proc. Nat. Acad. Sci. USA Vol. 70, No. 2, pp. 619-626, February 1973 CERN Intersecting Storage Rings (ISR) K. JOHNSEN CERN It has been realized for many years that it would be possible to beams of protons collide with sufficiently high interaction obtain a glimpse into a much higher energy region for ele- rates for feasible experimentation in an energy range otherwise mentary-particle research if particle beams could be persuaded unattainable by known techniques except at enormous cost. to collide head-on. A group at CERN started investigating this possibility in To explain why this is so, let us consider what happens in a 1957, first studying a special two-way fixed-field alternating conventional accelerator experiment. When accelerated gradient (FFAG) accelerator and then, in 1960, turning to the particles have reached the required energy they are directed idea of two intersecting storage rings that could be fed by the onto a target and collide with the stationary particles of the CERN 28 GeV proton synchrotron (CERN-PS). This change target. Most of the energy given to the accelerated particles in concept for these initial studies was stimulated by the then goes into keeping the particles that result from the promising performance of the CERN-PS from the very start collision moving in the direction of the incident particles (to of its operation in 1959. conserve momentum). Only a quite modest fraction is "useful After an extensive study that included building an electron energy" for the real purpose of the experiment-the trans- storage ring (CESAR) to investigate many of the associated formation of particles, the creation of new particles.
    [Show full text]
  • Femtoscopy of Proton-Proton Collisions in the ALICE Experiment
    Femtoscopy of proton-proton collisions in the ALICE experiment DISSERTATION Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of The Ohio State University By Nicolas Bock, B.Sc. B.Eng., M.Sc. Graduate Program in Physics The Ohio State University 2011 Dissertation Committee: Professor Thomas J. Humanic, Advisor Professor Michael Lisa #1 Professor Klaus Honscheid #2 Professor Richard Furnstahl #3 c Copyright by Nicolas Bock 2011 Abstract The Large Ion Collider Experiment (ALICE) at CERN has been designed to study matter at extreme conditions of temperature and pressure, with the long term goal of observing deconfined matter (free quarks and gluons), study its properties and learn more details about the phase diagram of nuclear matter. The ALICE experiment provides excellent particle tracking capabilities in high multiplicity proton-proton and heavy ion collisions, allowing to carry out detailed research of nuclear matter. This dissertation presents the study of the space time structure of the particle emission region, also known as femtoscopy, in proton- proton collisions at 0.9, 2.76 and 7.0 TeV. The emission region can be characterized by taking advantage of the Bose-Einstein effect for identical particles, which causes an enhancement of produced identical pairs at low relative momentum. The geometry of the emission region is related to the relative momentum distribution of all pairs by the Fourier transform of the source function, therefore the measurement of the final relative momentum distribution allows to extract the initial space-time characteristics. Results show that there is a clear dependence of the femtoscopic radii on event multiplicity as well as transverse momentum, a signature of the transition of nuclear matter into its fundamental components and also of strong interaction among these.
    [Show full text]
  • The Birth and Development of the First Hadron Collider the Cern Intersecting Storage Rings (Isr)
    Subnuclear Physics: Past, Present and Future Pontifical Academy of Sciences, Scripta Varia 119, Vatican City 2014 www.pas.va/content/dam/accademia/pdf/sv119/sv119-hubner.pdf The BirtTh a nd D eve lopment o f the Fir st Had ron C ollider The CERN Intersecting Storage Rings (ISR) K. H ÜBNER , T.M. T AYLOR CERN, 1211 Geneva 23, Switzerland Abstract The CERN Intersecting Storage Rings (ISR) was the first facility providing colliding hadron beams. It operated mainly with protons with a beam energy of 15 to 31 GeV. The ISR were approved in 1965 and were commissioned in 1971. This paper summarizes the context in which the ISR emerged, the design and approval phase, the construction and the commissioning. Key parameters of its performance and examples of how the ISR advanced accelerator technology and physics are given. 1. Design and approval The concept of colliding beams was first published in a German patent by Rolf Widerøe in 1952, but had already been registered in 1943 (Widerøe, 1943). Since beam accumulation had not yet been invented, the collision rate was too low to be useful. This changed only in 1956 when radio-frequency (rf) stacking was proposed (Symon and Sessler, 1956) which allowed accumulation of high-intensity beams. Concurrently, two realistic designs were suggested, one based on two 10 GeV Fixed-Field Alternating Gradient Accelerators (FFAG) (Kerst, 1956) and one suggesting two 3 GeV storage rings with synchrotron type magnet structure (O’Neill, 1956); in both cases the beams collided in one common straight section. The idea of intersecting storage rings to increase the number of interaction points appeared later (O’Neill, 1959).
