ATLAS Experiment at the CERN Large Hadron Collider

Total Page:16

File Type:pdf, Size:1020Kb

ATLAS Experiment at the CERN Large Hadron Collider ATLASATLAS experimentexperiment atat thethe CERNCERN LargeLarge HadronHadron ColliderCollider Peter Watkins, Head of Particle Physics Group, University of Birmingham, UK [email protected] Large Hadron Collider (LHC) PointPoint 11 activitiesactivities andand perspectivesperspectives MarzioMarzio NessiNessi ATLASATLAS plenaryplenary d OutlineOutline ofof talktalk •• BuildingBuilding blocksblocks ofof thethe universeuniverse •• WhyWhy dodo experimentsexperiments atat thethe LHCLHC ?? •• LHC,LHC, ATLASATLAS andand collaborationcollaboration •• SearchingSearching forfor aa newnew particleparticle •• RecentRecent LHCLHC newsnews AcknowledgementsAcknowledgements –– ManyMany slidesslides fromfrom LHCLHC colleaguescolleagues 4 The very small electron nucleus proton neutron up quark down quark 10-14 m10-15 m< 10-18 m 10-10 m (thickness of human hair ~ 10-5 m) FundamentalFundamental ForcesForces All forces are carried by particles ! Gravity – solar system, galaxies …- extremely weak force Electromagnetic – atoms, electricity ….. - carried by photons Weak force – beta decay and how stars generate energy - carried by massive W and Z bosons Strong – binds quarks inside proton carried by gluons Higgs boson? TheThe HiggsHiggs BosonBoson One key objective of the LHC is to understand the origin of mass – is it due to a universal Higgs field? (A Higgs field everywhere with the Higgs boson as the force carrier?). Massless particles are not impeded by the Higgs field and, thus, travel at the speed of light. Analogy: Downhill skier experiences no drag by the snow field. Light particles interact weakly with the Higgs field and travel slower. Analogy: Snowshoes on the top of the snow field experience some drag. Heavy particles interact strongly with the Higgs field and travel very slowly. Analogy: Wading through the snow field is a big drag! We call this drag “Mass”. WhatWhat elseelse isis outout there?there? •• VariousVarious ideasideas consideredconsidered…… •• DarkDark mattermatter • •• ExtraExtra dimensionsdimensions ofof spacespace • Suggested by superstring theory •• MicroscopicMicroscopic blackblack holesholes TheThe LHCLHC experimentsexperiments cancan looklook forfor allall ofof thesethese.. AlsoAlso sensitivesensitive toto somethingsomething “completely“completely different”different” TheThe LargeLarge HadronHadron ColliderCollider (LHC)(LHC) Mont Blanc The LHC is a 27km accelerator that collides counter-rotating beams of protons of up to 7 TeV. Geneva (Tev = million million eV) Airport Energy densities similar to billionths of a second after the big-bang will be recreated at collision points CERN laboratory on Swiss – French border BuildingBuilding thethe LHCLHC In the main ring: 1746 superconducting magnets … including 1232 15m SC dipoles … weighing 27 tonnes each … producing 8.36 Tesla … and running at –270c … needs 700,000 litres liquid He … and 12 million litres liquid N2 TheThe fastestfastest racetrackracetrack onon thethe planetplanet The protons will reach 99.9999991% speed of light, and go round the 27km ring 11,000 times per second CollisionCollision pointspoints At four places the beams intersect HotHot spotsspots tootoo !! When the two beams of protons collide, they will generate temperatures 1000 million times hotter than the heart of the sun, but in a minuscule space ATLASATLAS DetectorDetector 7,000 tonnes 42m long 22m wide 22m high (About the height of a 5 storey building) 2,800 Physicists 169 Institutes 37 Countries ElectromagneticElectromagnetic CalorimeterCalorimeter AA basicbasic calorimetercalorimeter Basics The past Challenges Where to start? Detector Design Tracker Calorimetry Particle ID LHC detectors “Events” Final thoughts Total # of particles is proportional to energy of incoming particle Active detector slices produce a signal proportional to the number of charged particles traversing MuonMuon DetectorsDetectors