Event Recorded by ATLAS When the LHC's Beam 2 Reached Closed

Total Page:16

File Type:pdf, Size:1020Kb

Event Recorded by ATLAS When the LHC's Beam 2 Reached Closed A ‘beam splash’ event recorded by ATLAS when the LHC’s beam 2 reached closed collimators near the detector on 20 November. 12 | CERN “The imminent start-up of the LHC is an event that excites everyone who has an interest in the fundamental physics of the Universe.” Kaname Ikeda, ITER Director-General, CERN Bulletin, 19 October 2009. Physics and Experiments The moment that particle physicists around the world had been The EMCal is an upgrade for ALICE, having received full waiting for finally arrived on 20 November 2009 when protons approval and construction funds only in early 2008. It will detect circulated again round the LHC. Over the following days, the high-energy photons and neutral pions, as well as the neutral machine passed a number of milestones, from the first collisions component of ‘jets’ of particles as they emerge from quark� at 450 GeV per beam to collisions at a total energy of 2.36 TeV gluon plasma formed in collisions between heavy ions; most — a world record. At the same time, the LHC experiments importantly, it will provide the means to select these events on began to collect data, allowing the collaborations to calibrate line. The EMCal is basically a matrix of scintillator and lead, detectors and assess their performance prior to the real attack which is contained in ‘supermodules’ that weigh about eight tonnes. It will consist of ten full supermodules and two partial on high-energy physics in 2010. supermodules. The repairs to the LHC and subsequent consolidation work For the ATLAS Collaboration, crucial repair work included following the incident in September 2008 took approximately modifications to the cooling system for the inner detector. one year (see p. 21). The teams working on the six LHC The shutdown also allowed some schedules to advance. This experiments — ALICE, ATLAS, CMS, LHCb, LHCf and included the partial installation of muon chambers in the region TOTEM — put this time to good use, undertaking maintenance, between the central barrel of the experiment and the endcaps, repair and installation work, as well as major test runs with which had been originally deferred. As a result, by the autumn cosmic rays. the ATLAS experiment was even better prepared for collisions than it had been in 2008. Installation and maintenance Some of the most important work on the CMS experiment Consolidation work on the ALICE experiment began as soon involved the complete refurbishment of the cooling system for as the LHC stopped. A major operation to move the cabling of the tracker. Other items included some channels of a few muon the inner tracking system to allow more space and better access detectors, which were removed, repaired and reinstalled. The took until July 2009. Other maintenance included replacing CMS Collaboration also installed the final sub-detector, the a number of capacitors on the time projection chamber. The pre-shower, which sits in front of the endcap calorimeters. The shutdown also provided the opportunity for installation work pre-shower consists of a lead�silicon ‘sandwich’ with silicon that was originally scheduled for after the first LHC run. Further sensors comprising strips that are 2 mm wide. It can distinguish modules were installed in the transition radiation detector and between single photons and pairs of ‘overlapping’ photons in the photon multiplicity detector, but the biggest addition arising from the decays of neutral pions in the endcap region, was the new electromagnetic calorimeter (EMCal). where particularly large numbers of particles will be produced. 2009 | 13 Installation of the EMCal supermodules in ALICE ‘Edgeless’ silicon detectors in one of the Roman pots used in employs a special device to insert them between the magnet the TOTEM experiment. coil and the time-of-flight counters. This is a crucial task when trying to spot certain decays of which allow the detectors to come to within 1 mm of the particles such as the long-sought Higgs boson. beam. There are currently two Roman pot stations, each one at a distance of 220 m from the interaction point. Each station The LHCb Collaboration took the opportunity to finish their contains six pots. For the start-up in 2008 only two pots had detector completely, with the installation of the final muon the silicon detectors in place. The collaboration completed the chambers. Other improvements included modifications to installation of the other four pots in 2009. In the future, two reduce noise in the electromagnetic calorimeter to a negligible more stations will be installed at 147 m. level and upgrades to the computing network. Cosmic calibrations LHCf is a small experiment made up of two independent Cosmic rays provide a natural source of particles, in particular detectors