Super Proton Synchrotron

Total Page:16

File Type:pdf, Size:1020Kb

Super Proton Synchrotron Status of the LHC Injectors Upgrade (LIU) project in 4th ICFA Mini-Workshop on Space Charge 2019, 4-6 November, CERN, Geneva Hannes Bartosik, Malika Meddahi, Giovanni Rumolo R. Alemany, G. Bellodi, J. Coupard, H. Damerau, G.P. Di Giovanni, A. Funken, B. Goddard, K. Hanke, A. Huschauer, V. Kain, A. Lombardi, B. Mikulec, F. Pedrosa, S. Prodon, R. Scrivens, E. Shaposhnikova https://indico.cern.ch/event/828559/ 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 2 Outline • LHC beam performance of the injectors complex and upgrade • LIU project timelines • Relevance of space charge within LIU • Conclusions 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 3 Outline • LHC beam performance of the injectors complex and upgrade • Pre-LIU performance • Definition of the LIU goals and baseline upgrades • LIU project timelines • Relevance of space charge within LIU • Conclusions 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 4 The CERN injector complex: protons Super Proton Synchrotron (SPS) C = 6.9 km 퐸표푢푡 = 450 GeV 푘푖푛 The CERN injector complex is used to feed LHC as well as to serve a number of fixed target PS-Booster (PSB) 4 rings of C =157 m Proton Synchrotron (PS) experiments 표푢푡 C = 628 m 퐸푘푖푛 = 1.4 GeV 표푢푡 퐸푘푖푛 = 25 GeV Linac 2 표푢푡 퐸푘푖푛 = 50 MeV 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 5 Production scheme of LHC beams Number of Bunch Beam transfer bunches spacing (ns) Linac2 PSB Multi-turn 표푢푡 injection of – 퐸푘푖푛 = 50 MeV coasting beam Super Proton Synchrotron PSB PS (SPS) 4 272 퐸표푢푡 = 1.4 GeV C = 6.9 km 푘푖푛 표푢푡 퐸푘푖푛 = 450 GeV PS-Booster (PSB) 4 rings of C =157 m Proton Synchrotron (PS) 표푢푡 C = 628 m 퐸푘푖푛 = 1.4 GeV 표푢푡 퐸푘푖푛 = 25 GeV Linac 2 표푢푡 퐸푘푖푛 = 50 MeV 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 6 Production scheme of LHC beams Number of Bunch Beam transfer bunches spacing (ns) Linac2 PSB Multi-turn 표푢푡 injection of – 퐸푘푖푛 = 50 MeV coasting beam Super Proton Synchrotron PSB PS (SPS) 4 272 퐸표푢푡 = 1.4 GeV C = 6.9 km 푘푖푛 표푢푡 퐸푘푖푛 = 450 GeV PS-Booster (PSB) 4 rings of C =157 m Proton Synchrotron (PS) 표푢푡 C = 628 m 퐸푘푖푛 = 1.4 GeV 표푢푡 퐸푘푖푛 = 25 GeV Linac 2 표푢푡 퐸푘푖푛 = 50 MeV 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 7 Production scheme of LHC beams Number of Bunch Beam transfer bunches spacing (ns) Linac2 PSB Multi-turn 표푢푡 injection of – 퐸푘푖푛 = 50 MeV coasting beam Super Proton Synchrotron PSB PS (SPS) 4 + 2 272 퐸표푢푡 = 1.4 GeV C = 6.9 km 푘푖푛 표푢푡 퐸푘푖푛 = 450 GeV PSOne SPStriple bunch splitting and two 표푢푡 72 25 퐸푘푖푛double= 25 GeV bunch splittings in the PS PS-Booster (PSB) 4 rings of C =157 m Proton Synchrotron (PS) 표푢푡 C = 628 m 퐸푘푖푛 = 1.4 GeV 표푢푡 퐸푘푖푛 = 25 GeV Linac 2 표푢푡 퐸푘푖푛 = 50 MeV 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 8 Production scheme of LHC beams Number of Bunch Beam transfer bunches spacing (ns) Linac2 PSB Multi-turn 표푢푡 injection of – 퐸푘푖푛 = 50 MeV coasting beam Super Proton Synchrotron PSB PS (SPS) 4 + 2 272 퐸표푢푡 = 1.4 GeV C = 6.9 km 푘푖푛 표푢푡 퐸푘푖푛 = 450 GeV PS SPS 표푢푡 72 25 퐸푘푖푛 = 25 GeV PS-Booster (PSB) SPS LHC Proton Synchrotron (PS) 표푢푡 Four injections4 x 72 into the SPS25 / 200 4 rings of C =157 m 퐸푘푖푛 = 450 GeV 표푢푡 C = 628 m 퐸푘푖푛 = 1.4 GeV 표푢푡 퐸푘푖푛 = 25 GeV Linac 2 표푢푡 퐸푘푖푛 = 50 MeV 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 9 LHC beam performance before upgrade • LHC beam parameters at the SPS extraction (450 GeV) result from intensity and brightness limitations of all injectors in the chain • Brightness Measured points: • PSB brightness determined by space charge at N = 1.1 – 1.3 x 1011 p/b b injection ex,y = 2.5 – 3.0 mm • Limit for PS space charge at injection DQy < 0.31 • Intensity • SPS is limited by beam loading and longitudinal instabilities