Moving Physics 'Forward' at the LHC

Total Page:16

File Type:pdf, Size:1020Kb

Moving Physics 'Forward' at the LHC TOTEM moving physics ‘forward’ at the LHC When protons meet head on at the LHC, the collisions provide a micro-laboratory to investigate many phenomena, including the protons themselves. This is the physics that the TOTEM (TOTal cross section, Elastic scattering and di!raction dissocia- tion Measurement at the LHC) experiment is especially designed to explore. By making precise measurements on particles that emerge from collisions very close to the direction of the LHC beams — the ‘forward’ direction — TOTEM probes physics that is not easily accessible by other LHC experiments. The initial protons can simply change direction without losing energy, in ‘elastic’ collisions, or they can generate new particles, in ‘inelastic’ collisions. Among a range of studies, TOTEM is mea- suring the total probability, or ‘cross-section’, for proton–proton interactions — in a sense, the overall size that a proton presents as a ‘target’. The experiment is also investigating scattering phenomena analogous to the di!raction of light. TOTEM has detectors on both sides of the interaction region at Point 5, where the CMS experiment is located. In each direction, there are two ‘telescopes’ to track charged particles and two sets of ‘Roman pots’ — movable devices that come particularly close to the beam — containing detectors to track elastically- scattered protons. www.cern.ch Approval as 5thPrototype LHC experiment RomanGEM potchambers testsRoman assembled pots installed forRoman 1st time inpots LHC equipped tunnel at with 220 siliconm detectorsFirst collisionsFirst detected results published on total Installation andInstallation commissioning of silicon of detectors T2 at 220 m Track multiplicities elastic cross-section published 2004 2005 2006 2007 2008 2009 2009 2010 2011 2012 Roman pots Particle telescopes Roman pots are devices named after their shape Two T1 telescopes are located starting from and their original use by physicists from Rome in Edgeless silicon 10.5 m from the interaction point inside the the 1970s at CERN’s "rst proton–proton collider, TOTEM’s silicon detectors are ‘edgeless’ in that endcaps of the CMS magnet. Each is made up the Intersecting Storage Rings. TOTEM has they have an insensitive region close to the of "ve detection planes, based on gas-"lled Roman pot stations at distances of 147-149 m beam of only a few hundredths of a millimetre. cathode-strip chambers. and 215-220 m on either side of the interaction Every detector is divided into 512 strips to Two T2 telescopes are installed external to CMS point. All of the stations have two units, each determine the location of scattered particles at a distance starting from 13.4 m. Each has a consisting of two pots that move vertically and with high precision. cylindrical structure, divided into 10 detection one that moves horizontally. Each pot contains planes that consist of pairs of semi-circular GEM 10 silicon detectors. chambers arranged back-to-back. TOTEM in numbers Little gems Some 100 people from 15 institutes in 7 countries The GEM (gas electron multiplier) chambers use work on the TOTEM experiment. technology invented at CERN, which combines excellent spatial resolution with a high rate- capability and good radiation resistance. CERN CH-1211 Geneva 23 Communication Group, September 2012 CERN-Brochure-2012-004-Eng Photos: CERN Photo Service totem-experiment.web.cern.ch.
Recommended publications
  • Diffraction at Hera, the Tevatron and the Lhc∗
    Vol. 37 (2006) ACTA PHYSICA POLONICA B No 12 DIFFRACTION AT HERA, THE TEVATRON AND THE LHC∗ C. Royon DAPNIA/Service de Physique des Particules, CEA/Saclay 91191 Gif-sur-Yvette Cedex, France (Received October 18, 2006) In these lectures, we present and discus the most recent results on inclusive diffraction from the HERA and Tevatron colliders and give the prospects for the future at the LHC. Of special interest is the exclusive production of Higgs boson and heavy objects (W , top, stop pairs) which will require a better understanding of diffractive events and the link between ep and hadronic colliders, as well as precise measurements and analyses of inclusive diffraction at the LHC in particular to constrain further the gluon density in the pomeron. PACS numbers: 12.38.–t, 13.60.–r, 13.85.–t In these lectures, we describe the most recent results on inclusive diff- raction at HERA, as well as diffractive results from the Tevatron. We finish the lecture by discussing the prospects of diffractive physics at the LHC. 1. Experimental definition of diffraction In this section, we discuss the different experimental ways to define diff- raction. As an example, we describe the methods used by the H1 and ZEUS experiments at HERA, DESY, Hamburg in Germany. 1.1. The rapidity gap method HERA is a collider where electrons of 27.6 GeV collide with protons of 920 GeV. A typical event as shown in the upper plot of Fig. 1 is ep ! eX where electron and jets are produced in the final state. We notice that the ∗ Presented at the XLVI Cracow School of Theoretical Physics, Zakopane, Poland May 27–June 5, 2006.