located in the tunnel at 140 m to either side of the muons, that proved extremely valuable for checking and aligning ATLAS collision point. Both detectors were completed and detectors before the LHC restarted. In a five-week data-taking ready to take data in 2008. During the shutdown period the exercise in July–August, CRAFT (Cosmic Rays At Four Tesla), LHCf Collaboration worked mainly to optimize the data the CMS experiment recorded more than 300 million cosmic acquisition system. events with the magnetic field on. This large data-set was used to improve further the alignment, calibration and performance The TOTEM experiment is situated in the CMS cavern, with of the various sub-detectors prior to collisions in the LHC. detectors on both sides of the interaction point. On each side there are two charged-particle trackers, T1 and T2, at distances The full ALICE detector system (with nearly 40% of the of about 10.5 m and 13.5 m from the interaction point; indeed, EMCal installed) ran with cosmic rays from August to October. T1 is within the endcap of CMS. During the shutdown, the Altogether, the experiment accumulated more than 600 million remaining three quarters of the T2 detector were tested and cosmic events during the year, both with and without the installed. The T1 detector was also assembled and tested with magnets turned on. beam from the SPS. It will be installed at the next opportunity. During the shutdown, the ATLAS Collaboration continued In addition TOTEM has silicon detectors installed in ‘Roman the analysis of cosmic data collected in 2008. This allowed for pots’. These are movable devices inserted in to the beam pipe, detailed alignment and calibrations studies, reaching a precision 14 | CERN In June, tests of the beam transfer systems from the SPS A ‘splash’ event in CMS recorded at the beginning of to the LHC allowed the reconstruction of tracks through November when beam travelled as far as collimators just the Vertex Locator in LHCb. before Point 5. far beyond expectations for this stage of the experiment. Once beam entered the LHC just before Point 2, where the ALICE the detector was fully closed again in September 2009 cosmic- experiment is installed, and was dumped before Point 3. ray studies restarted, and from mid-October, with the control Several sub-detectors of ALICE saw their first beam. This room staffed round the clock, the experiment collected cosmic helped the collaboration to synchronize with the LHC clock data continuously until first beam appeared in the LHC. and test the capability to measure large numbers of particles simultaneously. LHCb differs in design from the other big experiments, as its detectors are aligned along the LHC beam line to observe the decay of B mesons. These particles, which are a major focus for During the following day, protons were injected into the LHCb’s studies, stay close to the beam pipe as they fly out from anticlockwise beam pipe of the LHC. They passed through the the collision zone. Near-horizontal cosmic-rays proved valuable LHCb experiment at Point 8 before being dumped just before for checking and aligning the outer parts of the LHCb detector, Point 7. Most of the LHCb sub-detectors were switched off to and allowed the observation of the first rings from one of the keep the experiment safe at this early stage, but a highlight was two ring-imaging Cherenkov detectors, RICH1. the switching-on of the LHCb magnet. This allowed the LHC operators to measure its effect on the LHC beam and to adjust The rate of horizontal cosmic rays is too low to align smaller the magnetic compensators around LHCb to keep the beam in components near the beam line in LHCb, but fortunately the orbit. experiment is located close to the point where the anticlockwise beam enters the LHC. During tests of the transfer line from the SPS to the LHC in June, the beam was directed into a beam The first weekend of November saw protons complete their stopper, which produced dense bursts of muons that crossed journey anticlockwise through three octants of the LHC before LHCb horizontally. This allowed the collaboration to align the being dumped in collimators just prior to entering the cavern vertex detector and the inner tracker to a few microns. of the CMS experiment at Point 5. The particles produced by the impact of the protons on the collimators left energy and First beam tracks in the experiment’s calorimeters and muon chambers, On 23 October, particles entered the LHC for the first time respectively. The more delicate inner detectors remained since September 2008, during tests to provide lead ions. The switched off for reasons of protection. 2009 | 15 A proton–proton collision at 900 GeV recorded by the Tracks in the ATLAS inner detectors show the decay of a ALICE experiment with all the sub-detectors switched on neutral kaon to two pions (red) in this event from stable during stable running on 6 December.