on the ramp and flat top • PS is limited by longitudinal coupled bunch instability on the ramp and flat top 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 10 LHC beam performance before upgrade • LHC beam parameters at the SPS extraction (450 GeV) result from intensity and brightness limitations of all injectors in the chain • Brightness • PSB brightness determined by space charge at injection • Limit for PS space charge at injection DQy < 0.31 Space charge in SPS not a limit for LHC beams • Intensity • SPS is limited by beam loading and longitudinal instabilities on the ramp and flat top • PS is limited by longitudinal coupled bunch instability on the ramp and flat top PSB intensity limit well above displayed range 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 11 The LHC Injectors Upgrade (LIU) project • Performance goal Match the beam parameters at SPS extraction to the High Luminosity LHC (HL-LHC) target 11 Nb (x 10 p/b) ex,y, (mm) HL-LHC target 2.3 2.1 Before upgrades 1.3 2.7 • LIU strategy →Identify the sources of the performance limitations in each of the injectors impeding the achievement of the HL-LHC target parameters →Define and deploy the necessary upgrade items to overcome these limitations 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 12 The LHC Injectors Upgrade (LIU) project • Effect on beam parameter reach at SPS extraction of the upgrade items in the LIU project baseline 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 13 The LHC Injectors Upgrade (LIU) project • Effect on beam parameter reach at SPS extraction of the upgrade items in the LIU project baseline • Connection of PSB to Linac4 o Charge exchange H- injection at 160 MeV into PSB Linac4 25 mA, 0.4 um 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 14 The LHC Injectors Upgrade (LIU) project • Effect on beam parameter reach at SPS extraction of the upgrade items in the LIU project baseline Connection of PSB to Linac4 • PSB acceleration to 2 GeV o Reduced bg2 at PS injection by 40% o Updated longitudinal parameters at PSB-PS transfer to further reduce PS space charge tune spread 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 15 The LHC Injectors Upgrade (LIU) project • Effect on beam parameter reach at SPS extraction of the upgrade items in the LIU project baseline Connection of PSB to Linac4 PSB acceleration to 2 GeV • PS RF upgrades, e.g. o New Finemet cavity for longitudinal feedback system o Impedance reduction of RF systems 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 16 The LHC Injectors Upgrade (LIU) project • Effect on beam parameter reach at SPS extraction of the upgrade items in the LIU project baseline Connection of PSB to Linac4 PSB acceleration to 2 GeV PS RF upgrades • SPS upgrade o Power and LLRF upgrade of 200 MHz RF system o Longitudinal impedance reduction o a-C coating of focusing quadrupole chambers o Deployment of low gt optics o Upgrade of beam dump and protection devices 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 17 The LHC Injectors Upgrade (LIU) project • Effect on beam parameter reach at SPS extraction of the upgrade items in the LIU project baseline Connection of PSB to Linac4 PSB acceleration to 2 GeV PS RF upgrades • SPS upgrade o Power and LLRF upgrade of 200 MHz RF system o Longitudinal impedance reduction o a-C coating of focusing quadrupole chambers o Deployment of low gt optics o Upgrade of beam dump and protection devices 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 18 The LHC Injectors Upgrade (LIU) project • Effect on beam parameter reach at SPS extraction of the upgrade items in the LIU project baseline Connection of PSB to Linac4 PSB acceleration to 2 GeV PS RF upgrades SPS upgrade ⇒LIU parameter reach for proton beams matches the HL-LHC target within