    [Show full text]
  • A Very Forward Hadron Spectrometer for the LHC and Cosmic Ray Physics
    A Very Forward Hadron Spectrometer for the LHC and Cosmic Ray Physics Michael Albrow∗y Fermi National Accelerator Laboratory, Batavia, IL 60510, USA. ORCID 0000-0001-7329-4925 E-mail: [email protected] Charged hadron production in hadron-hadron collisions with longitudinal momentum fraction p Feynman-x, xF , between 0.1 and 0.9 has not been measured above s = 63 GeV at the CERN Intersecting Storage Rings. I discuss a way to measure this at the Large Hadron Collider at p s = 13 TeV, which is 40,000 times higher in equivalent fixed target energy, and important for understanding cosmic ray showers. arXiv:1811.02047v1 [physics.ins-det] 5 Nov 2018 2nd World Summit: Exploring the Dark Side of the Universe 25-29 June, 2018 University of Antilles, Pointe-Ã˘a-Pitre, Guadeloupe, France ∗Speaker. yScientist emeritus 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). https://pos.sissa.it/ Very Forward Hadron Spectrometer Michael Albrow Figure 1: The flux of cosmic rays multiplied by E2:5, showing the “knee" and the “ankle" vs. primary energy E. All this data is based on measuring showers in the atmosphere. The maximum energy of the CERN ISR and LHC are indicated. 1. Introduction When the first hadron collider, the CERN Intersecting Storage Rings, ISR, came into operation in 1971 it was known that most produced particles in inelastic collisions have small transverse q 2 2 momenta, pT = px + py less than about 1 GeV/c.
    [Show full text]
  • Future Physics Program with Tagged Forward Protons at RHIC
    Future Physics Program with Tagged Forward Protons at RHIC J.H. Lee For STAR Collaboration BNL April 29, DIS09, Madrid 1 Relativistic Heavy Ion Collider (RHIC): THE QCD Factory QCD is the theory of strong interaction: “Theoretical evidences” vs. current and future Experimental QCD measurements at RHIC z Confinement/ phase of QCD - QGP Further investigationateRHIC z Distribution of spin in the nucleon - Spin sum rule z Parton splitting limit - Saturated gluon state (Color Glass Condensate…) z Gluonic degree of freedom in Hadrons – exotica (glueballs…) z Nature of diffractive processes – structure of Pomeron, Odderon… April 29 DIS09 J.H. Lee 2 near Future Program with tagged forward protons at RHIC studying: Elastic scattering for understanding structure of Pomeron and Odderon Central production for searching for glueballs in Double Pomeron Exchange (DPE) processes April 29 DIS09 J.H. Lee 3 Summary of the Existing Elastic Data (unpolarized) 50 500 RHIC Highest energy so far: pp: 62 GeV (ISR) pp: 1.8 Tev (Tevatron) RHIC energy range: 50 GeV ≤√s ≤ 500 GeV Elastic measurements: Details on the nature of elastic scattering at the energy are NOT well understood in the energy range: Unique measurements in wide t- range with polarized beams April 29 DIS09 J.H. Lee 4 Can Odderon be identified at RHIC? Odderon is a counterpart of pomeron (C=1) with C=-1: “RHIC is the machine to find it” (E. Leader, Odderon Workshop (2005)) by measuring Δσpp –Δσpbarp ≠ 0 (~3mb) dσ/dtpp ≠ dσ/dtpbarp Shape of Asymmetries: ANN Centrally produced C=-1 particle hep-ph/0210437 M. Islam et al.