Recommended publications
  • CERN Courier–Digital Edition
    CERNMarch/April 2021 cerncourier.com COURIERReporting on international high-energy physics WELCOME CERN Courier – digital edition Welcome to the digital edition of the March/April 2021 issue of CERN Courier. Hadron colliders have contributed to a golden era of discovery in high-energy physics, hosting experiments that have enabled physicists to unearth the cornerstones of the Standard Model. This success story began 50 years ago with CERN’s Intersecting Storage Rings (featured on the cover of this issue) and culminated in the Large Hadron Collider (p38) – which has spawned thousands of papers in its first 10 years of operations alone (p47). It also bodes well for a potential future circular collider at CERN operating at a centre-of-mass energy of at least 100 TeV, a feasibility study for which is now in full swing. Even hadron colliders have their limits, however. To explore possible new physics at the highest energy scales, physicists are mounting a series of experiments to search for very weakly interacting “slim” particles that arise from extensions in the Standard Model (p25). Also celebrating a golden anniversary this year is the Institute for Nuclear Research in Moscow (p33), while, elsewhere in this issue: quantum sensors HADRON COLLIDERS target gravitational waves (p10); X-rays go behind the scenes of supernova 50 years of discovery 1987A (p12); a high-performance computing collaboration forms to handle the big-physics data onslaught (p22); Steven Weinberg talks about his latest work (p51); and much more. To sign up to the new-issue alert, please visit: http://comms.iop.org/k/iop/cerncourier To subscribe to the magazine, please visit: https://cerncourier.com/p/about-cern-courier EDITOR: MATTHEW CHALMERS, CERN DIGITAL EDITION CREATED BY IOP PUBLISHING ATLAS spots rare Higgs decay Weinberg on effective field theory Hunting for WISPs CCMarApr21_Cover_v1.indd 1 12/02/2021 09:24 CERNCOURIER www.
    [Show full text]
  • Very Forward Photon Production in Proton-Proton Collisions Measured by the Lhcf Experiment at the Large Hadron Collider
    Very forward photon production in proton-proton collisions measured by the LHCf experiment at the Large Hadron Collider Author: Alessio Tiberio Supervisor: Lorenzo Bonechi The LHC-forward (LHCf) experiment, situated at the LHC accelerator, has measured neutral particles production in a very forward region (pseudo-rapidity η > 8:4) in proton-proton and proton- lead collisions. The main purpose of the LHCf experiment is to test hadronic interaction models used in ground based cosmic rays experiments to simulate cosmic rays induced air-showers in the Earth's atmosphere. Highest energy cosmic rays can only be detected from secondary particles which are produced by the interaction of the primary particle with nuclei of the atmosphere. Studying the development of air showers, it is possible to reconstruct the type and kinematic parameters of primary particle. For this reason, Monte Carlo (MC) simulations with accurate hadronic interaction models are needed to reproduce the development of air-showers. Since the energy flow of secondary particles is concentrated in the forward direction, measurements of particle production at high pseudo-rapidity (i.e. small angles) are very important. Furthermore, soft QCD interactions (non perturbative regime) dominates in the very forward region and MC simulations of air showers are based on phenomenological model, so inputs from experimental data are crucial. The experiment is composed by two independent detectors (Arm1 and Arm2 ) located at 140 m from the ATLAS's interaction point (IP1) on opposite sides [1]. Detectors are placed inside the Target Neutral Absorber (TAN), where the beam pipe from IP1 turns into two separates tubes: the position between the two beam pipes allows to measure particles produced at zero degrees.
    [Show full text]
  • CERN to Seek Answers to Such Fundamental 1957, Was CERN’S First Accelerator
    What is the nature of our universe? What is it ----------------------------------------- DAY 1 -------- made of? Scientists from around the world go to The 600 MeV Synchrocyclotron (SC), built in CERN to seek answers to such fundamental 1957, was CERN’s first accelerator. It provided questions using particle accelerators and pushing beams for CERN’s first experiments in particle and nuclear the limits of technology. physics. In 1964, this machine started to concentrate on nuclear physics alone, leaving particle physics to the newer During February 2019, I was given a once in a lifetime and more powerful Proton Synchrotron. opportunity to be part of The Maltese Teacher Programme at CERN, which introduced me, as one of the participants, to cutting-edge particle physics through lectures, on-site visits, exhibitions, and hands-on workshops. Why do they do all this? The main objective of these type of visits is to bring modern science into the classroom. Through this report, my purpose is to give an insight of what goes on at CERN as well as share my experience with you students, colleagues, as well as the general public. The SC became a remarkably long-lived machine. In 1967, it started supplying beams for a dedicated radioactive-ion-beam facility called ISOLDE, which still carries out research ranging from pure What does “CERN” stand for? At an nuclear physics to astrophysics and medical physics. In 1990, intergovernmental meeting of UNESCO in Paris in ISOLDE was transferred to the Proton Synchrotron Booster, and the SC closed down after 33 years of service. December 1951, the first resolution concerning the establishment of a European Council for Nuclear Research SM18 is CERN’s main facility for testing large and heavy (in French Conseil Européen pour la Recherche Nucléaire) superconducting magnets at liquid helium temperatures.