baseline 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 19 Not only protons … • CERN injector complex also accelerates heavy ions (Pb) N e # of (x 108 ions/b) (mm) bunches Super Proton Synchrotron HL-LHC target 1.9 1.5 1248 (SPS) (7x 8 bunches, 50 ns) C = 6.9 km Achieved 2018 표푢푡 2.0 1.5 648 퐸푘푖푛 = 176.4 GeV/u (9x 4 bunches, 100 ns) Proton Synchrotron (PS) Relies on SPS C = 628 m 표푢푡 Single bunch parameters slip stacking 퐸푘푖푛 = 5.9 GeV/u already achieved Linac 3 Low Energy Ion Ring (LEIR) 표푢푡 퐸푘푖푛 = 4.2 MeV/u C = 78 m 표푢푡 퐸푘푖푛 = 72.2 MeV/u 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 20 Outline • LHC beam performance of the injectors complex • LIU project timelines • Project evolution • Current status and future steps • Relevance of space charge within LIU • Conclusions 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 21 2010 Run 1 + LS1 + Run 2 (2010 – 2018) Preparing, defining, testing, executing • Start of LIU project • Studies, advanced installation and testing, new buildings • Linac4 commissioning and quality/reliability runs Long Shutdown 2 (2018 – 2020) 2018 Peak of LIU execution phase 2020 • End of LIU equipment production • LIU equipment installation across all injectors 2024 Run 3 (2020 – 2024) • Recommissioning of upgraded injectors • End of LIU project in 2021! → Beam commissioning to LIU specifications throughout Run 3 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 22 2010 Run 1 + LS1 + Run 2 (2010 – 2018) Preparing, defining, testing, executing • Start of LIU project • Studies, advanced installation and testing, new buildings • Linac4 commissioning and quality/reliability runs Long Shutdown 2 (2018 – 2020) 2018 Peak of LIU execution phase 2020 • End of LIU equipment production • LIU equipment installation across all injectors 2024 Run 3 (2020 – 2024) • Recommissioning of upgraded injectors • End of LIU project in 2021! → Beam commissioning to LIU specifications throughout Run 3 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 23 Time lapse Emptying part of PSB injection area, before installing the new H- charge exchange injection system 4/11/2019 Space Charge 2019, CERN, 4-6 November 2019 Giovanni Rumolo 24 Hardware and beam commissioning in 2020 J.
Recommended publications
  • Il Nostro Mondo
    IL NOSTRO MONDO THE DESIGN, CONSTRUCTION AND PERFORMANCE OF THE CERN INTERSECTING STORAGE RINGS (ISR) A RECOLLECTION OF WORLD’S FIRST PROTON-PROTON COLLIDER KURT HÜBNER CERN, Geneva, Switzerland 1 Design which had a beam energy of 160 MeV. The interaction points to increase the collision rate The concept of colliding beams appeared design of these colliders started in 1957. but without special lattice insertions as one first in a German patent by Rolf Widerøe In 1961, the Accelerator Research Group would use these days. registered in 1943 and published in 1952. Division was expanded into the Accelerator Combined-function magnets were chosen However, at that time the intensity of beams Division as experienced manpower had as in the PS, i.e. the main magnets had a was too low for an exploitable collision rate as become available after the running-in of the magnetic dipole field to bend the beam and a beam accumulation had not yet been invented. PS in 1960. At the same time it was decided quadrupole field to focus the beam. This type The first ideas of a realistic design were to construct a small accelerator to test rf of magnet provided space for the elaborate published in 1956 by Gerard O’Neill and by the stacking, a technique to be experimentally pole-face windings foreseen to control the MURA Group lead by Donald Kerst in the USA. proven, as it was essential for the performance magnetic field to a very high precision. It also MURA had come up with beam accumulation and success of the ISR.