    [Show full text]
  • At the ISR the Luminosity Was Determined with an Accuracy of 1% [41]. This Was Helped by the Fact That the ISR Operated With
    112 C. Fabjan & K. Hübner Fig. 4.11. Concept of the Van der Meer scan to determine the beam profile. At the ISR the luminosity was determined with an accuracy of 1% [41]. This was helped by the fact that the ISR operated with continuous beams (not bunched), allowing absolute beam current measurements, and beam cross sections that were large enough for length scales to be calibrated precisely by mechanical means (using scrapers). For the Tevatron, which could not use the VdM method, the luminosity uncertainty was typically 15–20%. The LHC renewed with the ISR tradition of VdM scans for determining luminosity [42] and optimizing the collisions [43]. After three years of operation, systematic uncertainties down to 1.5% have been achieved [42]. An automatic online procedure has also been developed for making VdM scans and directly sharing the results with the experiments [44]. The procedure includes a detailed analysis of beam dynamics uncertainties in VdM scans and has been adopted at both RHIC and the LHC. Automatic mini-VdM scans are now standard procedure in LHC operation and are used to optimize collisions for every physics run. 4.7 Roman Pots: Physics Next to the Accelerator Beam Technology Meets Research Downloaded from www.worldscientific.com Giorgio Matthiae The “Roman pot” technique was invented at the ISR to study particles scattered at by GERMAN ELECTRON SYNCHROTRON @ HAMBURG on 05/10/17. For personal use only. very small angles. These particles travel close to the circulating beams — in fact inside the vacuum chamber. They can only be detected by a special system able to place detectors a few millimetres from the beam.
    [Show full text]
  • Upgrade of the Global Muon Trigger for the Compact Muon Solenoid Experiment at CERN
    DISSERTATION/DOCTORAL THESIS Titel der Dissertation/Title of the Doctoral Thesis “Upgrade of the Global Muon Trigger for the Compact Muon Solenoid experiment at CERN” verfasst von/submitted by Mag. Dinyar Sebastian Rabady angestrebter akademischer Grad/in partial fulfilment of the requirements for the degree of Doktor der Naturwissenschaften (Dr. rer. nat.) CERN-THESIS-2018-033 25/04/2018 Wien, im Jänner 2018/Vienna, in January 2018 Studienkennzahl lt. Studienblatt/ A 796 605 411 degree programme code as it appears on the student record sheet: Studienrichtung lt. Studienblatt/ Physik field of study as it appears onthe student record sheet: Betreut von/Supervisor: Dipl.-Ing. Dr. Claudia-Elisabeth Wulz Hon.-Prof. Dipl.-Phys. Dr. Eberhard Widmann Für meinen Großvater. Abstract The Large Hadron Collider is a large particle accelerator at the CERN research labo- ratory, designed to provide particle physics experiments with collisions at unprece- dented centre-of-mass energies. For its second running period both the number of colliding particles and their collision energy were increased. To cope with these more challenging conditions and maintain the excellent performance seen during the first running period, the Level-1 trigger of the Compact Muon Solenoid experiment — a so- phisticated electronics system designed to filter events in real-time — was upgraded. This upgrade consisted of the complete replacement of the trigger electronics andafull redesign of the system’s architecture. While the calorimeter trigger path now follows a time-multiplexed processing model where the entire trigger data for a collision are received by a single processing board, the muon trigger path was split into regional track finding systems where each newly introduced track finder receives data from all three muon subdetectors for a certain geometric detector slice and reconstructs fully formed muon tracks from this.