    [Show full text]
  • Detection of Cosmic Rays at the LHC Detection of Cosmic Rays at the LHC
    Particle and Astroparticle Physics at the Large Hadron Collider --Hadronic Interactions-- Albert De Roeck CERN, Geneva, Switzerland Antwerp University Belgium UC-Davis California USA NTU, Singapore November 15th 2019 Outline • Introduction on the LHC and LHC physics program • LHC results for Astroparticle physics • Measurements of event characteristics at 13 TeV • Forward measurements • Cosmic ray measurements • LHC and light ions? • Summary The LHC Machine and Experiments MoEDAL LHCf FASER totem CM energy → Run-1: (2010-2012) 7/8 TeV Run-2: (2015-2018) 13 TeV -> Now 8 experiments Run-2 starts proton-proton Run-2 finished 24/10/18 6:00am 2018 2010-2012: Run-1 at 7/8 TeV CM energy Collected ~ 27 fb-1 2015-2018: Run-2 at 13 TeV CM Energy Collected ~ 140 fb-1 2021-2023/24 : Run-3 Expect ⇨ 14 TeV CM Energy and ~ 200/300 fb-1 The LHC is also a Heavy Ion Collider ALICE Data taking during the HI run • All experiments take AA or pA data (except TOTEM) Expected for Run-3: in addition short pO and OO runs ⇨ pO certainly of interest for Cosmic Ray Physics Community! 4 10 years of LHC Operation • LHC: 7 TeV in March 2010 ->The highest energy in the lab! • LHC @ 13 TeV from 2015 onwards March 30 2010 …waiting.. • Most important highlight so far: …since 4:00 am The discovery of a Higgs boson • Many results on Standard Model process measurements, QCD and particle production, top-physics, b-physics, heavy ion physics, searches, Higgs physics • Waiting for the next discovery… -> Searches beyond the Standard Model 12:58 7 TeV collisions!!! New Physics Hunters
    [Show full text]
  • Beam–Material Interactions
    Beam–Material Interactions N.V. Mokhov1 and F. Cerutti2 1Fermilab, Batavia, IL 60510, USA 2CERN, Geneva, Switzerland Abstract This paper is motivated by the growing importance of better understanding of the phenomena and consequences of high-intensity energetic particle beam interactions with accelerator, generic target, and detector components. It reviews the principal physical processes of fast-particle interactions with matter, effects in materials under irradiation, materials response, related to component lifetime and performance, simulation techniques, and methods of mitigating the impact of radiation on the components and environment in challenging current and future applications. Keywords Particle physics simulation; material irradiation effects; accelerator design. 1 Introduction The next generation of medium- and high-energy accelerators for megawatt proton, electron, and heavy- ion beams moves us into a completely new domain of extreme energy deposition density up to 0.1 MJ/g and power density up to 1 TW/g in beam interactions with matter [1, 2]. The consequences of controlled and uncontrolled impacts of such high-intensity beams on components of accelerators, beamlines, target stations, beam collimators and absorbers, detectors, shielding, and the environment can range from minor to catastrophic. Challenges also arise from the increasing complexity of accelerators and experimental set-ups, as well as from design, engineering, and performance constraints. All these factors put unprecedented requirements on the accuracy of particle production predictions, the capability and reliability of the codes used in planning new accelerator facilities and experiments, the design of machine, target, and collimation systems, new materials and technologies, detectors, and radiation shielding and the minimization of radiation impact on the environment.
    [Show full text]
  • Sub Atomic Particles and Phy 009 Sub Atomic Particles and Developments in Cern Developments in Cern
    1) Mahantesh L Chikkadesai 2) Ramakrishna R Pujari [email protected] [email protected] Mobile no: +919480780580 Mobile no: +917411812551 Phy 009 Sub atomic particles and Phy 009 Sub atomic particles and developments in cern developments in cern Electrical and Electronics Electrical and Electronics KLS’s Vishwanathrao deshpande rural KLS’s Vishwanathrao deshpande rural institute of technology institute of technology Haliyal, Uttar Kannada Haliyal, Uttar Kannada SUB ATOMIC PARTICLES AND DEVELOPMENTS IN CERN Abstract-This paper reviews past and present cosmic rays. Anderson discovered their existence; developments of sub atomic particles in CERN. It High-energy subato mic particles in the form gives the information of sub atomic particles and of cosmic rays continually rain down on the Earth’s deals with basic concepts of particle physics, atmosphere from outer space. classification and characteristics of them. Sub atomic More-unusual subatomic particles —such as particles also called elementary particle, any of various self-contained units of matter or energy that the positron, the antimatter counterpart of the are the fundamental constituents of all matter. All of electron—have been detected and characterized the known matter in the universe today is made up of in cosmic-ray interactions in the Earth’s elementary particles (quarks and leptons), held atmosphere. together by fundamental forces which are Quarks and electrons are some of the elementary represente d by the exchange of particles known as particles we study at CERN and in other gauge bosons. Standard model is the theory that laboratories. But physicists have found more of describes the role of these fundamental particles and these elementary particles in various experiments.