    [Show full text]
  • Pos(ICRC2019)446
    New Results from the Cosmic-Ray Program of the NA61/SHINE facility at the CERN SPS PoS(ICRC2019)446 Michael Unger∗ for the NA61/SHINE Collaborationy Karlsruhe Institute of Technology (KIT), Postfach 3640, D-76021 Karlsruhe, Germany E-mail: [email protected] The NA61/SHINE experiment at the SPS accelerator at CERN is a unique facility for the study of hadronic interactions at fixed target energies. The data collected with NA61/SHINE is relevant for a broad range of topics in cosmic-ray physics including ultrahigh-energy air showers and the production of secondary nuclei and anti-particles in the Galaxy. Here we present an update of the measurement of the momentum spectra of anti-protons produced in p−+C interactions at 158 and 350 GeV=c and discuss their relevance for the understanding of muons in air showers initiated by ultrahigh-energy cosmic rays. Furthermore, we report the first results from a three-day pilot run aimed at investigating the ca- pability of our experiment to measure nuclear fragmentation cross sections for the understanding of the propagation of cosmic rays in the Galaxy. We present a preliminary measurement of the production cross section of Boron in C+p interactions at 13.5 AGeV=c and discuss prospects for future data taking to provide the comprehensive and accurate reaction database of nuclear frag- mentation needed in the era of high-precision measurements of Galactic cosmic rays. 36th International Cosmic Ray Conference -ICRC2019- July 24th - August 1st, 2019 Madison, WI, U.S.A. ∗Speaker. yhttp://shine.web.cern.ch/content/author-list c Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 International License (CC BY-NC-ND 4.0).
    [Show full text]
  • NA61/SHINE Facility at the CERN SPS: Beams and Detector System
    Preprint typeset in JINST style - HYPER VERSION NA61/SHINE facility at the CERN SPS: beams and detector system N. Abgrall11, O. Andreeva16, A. Aduszkiewicz23, Y. Ali6, T. Anticic26, N. Antoniou1, B. Baatar7, F. Bay27, A. Blondel11, J. Blumer13, M. Bogomilov19, M. Bogusz24, A. Bravar11, J. Brzychczyk6, S. A. Bunyatov7, P. Christakoglou1, T. Czopowicz24, N. Davis1, S. Debieux11, H. Dembinski13, F. Diakonos1, S. Di Luise27, W. Dominik23, T. Drozhzhova20 J. Dumarchez18, K. Dynowski24, R. Engel13, I. Efthymiopoulos10, A. Ereditato4, A. Fabich10, G. A. Feofilov20, Z. Fodor5, A. Fulop5, M. Ga´zdzicki9;15, M. Golubeva16, K. Grebieszkow24, A. Grzeszczuk14, F. Guber16, A. Haesler11, T. Hasegawa21, M. Hierholzer4, R. Idczak25, S. Igolkin20, A. Ivashkin16, D. Jokovic2, K. Kadija26, A. Kapoyannis1, E. Kaptur14, D. Kielczewska23, M. Kirejczyk23, J. Kisiel14, T. Kiss5, S. Kleinfelder12, T. Kobayashi21, V. I. Kolesnikov7, D. Kolev19, V. P. Kondratiev20, A. Korzenev11, P. Koversarski25, S. Kowalski14, A. Krasnoperov7, A. Kurepin16, D. Larsen6, A. Laszlo5, V. V. Lyubushkin7, M. Mackowiak-Pawłowska´ 9, Z. Majka6, B. Maksiak24, A. I. Malakhov7, D. Maletic2, D. Manglunki10, D. Manic2, A. Marchionni27, A. Marcinek6, V. Marin16, K. Marton5, H.-J.Mathes13, T. Matulewicz23, V. Matveev7;16, G. L. Melkumov7, M. Messina4, St. Mrówczynski´ 15, S. Murphy11, T. Nakadaira21, M. Nirkko4, K. Nishikawa21, T. Palczewski22, G. Palla5, A. D. Panagiotou1, T. Paul17, W. Peryt24;∗, O. Petukhov16 C.Pistillo4 R. Płaneta6, J. Pluta24, B. A. Popov7;18, M. Posiadala23, S. Puławski14, J. Puzovic2, W. Rauch8, M. Ravonel11, A. Redij4, R. Renfordt9, E. Richter-Wa¸s6, A. Robert18, D. Röhrich3, E. Rondio22, B. Rossi4, M. Roth13, A. Rubbia27, A. Rustamov9, M.