    [Show full text]
  • PPS) Past, Present, and Future
    The CMS Precision Proton Spectrometer (PPS) Past, Present, and Future Jonathan Hollar (LIP) LIP Seminar, Jan. 21, 2021 1 PPS: The Precision Proton Spectrometer • A series of very small detectors (few cm2 active area) Roman Pot stations Set of movable detectors to approach the beam. • Located very far from the central CMS detector (~210m)RP for tracking at the stations CERN LHC RP for timing stations RF shield Each unit includes 3 RPs (1 horizontal and 2 New cylindrical design to host larger detectors vertical for alignment runs only). and reduce the impedance and increase available vacuum compatibility in terms of outgassing, and particle shower development have to be taken space. Detector Only one inserted into account in the geometrical designpackage and in the choice of materials (Section 3.4). for high lumi runs Top • • The timing RPs are equipped with a 300 μm thick Approachingwindow very towards close the beam.to Horizontal the LHC beam• The thickness (~2 mm) is required to compensate the pressure inside movablegradient "Roman on the larger window. • No vertical stations needed because the alignment is Bottom Pot” vesselsdone in byevery propagating LHC tracks from the tracking stations. BeamThe tracking RPs are equipped withfill a thin window 150 μm thick towards the beam. The CT-PPS RPs are inserted at ~15σ from the LHC beam in standard high luminosity fills. 26 2 Figure 42: Top: drawings of the cylindrical detector housing for the new RPs designed to accomodate timing detectors. Bottom: the manufactured pots. Figure 43: Dimensions of the cylindrical RP. After considering various options and after an iterative optimisation, the following design has been adopted for the new RPs (Figures 42 and 43)[6].
    [Show full text]
  • Test of an ALFA Prototype Detector at the CERN SPS
    Test of an ALFA prototype detector at the CERN SPS MASTERARBEIT zur Erlangung des akademischen Grades Master of Science (M.Sc. Phys.)im Fach Physik eingereicht an der Mathematisch-Naturwissenschaftlichen Fakultät I Institut für Physik Humboldt-Universität zu Berlin von Yohany Rodríguez García geboren am 14.09.1973 in Bogotá - Kolumbien Präsident der Humboldt-Universität zu Berlin: Prof. Dr. Jan-Hendrik Olbertz Gutachter: 1. Herr Prof. Dr. Thomas Lohse 2. Herr Dr. Ulrich Husemann eingereicht am: 05. April 2011 Abstract ALFA (Absolute Luminosity for ATLAS) is a high-precision scintillating fibre de- tector which has been designed to determine the LHC absolute luminosity at the ATLAS interaction point. This detector consists of eight Roman Pots arranged in four pairs of detector modules on each side of ATLAS at a distance of 240 m. Each detector module is made of ten layers of two times 64 scintillating fibres each (U and V planes). The fibres are coupled to 64 channels Multi-Anodes PhotoMultipliers Tubes read out by compact front-end electronics. The detector modules approach the LHC beam axis up to 1.5 mm to determine the luminosity from the differential spectrum of elastically scattered protons using the optical theorem. This Master thesis deals with the study of hit multiplicity, layer efficiency and spatial resolution of an ALFA prototype using the data obtained during the test beam performed in 2009 at Super Proton Synchrotron (SPS) of CERN. Zusammenfassung ALFA (Absolute Luminosity for ATLAS) ist ein hochpräziser Spurdetektor aus szin- tillierenden Fasern, der konzipiert wurde, um die absoluten Luminosität von LHC an der ATLAS Interaktionspunkt zu messen.
    [Show full text]
  • Hard Diffraction at The
    Hard diffraction at the LHC Christophe Royon DAPNIA-SPP, CEA Saclay Seminar at Brookhaven National Laboratory, December 21 2006 Contents: Standard Higgs physics at the LHC • What is diffraction (HERA and Tevatron)? • Inclusive diffraction at the LHC • Diffractive Higgs production at the LHC: exclusive and • inclusive production Background studies: How to measure the high β gluon? • Exclusive top and stop production • Work done in collaboration with M. Boonekamp. J. Cammin, O. Kepka, A. Kupco, R. Peschanski, L. Schoeffel NB: Many results coming from the “Saclay” group, see also results from Durham group in particular (A. Martin, V. Khoze, M. Ryskin) LEP experiments limits on Higgs mass Q: ratio of the