    [Show full text]
  • Particle Accelerators and Experiments Albert De Roeck CERN, Geneva, Switzerland Antwerp University Belgium UC-Davis California USA NTU, Singapore
    Particle Accelerators and Experiments Albert De Roeck CERN, Geneva, Switzerland Antwerp University Belgium UC-Davis California USA NTU, Singapore March 30th- April 2nd Muscat 1 Part I Accelerators 2 Different types of Methodology tools and equipment are needed to observe different sizes of object Only particle accelerators can explore the tiniest objects in the 5 Universe 5 Accelerators are Powerful Microscopes Planck constant They make high energy particle beams h = momentum that allow us to see small things. wavelength p ~ energy seen by low energy seen by high energy beam of particles beam of particles (poorer resolution) (better resolution) High Energy Physics Experiments Rutherford experiment (1909) Centre of mass energy squared s=E1m2 Centre of mass energy squared s=4E1E2 Detectors techniques have followed these developments Accelerators for Charged Particles 9 Recent High Energy Colliders Highest energies can be reached with proton colliders Machine Year Beams Energy (s) Luminosity SPPS (CERN) 1981 pp 630-900 GeV 6.1030cm-2s-1 Tevatron (FNAL) 1987 pp 1800-2000 GeV 1031-1032cm-2s-1 SLC (SLAC) 1989 e+e- 90 GeV 1030cm-2s-1 LEP (CERN) 1989 e+e- 90-200 GeV 1031-1032cm-2s-1 HERA (DESY) 1992 ep 300 GeV 1031-1032cm-2s-1 RHIC (BNL) 2000 pp /AA 200-500 GeV 1032cm-2s-1 LHC (CERN) 2009 pp (AA) 7-14 TeV 1033-1034cm-2s-1 Luminosity = number of events/cross section/sec • Limits on circular machines – Proton colliders: Dipole magnet strength superconducting magnets – Electron colliders: Synchrotron10 radiation/RF power: loss ~E4/R2 How Many Accelerators Worldwide? a) 1-10 b) 10-100 c) 100-1,000 d) 1,000-10,000 e) > 10,000 11 Accelerators Worldwide > 25,000 accelerators in use 12 Accelerators Worldwide 44% Radio- therapy 13 Accelerators Worldwide 44% 40% Radio- Ion therapy implant.
    [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 Muon Puzzle in Cosmic-Ray Induced Air Showers and Its Connection to the Large Hadron Collider
    The Muon Puzzle in cosmic-ray induced air showers and its connection to the Large Hadron Collider 1 2 Johannes Albrecht • Lorenzo Cazon • 1,? 3 Hans Dembinski • Anatoli Fedynitch • 4 5 Karl-Heinz Kampert • Tanguy Pierog • 1 6 Wolfgang Rhode • Dennis Soldin • 1 5 5 Bernhard Spaan • Ralf Ulrich • Michael Unger Abstract High-energy cosmic rays are observed indi- Hadron Collider. An effect that can potentially explain rectly by detecting the extensive air showers initiated the puzzle has been discovered at the LHC, but needs to in Earth's atmosphere. The interpretation of these be confirmed for forward produced hadrons with LHCb, observations relies on accurate models of air shower and with future data on oxygen beams. physics, which is a challenge and an opportunity to test QCD under extreme conditions. Air showers are Keywords cosmic rays, air showers, particle physics, hadronic cascades, which eventually decay into muons. strangeness enhancement, cosmic rays, mass composi- The muon number is a key observable to infer the tion mass composition of cosmic rays. Air shower simula- tions with state-of-the-art QCD models show a signif- icant muon deficit with respect to measurements; this 1 Introduction is called the Muon Puzzle. The origin of this discrep- ancy has been traced to the composition of secondary Cosmic rays are fully-ionised nuclei with relativistic particles in hadronic interactions. The muon discrep- kinetic energies that arrive at Earth. The elements ancy starts at the TeV scale, which suggests that this range from proton to iron, with a negligible fraction change in hadron composition is observable at the Large of heavier nuclei.