    [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]
  • Particle Physics Lecture 4: the Large Hadron Collider and Other Accelerators November 13Th 2009
    Subatomic Physics: Particle Physics Lecture 4: The Large Hadron Collider and other accelerators November 13th 2009 • Previous colliders • Accelerating techniques: linacs, cyclotrons and synchrotrons • Synchrotron Radiation • The LHC • LHC energy and luminosity 1 Particle Acceleration Long-lived charged particles can be accelerated to high momenta using electromagnetic fields. • e+, e!, p, p!, µ±(?) and Au, Pb & Cu nuclei have been accelerated so far... Why accelerate particles? • High beam energies ⇒ high ECM ⇒ more energy to create new particles • Higher energies probe shorter physics at shorter distances λ c 197 MeV fm • De-Broglie wavelength: = 2π pc ≈ p [MeV/c] • e.g. 20 GeV/c probes a distance of 0.01 fm. An accelerator complex uses a variety of particle acceleration techniques to reach the final energy. 2 A brief history of colliders • Colliders have driven particle physics forward over the last 40 years. • This required synergy of - hadron - hadron colliders - lepton - hadron colliders & - lepton - lepton colliders • Experiments at colliders discovered W- boson, Z-boson, gluon, tau-lepton, charm, bottom and top-quarks. • Colliders provided full verification of the Standard Model. DESY Fermilab CERN SLAC BNL KEK 3 SppS̅ at CERNNo b&el HERAPrize for atPhy sDESYics 1984 SppS:̅ Proton anti-Proton collider at CERN. • Given to Carlo Rubbia and Simon van der Meer • Ran from 1981 to 1984. Nobel Prize for Physics 1984 • Centre of Mass energy: 400 GeV • “For their decisive • 6.9 km in circumference contributions to large • Two experiments:
    [Show full text]
  • The Search for Charged Massive Supersymmetric Particles at the LHC
    The Search for Charged Massive Supersymmetric Particles at the LHC Aleksey Pavlov A Senior Project Presented to Cal Poly June 5, 2012 This material is based upon work supported by The National Science Foundation under grant number 0969966. 1 Contents 1 Abstract 3 2 Introduction 3 3 Supersymmetry: An Extension of the Standard Model 5 4 CHAMPs 8 5 The LHC 9 6 The ALICE Detector 12 7 Analysis 14 8 Results 17 2 1 Abstract Charged Massive Particles (CHAMPs) are predicted in the Supersymmetry (SUSY) extension of the Standard Model though they have never been ob- served. We look for CHAMPs in the ALICE Detector at the Large Hadron Collider at CERN. While the main purpose of ALICE is to study Quark- Gluon Plasma, we take advantage of the tracking and time of flight capabil- ities of several sub-detectors in ALICE to look for signs of CHAMPs. These elusive particles are characterized by their slow velocity, high transverse mo- mentum and therefore heavy mass. Our research found a small handful of candidates among a large sample size but more work is required to confirm their identity and exclude the possibility that they have been misidentified. 2 Introduction The Standard Model of Particle Physics (SM) is the modern theory describ- ing how fundamental particles interact and behave. It was developed in the second half of the 20th Century after physicist Sheldon Glashow found a way to combine, or unify, the electromagnetic and electroweak forces [7]. In 1973 Glashow's electroweak theory was experimentally confirmed at CERN, the European Organization for Nuclear Research in Geneva, Switzerland, when nuetral currents through the weak nuclear force were measured.