    [Show full text]
  • Proton Synchrotron
    PROTON SYNCHROTRON 1. Introduction of the machine. The earliest operational runs were carried out without any of the correcting devices The 25 GeV proton synchrotron has now been being employed, except for the self-powered pole put into operation. Towards the end of November face windings needed to correct eddy currents in 1959 protons were accelerated up to 24 GeV kinetic the metal vacuum chamber at injection when the energy and a few weeks later, after adjustments guiding magnetic field is only 140 gauss. The had been made to the shape of the magnetic field proton beam then disappeared at a magnetic field at field values above 12 OOO gauss by means of pole of about 12 kgauss due to the number of free face windings, the maximum energy was increased oscillations of the particles per revolution becoming to 28 GeV. The intensity of the accelerated beam an integer. As the magnet yoke saturates, the focus­ of protons was measured as 1010 protons per pulse ing forces diminish slightly, and instead of the and there was no noticeable loss of particles during machine working in the stable region between the the whole acceleration period up to the maximum unstable resonance bands, the operating point is energy. slowly forced into a resonance and the particles Measurements so far carried out on the PS are are lost to the walls of the vacuum chamber. In necessarily preliminary and incomplete. It will take later runs the pole face windings were energized by at least six months of measurement work before programmed generators designed to keep the sufficient is known about the behaviour of the ma­ focusing forces constant up to magnetic fields of chine to exploit it as a working nuclear physics tool.
    [Show full text]
  • Improving the Slow Extraction Efficiency of the CERN Super
    Improving the slow extraction efficiency of the CERN Super Proton Synchrotron Brunner Kristóf Faculty of Science Eötvös Loránd University Supervisors: Barna Dániel, Wigner RCP Christoph Wiesner, CERN May 2018 Contents 1 Introduction4 2 CERN accelerator complex5 2.1 Accelerators..................................... 5 2.2 Experiments..................................... 6 2.2.1 Colliders .................................. 7 2.2.2 Fixed target experiments.......................... 7 2.3 Current and future demands of fixed target experiments.............. 7 3 Introduction to accelerator physics9 3.1 History of linear and circular accelerators ..................... 9 3.2 Design orbit, focusing................................. 11 3.3 Betatron oscillation, the behaviour of single particles ................ 11 3.4 The Twiss-ellipse, the behaviour of the beam ................... 13 3.5 Normalised phase space............................... 15 3.6 Tune and resonances ................................ 16 4 Extraction from a synchrotron 19 4.1 Fast extraction.................................... 19 4.2 Multi-turn extraction ................................ 20 4.3 Sextupole driven slow extraction........................... 21 4.4 Possible enhancements............................... 24 4.4.1 Diffuser................................... 24 4.4.2 Dynamic bump............................... 26 4.4.3 Phase space folding............................. 26 5 Massless septum 28 5.1 Method of phase space folding using a massless septum.............. 29 6 Simulation
    [Show full text]
  • Beam Monitoring System for the ATLAS Experiment at CERN
    Department of Physics, Chemistry and Biology Master’s Thesis Phase and Intensity Monitoring of the Particle Beams at the ATLAS Experiment Christian Ohm LITH-IFM-EX--07/1808--SE CERN-THESIS-2007-055 24/05/2007 Department of Physics, Chemistry and Biology Linköpings universitet SE-581 83 Linköping, Sweden Master’s Thesis LITH-IFM-EX--07/1808--SE Phase and Intensity Monitoring of the Particle Beams at the ATLAS Experiment Christian Ohm Supervisor: Thilo Pauly CERN Examiner: Patrick Norman ifm, Linköpings universitet Linköping, 24 May, 2007 Avdelning, Institution Datum Division, Department Date Division of Computational Physics Department of Physics, Chemistry and Biology 2007-05-24 Linköpings universitet SE-581 83 Linköping, Sweden Språk Rapporttyp ISBN Language Report category — Svenska/Swedish Licentiatavhandling ISRN Engelska/English Examensarbete LITH-IFM-EX--07/1808--SE C-uppsats Serietitel och serienummer ISSN D-uppsats Title of series, numbering — Övrig rapport URL för elektronisk version http://urn.kb.se/resolve?urn=urn:nbn:se:liu:diva-9614 Titel Intensitets- och fasövervakningssystem för partikelstrålarna vid ATLAS- Title experimentet Phase and Intensity Monitoring of the Particle Beams at the ATLAS Experiment Författare Christian Ohm Author Sammanfattning Abstract At the ATLAS experiment at CERN’s Large Hadron Collider, bunches of protons will cross paths at a rate of 40 MHz, resulting in 14 TeV head-on collisions. During these interactions, calorimeters, spectrometers and tracking detectors will look for evidence that can confirm or disprove theories about the smallest constituents of matter and the forces that hold them together. In order for these sub-detectors to sample the signals from exotic particles correctly, they rely on a constant phase between a clock signal and the bunch crossings in the experiment.