probability to observe what has been seen • if it is a Higgs signal by the probability to observe the same if it is only background Limit on Higgs mass: 114.4 GeV • 50 40 LEP -2 ln(Q) 30 20 10 0 -10 Observed Expected for background -20 Expected for signal plus background -30 106 108 110 112 114 116 118 120 2 mH(GeV/c ) Electroweak fits and mass of Higgs boson Use new Mtop, width of W boson from Tevatron and • LEP, and mass of W from LEP MHiggs = 89 + 42 30 GeV (68% CL), and < 175 GeV • at 95% CL − 6 Theory uncertainty LEP1 and SLD ∆α(5) = had LEP2 and Tevatron (prel.) 5 0.02758±0.00035 80.5 0.02749±0.00012 68% CL 2 4 incl. low Q data ] 2 GeV 3 [ 80.4 ∆χ W 2 m 1 80.3 ∆α mH [GeV] Excluded 114 300 1000 0 30100 300 150 175 200 mH [GeV] mt [GeV] Standard search for Higgs boson at the LHC Low masses: difficult region at the LHC: other ways of • finding
    [Show full text]
  • A Study of Double Pomeron Exchange in ALICE
    EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH ALICE/98-45 3 November 1998 A study of Double Pomeron Exchange in ALICE A. Kirk and O. Villalobos Baillie School of Physics and Astronomy, University of Birmingham, Birmingham, U.K. Abstract The non-Abelian nature of QCD suggests that particles that have a gluon constituent, such as glueballs or hybrids, should exist. Experiments WA76, WA91 and WA102 have performed a dedicated search for these states in central production using the CERN Omega Spectrometer. New results from central production show that there is a kinematical filter which can select out glueball candidates from known qq states. A further study of this at high energies is essential in order to get information on the M(X0) > 2 GeV region. This paper describes how this could be done using the the ALICE detector at the LHC. 1 Introduction Recent developments in the study of hadronic interactions show that central production is a mechanism which can be used to great advantage in the study of hadronic spectra. The current studies have been performed in fixed target experiment at √s 20 GeV. It would be of great interest to extend these studies to higher energies, where it should∼ be much easier to disentangle the production mechanism. This paper is organized as follows. In section 2 the spectrum of non-qq mesons is discussed, in section 3 the results from the Omega Central Production experiments are reviewed, and in section 4 a possible extension of these studies using the ALICE detector in pp mode is presented. 2 The Glueball Spectrum The present understanding of strong interactions is that they are described by Quantum Chro- moDynamics (QCD).
    [Show full text]
  • Central Exclusive Production in the STAR Experiment at RHIC
    Central Exclusive Production in the STAR Experiment at RHIC Rafal Sikora1 for the STAR Collaboration 1AGH University of Science and Technology, 30 Mickiewicza Ave, PL 30-059 Krakow, Poland E-mail: rafal.sikora@fis.agh.edu.pl Abstract. The STAR experiment at the Relativistic Heavy Ion Collider (RHIC) performs studies of diffractive processes with the −1 focus on the exclusive productionp of particles in central range of rapidity. In 2015 STAR collected 18 pb of data in polarized proton+proton collisions at s =200 GeV to measure Central Exclusive Production (CEP) process pp ! pXp through Double Pomeron Exchange (DPE) mechanism. The intact protons moving inside the RHIC beampipe after the collision were measured in silicon strip detectors (SSD), which were placed in the Roman Pot vessels. This enables full control over interaction kinematics and verification of the exclusivity of the reaction by measuring the total (missing) transverse momenta of all final state particles: the central diffractive system in the Time Projection Chamber (TPC) and the forward protons in the Roman Pots. With the use of ionization energy loss in the TPC, dE/dx, it was possible to discriminate various production channels in pp ! pXp reaction. This paper presents results on exclusive production of two charged particles (π+π− and K+K−) in mid-rapidity region, −1 < η < 1, with small squared four-momentum transfer of forward protons, 0:03 < −t < 0:3 (GeV=c)2, obtained using 2.5% of full statistics. INTRODUCTION A process is defined as exclusive when all particles in the final state, after the interaction, are measured and identified.