    [Show full text]
  • THE PROTON-ANTIPROTON COLLIDER Lecture Delivered at CERN on 25 November 1987 Lyndon Evans
    CERN 88-01 11 March 1988 ORGANISATION EUROPÉENNE POUR LA RECHERCHE NUCLÉAIRE CERN EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH CERN ACCELERATOR SCHOOL Third John Adams Memorial Lecture THE PROTON-ANTIPROTON COLLIDER Lecture delivered at CERN on 25 November 1987 Lyndon Evans GENEVA 1988 ABSTRACT The subject of this lecture is the CERN Proton-Antiproton (pp) Collider, in which John Adams was intimately involved at the design, development, and construction stages. Its history is traced from the original proposal in 1966, to the first pp collisions in the Super Proton Synchrotron (SPS) in 1981, and to the present time with drastically improved performance. This project led to the discovery of the intermediate vector boson in 1983 and produced one of the most exciting and productive physics periods in CERN's history. RN —Service d'Information Scientifique-RD/757-3000-Mars 1988 iii CONTENTS Page 1. INTRODUCTION 1 2. BEAM COOLING l 3. HISTORICAL DEVELOPMENT OF THE pp COLLIDER CONCEPT 2 4. THE SPS AS A COLLIDER 4 4.1 Operation 4 4.2 Performance 5 5. IMPACT OF EARLIER CERN DEVELOPMENTS 5 6. PROPHETS OF DOOM 7 7. IMPACT ON THE WORLD SCENE 9 8. CONCLUDING REMARKS: THE FUTURE OF THE pp COLLIDER 9 REFERENCES 10 Plates 11 v 1. INTRODUCTION The subject of this lecture is the CERN Proton-Antiproton (pp) Collider and let me say straightaway that some of you might find that this talk is rather polarized towards the Super Proton Synchrotron (SPS). In fact, the pp project was a CERN-wide collaboration 'par excellence'. However, in addition to John Adams' close involvement with the SPS there is a natural tendency for me to remain within my own domain of competence.
    [Show full text]
  • Discovery Machines
    DISCOVERY MACHINES 2019 was noteworthy for being the start of Long Shutdown 2 (LS2) of the CERN accelerator complex. Across all the machines, teams began the tasks of maintaining or renovating numerous items of equipment or replacing them with new, innovative systems. These major upgrades are being carried out in preparation for the third run of the LHC and for the High-Luminosity LHC (HL-LHC). What’s more, they will benefit the users of all the accelerators as many aspects of the work are being carried out as part of the LHC Injectors Upgrade (LIU) project. ISOLDE The front-ends for the LINEAR ACCELERATOR 4 (LINAC4) isotope separator targets have been built, tested Linac4 is now connected to the LHC and partially installed. accelerator chain. A nominal beam The new Offline2 test of 160 MeV reached the Linac4 beam facility, equipped with dump in October. a laser ion source, was (CERN-PHOTO-201704-093-27) commissioned. (CERN-PHOTO-201911-394-28) PS BOOSTER (PSB) Seventy of the 215 metres of the PSB’s beam lines have been removed to allow the installation of new equipment. More than 60 magnets have been renovated or replaced in the accelerator. A new RF acceleration system has been installed. After LS2, the energy of the PS Booster will increase from 1.4 to 2 GeV. (CERN-PHOTO-201906-149-11) 22 | CERN SUPER PROTON SYNCHROTRON (SPS) LARGE HADRON COLLIDER (LHC) A new RF acceleration system is under The electrical insulation of the diodes has construction. The SPS beam dump is being been completed on 94% of the accelerator’s replaced.
    [Show full text]
  • Charged Pion Spectra in Proton–Carbon Interactions at 31 Gev/C
    XIII International Workshop on Neutrino Factories, Super beams and Beta beams (NUFACT11) IOP Publishing Journal of Physics: Conference Series 408 (2013) 012048 doi:10.1088/1742-6596/408/1/012048 Charged pion spectra in proton–carbon interactions at 31 GeV/c Magdalena Zofia Posiada la on behalf of the NA61/SHINE Collaboration Faculty of Physics, University of Warsaw, Ho˙za69, 00-681 Warsaw, Poland E-mail: [email protected] Abstract. The NA61/SHINE experiment at CERN SPS measured charged pion spectra in p+C interactions at 31 GeV/c. These measurements are necessary to improve predictions of the neutrino flux for the T2K long baseline neutrino oscillation experiment in Japan. Presented analysis was based on the data collected during the first NA61/SHINE run in 2007 with an isotropic graphite target with a thickness of 4% of nuclear interaction length. Three different methods which were used in order to obtain π+ and π− spectra are introduced. Differential cross sections for negatively and positively charged pions are presented as a function of laboratory momentum in ten intervals of the laboratory polar angle up to 420 mrad. 1. Introduction The NA61/SHINE (SHINE = SPS Heavy Ion and Neutrino Experiment) is a large acceptance hadron spectrometer located in the North Area H2 beam line of the European Centre for Nuclear Research (CERN) in Geneva. The experiment uses beams from the Super Proton Synchrotron (SPS). The NA61/SHINE experiment combines a rich physics program in three different fields: auxiliary measurements for neutrino experiments, cosmic-ray simulations, and the behavior of strongly interacting matter at high density (see: [1, 2, 3] for details).