    [Show full text]
  • Synchro-Cyclotronsynchro-Cyclotron
    SYNCHRO-CYCLOTRONSYNCHRO-CYCLOTRON A BRIEF INTRODUCTION - ORIGINS, PRINCIPLE - PAST SYNCHROCYCLOTRONS - SYNCHROCYCLOTRON TODAY In real life... CERN 600 MeV SC McMillan's patent A way to apply the brand new concept of “phase stability”, using existing technology - the cyclotron (weak focusing, dB/dr<0) The oscillating electric voltage is applied to a (unique) dee Its frequency decreases with increasing energy Thus voltage can be much lower compared to cyclotron, ~kVs : easier technology than ~100skV → many more turns needed ~105 vs. 100s– not a problem Yet, drawback: - acceleration is to be cycled, - only ions with correct, accelerating, phase (a few 10s degrees of a 360 degree period) are “captured” by the voltage wave → much lower average current The acceleration of the ions takes place twice per turn. At the outer edge, an electrostatic deflector extracts the ion beam. The first synchrocyclotron produced 195 MeV deuterons and 390 MeV α-particles. Mid. 1950s: a typical nuclear Orsay 1 kHz synchrocyclotron physics research installtion 1958: first beam from the 157 MeV synchro-cyclotron 1975: shut-down for evolution to 200 MeV synchro-cylco 1993: installation converted to a hadrontherapy hospital, “IC- CPO” : Institut Curie-Centre de Protontherapie d'Orsay, one of the two in France 2010: synchro-cyclo stopped, proton-therapy persued with an IBA C250 cyclotron CERN Synchrocyclotron (SC) 1957: construction. CERN’s first accelerator, provided beams for CERN's first experiments in particle and nuclear physics, up to 600 MeV. 1964: started to concentrate on nuclear physics, leaving particle physics to the newer, 30 GeV, Proton Synchrotron. 1967: start supplying beams for the radioactive-ion-beam facility ISOLDE (nuclear physics, astrophysics, Medical.) 1990: SC closed, after 33 years of service.