    [Show full text]
  • Arxiv:Hep-Ex/0602021V1 9 Feb 2006 N 4TV Ftetotal the of Tev) 14 and Aiiycvrg Pt H Eyfradrgo.Ti Is This High- Region
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Helsingin yliopiston digitaalinen arkisto EPJ manuscript No. (will be inserted by the editor) Diffraction and Total Cross-Section at the Tevatron and the LHC M. Deile1, G. Anelli1, A. Aurola2, V. Avati1, V. Berardi3, U.Bottigli4, M. Bozzo5, E. Br¨ucken2, A. Buzzo5, M. Calicchio3, F. Capurro5, M.G. Catanesi3, M.A.Ciocci4, S. Cuneo5, C. Da Vi`a6, E. Dimovasili1, K. Eggert1, M. Er¨aluoto2, F. Ferro5, A. Giachero5, J.P. Guillaud7, J. Hasi6, F. Haug1, J. Heino2, T. Hilden2, P. Jarron1, J. Kalliopuska2, J. Kaˇspar8, J. Kempa9, C. Kenney10, A. Kok6, V. Kundr´at8, K. Kurvinen2, S. Lami4, J. L¨ams¨a2, G. Latino4, R. Lauhakangas2, J. Lippmaa2, M. Lokaj´ıˇcek8, M. LoVetere5, D. Macina1, M. Macr´ı5, M. Meucci4, S. Minutoli5, A. Morelli5, P. Musico5, M. Negri5, H. Niewiadomski1, E. Noschis1, J. Ojala2, F. Oljemark2, R. Orava2, M. Oriunno1, K. Osterberg¨ 2, R.Paoletti4, S. Parker11, A.-L. Perrot1, E. Radermacher1, E. Radicioni3, E. Robutti5, L. Ropelewski1, G. Ruggiero1, H. Saarikko2, G.Sanguinetti4, A. Santroni5, S. Saramad1, F. Sauli1, A.Scribano4, G. Sette5, J. Smotlacha8, W. Snoeys1, C. Taylor12, A. Toppinen2, N.Turini4, N. Van Remortel2, L. Verardo5, A. Verdier1, S. Watts6, and J. Whitmore13 1 CERN, Gen`eve, Switzerland 2 Helsinki Institute of Physics and University of Helsinki, Finland 3 INFN Sezione di Bari and Politecnico di Bari, Bari, Italy 4 Universit`adi Siena and Sezione INFN-Pisa, Italy 5 Universit`adi Genova and Sezione INFN, Genova, Italy 6 Brunel University, Uxbridge, UK 7 LAPP Annecy, France 8 Academy of Sciences of the Czech Republic and Institute of Physics, Praha, Czech Republic 9 Warsaw University of Technology, Plock, Poland 10 Molecular Biology Consortium, SLAC, USA 11 University of Hawaii, USA 12 Case Western Reserve University, Dept.
    [Show full text]
  • Elastic Scattering of Protons at the TOTEM Experiment at the LHC
    Elastic scattering of protons at the TOTEM experiment at the LHC A thesis submitted to the E¨otv¨os University of Budapest for the degree of Doctor of Philosophy in the Faculty of Natural Sciences Written by: Frigyes Nemes PhD School of Physics Particle and Astrophysics program PhD school leader: Dr. L´aszl´oPalla, professor PhD program leader: Dr. Ferenc Csikor, professor Supervisor: Tam´as Cs¨org˝o, DSc, scientific advisor, honorary professor Co-Supervisor: Dr. M´at´eCsan´ad, associate professor 2015 Elastic scattering of protons at the TOTEM experiment at the LHC A thesis presented for the degree of Doctor of Philosophy Written by: Frigyes Nemes E¨otv¨os University, Budapest, Hungary, PhD School of Physics, Particle and Astrophysics program, 2015 PhD school leader: Dr. L´aszl´oPalla, DSc, professor PhD program leader: Dr. Ferenc Csikor, DSc, professor Supervisor: Tam´as Cs¨org˝o, Member of the European Academy, DSc, scientific advisor, honorary professor Co-Supervisor: Dr. M´at´eCsan´ad, associate professor 1 Abstract The TOTEM experiment at the LHC at CERN is optimized to measure elastic and diffractive scattering at the LHC and measures the total proton-proton cross-section with the luminosity-independent method. The TOTEM experiment uses the special technique of movable beam pipe insertions – called Roman Pots – to detect very forward protons. The reconstruction of the forward proton kinematics requires the precise understanding of the LHC beam optics. A new method of LHC optics determination is reported, which exploits kinematical distributions of elastically scattered proton-proton data measured by the Roman Pots of the TOTEM experiment.
    [Show full text]