    [Show full text]
  • CERN's Scientific Strategy
    CERN’s Scientific Strategy Fabiola Gianotti ECFA HL-LHC Experiments Workshop, Aix-Les-Bains, 3/10/2016 CERN’s scientific strategy (based on ESPP): three pillars Full exploitation of the LHC: successful operation of the nominal LHC (Run 2, LS2, Run 3) construction and installation of LHC upgrades: LIU (LHC Injectors Upgrade) and HL-LHC Scientific diversity programme serving a broad community: ongoing experiments and facilities at Booster, PS, SPS and their upgrades (ELENA, HIE-ISOLDE) participation in accelerator-based neutrino projects outside Europe (presently mainly LBNF in the US) through CERN Neutrino Platform Preparation of CERN’s future: vibrant accelerator R&D programme exploiting CERN’s strengths and uniqueness (including superconducting high-field magnets, AWAKE, etc.) design studies for future accelerators: CLIC, FCC (includes HE-LHC) future opportunities of diversity programme (new): “Physics Beyond Colliders” Study Group Important milestone: update of the European Strategy for Particle Physics (ESPP): ~ 2019-2020 CERN’s scientific strategy (based on ESPP): three pillars Covered in this WS I will say ~nothing Full exploitation of the LHC: successful operation of the nominal LHC (Run 2, LS2, Run 3) construction and installation of LHC upgrades: LIU (LHC Injectors Upgrade) and HL-LHC Scientific diversity programme serving a broad community: ongoing experiments and facilities at Booster, PS, SPS and their upgrades (ELENA, HIE-ISOLDE) participation in accelerator-based neutrino projects outside Europe (presently mainly
    [Show full text]
  • Results from Lhcf Experiment
    EPJ Web of Conferences 28, 02003 (2012) DOI: 10.1051/epjconf/ 20122802003 C Owned by the authors, published by EDP Sciences, 2012 Results from LHCf Experiment Alessia Tricomi on behalf of the LHCf Collaboration University of Catania and INFN Catania, Italy √ Abstract.√ The LHCf experiment has taken data in 2009 and 2010 p-p collisions at LHC at s = 0.9 TeV and s = 7 TeV. The measurement of the forward neutral particle spectra produced in proton-proton collisions at LHC up to an energy of 14 TeV in the center of mass system are of fundamental importance to calibrate the Monte Carlo models widely used in the high energy cosmic ray (HECR) field, up to an equivalent laboratory energy of the order of 1017 eV. In this paper the first results on the inclusive photon spectrum measured by LHCf is reported. Comparison of this spectrum with the model expectations show significant discrepancies, mainly in the high energy region. In addition, perspectives for future analyses as well as the program for the next data taking period, in particular the possibility to take data in p-Pb collisions, will be discussed. 1 Introduction Each calorimeter (ARM1 and ARM2) has a double tower structure, with the smaller tower located at zero degree col- The LHCf experiment at LHC has been designed to cali- lision angle, approximately covering the region with pseudo- brate the hadron interaction models used in High Energy rapidity η > 10 and the larger one, approximately cover- Cosmic Ray (HECR) Physics through the measurement of ing the region with 8.4 < η < 10.
    [Show full text]
  • Lambda and Anti-Labmda Production in the ALICE Experiment at the LHC
    LLNL-TR-643836 Lambda and Anti-Labmda production in the ALICE experiment at the LHC. R. Carmona, R. Soltz September 12, 2013 Disclaimer This document was prepared as an account of work sponsored by an agency of the United States government. Neither the United States government nor Lawrence Livermore National Security, LLC, nor any of their employees makes any warranty, expressed or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States government or Lawrence Livermore National Security, LLC. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States government or Lawrence Livermore National Security, LLC, and shall not be used for advertising or product endorsement purposes. This work performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344. Strangeness Production in Jets with ALICE at the LHC Rodney Carmona, Mike Tyler II, Ron Soltz, Austin Harton, Edmundo Garcia Chicago State University, Lawrence Livermore National Laboratory Cern (European Organization for Nuclear Research) At this laboratory Physicists and Engineers study fundamental particles using the world’s largest and most complex instruments. Here particles are made to collide at close to the speed of light to see how they interact and help to discover the basic laws of nature.
    [Show full text]