    [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]
  • Discovery Machines
    DISCOVERY MACHINES CERN operates a unique complex of eight accelerators and one decelerator. The accelerators speed particles up to almost the speed of light before colliding them with each other or launching them at targets. Detectors record what happens during these collisions, and all the data collected is stored and analysed using a worldwide computing grid. Hundreds of physicists, engineers and technicians contribute to the operation and maintenance of these sophisticated machines. The LHC performed remarkably in 2016, delivering far more collisions than expected. (CERN-GE-1101021-08) 20 | CERN 2011: 6 fb-1 2012: 23 fb-1 2015: 4 fb-1 2016: 40 fb-1 7 and 8 TeV runs 13 TeV runs LHC operators at the controls in July 2016. Above, the amount of data delivered by the LHC to the ATLAS (CERN-PHOTO-201607-171-3) and CMS experiments over the course of its proton runs. These quantities are expressed in terms of integrated luminosity, which refers to the number of potential collisions during a given period. LARGE HADRON COLLIDER IN FULL SWING 2016 was an exceptional year for the Large Hadron Collider magnet, which injects the particle bunches into the machine, (LHC). In its second year of running at a collision energy of limited the number of particles per bunch. 13 teraelectronvolts (TeV), the accelerator’s performance exceeded expectations. In spite of these interruptions, the performance of the machines was excellent. Numerous adjustments had been The LHC produced more than 6.5 million billion collisions made to all systems over the previous two years to improve during the proton run from April to the end of October, their availability.
    [Show full text]
  • Partially Strip Ions Tests and Plans for the Large Hadron Collider (LHC)
    Super Proton Synchrotron (SPS) Partially Strip Ions tests and plans for the Large Hadron Collider (LHC) R. Alemany Fernandez on behalf of W. Krasny, N. Biancacci, S. Hirlaender, K. Kornelis, T. Bohl, S. Cettour, V. Kain, H. Bartosik, M. Lamont, F. Zimmermann, B. Goddard, SPS Operations team and the Gamma Factory enthusiasts. Topics: 1. Just in case: why do we do this? 2. The CERN Ion Injector Complex & the LHC 3. Life time studies with partially strip ions: Xe39+ 4. Plans for 2018: Pb80+ & Pb81+ 5. Conclusions Photon beams workshop, Padova, 27-28 November 2017 Why do we do this? Goal: achieve comparable fluxes of gamma rays, of up to ~ 400 MeV, as those in the keV domain of X-ray sources Photons Photons per pulse brillance Peak Peak Energy (eV) Are thre “alternative solutions to traditional sources” to increase the photon energy and intensity? 1. Explore the EXISTING world unique opportunities offered by the CERN accelerator complex and scientific infrastructure Partially strip ion Resonant cross section = 5.9e-16 cm2 ~ 9 orders of magnitude bigger cross-section than Compton process E.g. (maximal energy): LHC, Pb80+ = 2887 n=12 laser =104.4 nm (max) = 396 MeV Intensity increase match target size and laser wave length 1.Let’s explore the CERN accelerator facilities 2.Let’s try to inject partially strip ions in this facility LHC 27 km SPS 7 km 24 January 2017 JUAS 2017 10 ION accelerator complex SPS LHC PS LEIR SOURCE+LINAC3 Pb Ion source Small sliver of solid isotopically pure 208Pb is placed in a ceramic crucible that sits in an "oven" The metal is heated to around 800°C and ionized to become plasma.
    [Show full text]