    [Show full text]
  • Introduction to Accelerators: Evolution of Accelerators and Modern Day Applications
    Lecture 1 Introduction to Accelerators: Evolution of Accelerators and Modern Day Applications Sarah Cousineau, Jeff Holmes, Yan Zhang USPAS January, 2011 What are accelerators used for? • Particle accelerators are devices that produce energetic beams of particles which are used for – Understanding the fundamental building blocks of nature and the forces that act upon them (nuclear and particle physics) – Understanding the structure and dynamics of materials and their properties (physics, chemistry, biology, medicine) – Medical treatment of tumors and cancers – Production of medical isotopes – Sterilization – Ion Implantation to modify the surface of materials • There is active, ongoing work to utilize particle accelerators for – Transmutation of nuclear waste – Generating power more safely in sub-critical nuclear reactors Accelerators by the Numbers World wide inventory of accelerators, in total 15,000. The data have been collected by W. Scarf and W. Wiesczycka (See U. Amaldi Europhysics News, June 31, 2000) Category Number Ion implanters and surface modifications 7,000 Accelerators in industry 1,500 Accelerators in non-nuclear research 1,000 Radiotherapy 5,000 Medical isotopes production 200 Hadron therapy 20 Synchrotron radiation sources 70 Nuclear and particle physics research 110 The most well known category of accelerators – particle physics research accelerators – is one of the smallest in number. The technology for other types of accelerators was born from these machines. Nuclear and Particle Physics • Much of what we know about
    [Show full text]
  • ATLAS Experiment 1 ATLAS Experiment
    ATLAS experiment 1 ATLAS experiment Large Hadron Collider (LHC) LHC experiments ATLAS A Toroidal LHC Apparatus CMS Compact Muon Solenoid LHCb LHC-beauty ALICE A Large Ion Collider Experiment TOTEM Total Cross Section, Elastic Scattering and Diffraction Dissociation LHCf LHC-forward MoEDAL Monopole and Exotics Detector At the LHC LHC preaccelerators p and Pb Linear accelerators for protons (Linac 2) and Lead (Linac 3) (not marked) Proton Synchrotron Booster PS Proton Synchrotron SPS Super Proton Synchrotron ATLAS (A Toroidal LHC Apparatus) is one of the seven particle detector experiments (ALICE, ATLAS, CMS, TOTEM, LHCb, LHCf and MoEDAL) constructed at the Large Hadron Collider (LHC), a new particle accelerator at the European Organization for Nuclear Research (CERN) in Switzerland. ATLAS is 44 metres long and 25 metres in diameter, weighing about 7,000 tonnes. The project is led by Fabiola Gianotti and involves roughly 2,000 scientists and engineers at 165 institutions in 35 countries.[1][2] The construction was originally scheduled to be completed in June 2007, but was ready and detected its first beam events on 10 September 2008.[3] The experiment is designed to observe phenomena that involve highly massive particles which were not observable using earlier lower-energy accelerators and might shed light on new theories of particle physics beyond the Standard Model. The ATLAS collaboration, the group of physicists building the detector, was formed in 1992 when the proposed EAGLE (Experiment for Accurate Gamma, Lepton and Energy Measurements) and ASCOT (Apparatus with Super Conducting Toroids) collaborations merged their efforts into building a single, general-purpose particle detector for the Large Hadron Collider.[4] The design was a combination of those two previous designs, as well as the detector research and development that had been done for the Superconducting Supercollider.
    [Show full text]
  • Fifty Years of the CERN Proton Synchrotron: Volume 2
    CERN–2013–005 12 August 2013 ORGANISATION EUROPÉENNE POUR LA RECHERCHE NUCLÉAIRE CERN EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH Fifty years of the CERN Proton Synchrotron Volume II Editors: S. Gilardoni D. Manglunki arXiv:1309.6923v1 [physics.acc-ph] 26 Sep 2013 GENEVA 2013 ISBN 978–92–9083–391–8 ISSN 0007–8328 DOI 10.5170/CERN–2013–005 Copyright c CERN, 2013 Creative Commons Attribution 3.0 Knowledge transfer is an integral part of CERN’s mission. CERN publishes this report Open Access under the Creative Commons Attribution 3.0 license (http://creativecommons.org/licenses/by/3.0/) in order to permit its wide dissemination and use. This monograph should be cited as: Fifty years of the CERN Proton Synchrotron, volume II edited by S. Gilardoni and D. Manglunki, CERN-2013-005 (CERN, Geneva, 2013), DOI: 10.5170/CERN–2013–005 Dedication The editors would like to express their gratitude to Dieter Möhl, who passed away during the preparatory phase of this volume. This report is dedicated to him and to all the colleagues who, like him, contributed in the past with their cleverness, ingenuity, dedication and passion to the design and development of the CERN accelerators. iii Abstract This report sums up in two volumes the first 50 years of operation of the CERN Proton Synchrotron. After an introduction on the genesis of the machine, and a description of its magnet and powering systems, the first volume focuses on some of the many innovations in accelerator physics and instrumentation that it has pioneered, such as transition crossing, RF gymnastics, extractions, phase space tomography, or transverse emittance measurement by wire scanners.
    [Show full text]