E2 = p2c2+ m2c4 DiscoveringDiscovering aa newnew particleparticle TheThe collisioncollision raterate challengechallenge •• ProtonProton bunchesbunches collidecollide 4040 millionmillion timestimes aa secondsecond •• ~25~25 protonproton--protonproton collisionscollisions occuroccur eacheach timetime •• 10000000001000000000 collisionscollisions perper secsec –– 200200 perper secondsecond limitlimit forfor recordingrecording •• SelectSelect thethe mostmost ‘‘interestinginteresting’’ collisionscollisions inin fewfew microsecondsmicroseconds SearchingSearching forfor RareRare PhenomenaPhenomena Number of collisions All interactions 9 orders of magnitude The HIGGS Collision energy 50 magnets repaired 3 km of beam pipe cleaned LHCLHC statusstatus andand plansplans •• LargeLarge HadronHadron ColliderCollider restartedrestarted inin NovNov 20092009 andand isis workingworking wellwell •• WorldWorld recordrecord waswas setset forfor collisioncollision energyenergy inin DecemberDecember 20092009 •• OnOn MarchMarch 3030th 20102010 thethe collisioncollision energyenergy waswas increasedincreased toto 77 TeVTeV •• SomeSome earlyearly measurementsmeasurements alreadyalready publishedpublished •• SearchSearch forfor HiggsHiggs bosonboson needsneeds moremore collisionscollisions ZZ bosonboson candidatecandidate SummarySummary •• ManyMany peoplepeople areare interestedinterested inin thethe LHCLHC andand thethe keykey ideasideas areare widelywidely accessibleaccessible •• TheThe searchessearches forfor newnew particlesparticles areare onlyonly justjust beginningbeginning andand willwill lastlast forfor aa decadedecade •• WeWe workwork onon sharingsharing thethe excitementexcitement ofof thethe projectproject withwith thethe widestwidest possiblepossible audienceaudience •• WeWe needneed youryour helphelp toto dodo thisthis toto anan eveneven widerwider audience!audience! Thanks for listening .
Recommended publications
  • The ATLAS Experiment
    The ATLAS Experiment Mapping the Secrets of the Universe Michael Barnett Physics Division July 2007 With help from: Joao Pequenao Paul Schaffner M. Barnett – July 2007 1 Large Hadron Collider CERN lab in Geneva Switzerland Protons will circulate in opposite directions and collide inside experimental areas 100 meters underground 17 miles around M. Barnett – July 2007 2 The ATLAS Experiment See animation M. Barnett – July 2007 3 Large Hadron Collider Numbers The fastest racetrack on the planet Trillions of protons will race around the 17-mile ring 11,000 times a second, traveling at 99.9999991% the speed of light. Seven times the energy of any previous accelerator. The emptiest space in the solar system Accelerating protons to almost the speed of light requires a vacuum as empty as interplanetary space. There is 10 times more atmosphere on the moon than there will be in the LHC. M. Barnett – July 2007 4 Large Hadron Collider Numbers The hottest spot in our galaxy Colliding protons will generate temperatures 100,000 times hotter than the sun (but in a minuscule space). Equivalent to a billionth of a second after the Big Bang M. Barnett – July 2007 5 LHC Exhibition at London Science Museum M. Barnett – July 2007 6 Large Hadron Collider Numbers The biggest most sophisticated detectors ever built Recording the debris from 600 million proton collisions per second requires building gargantuan devices that measure particles with 0.0004 inch precision. The most extensive computer system in the world Analyzing the data requires tens of thousands of computers around the world using the Grid.
    [Show full text]
  • Aaron Taylor Physics and Astronomy This
    Aaron Taylor Candidate Physics and Astronomy Department This dissertation is approved, and it is acceptable in quality and form for publication: Approved by the Dissertation Committee: Dr. Sally Seidel , Chairperson Dr. Pavel Reznicek Dr. Huaiyu Duan Dr. Douglas Fields Dr. Bruce Schumm CERN-THESIS-2017-006 04/11/2016 SEARCH FOR NEW PHYSICS PROCESSES WITH HEAVY QUARK SIGNATURES IN THE ATLAS EXPERIMENT by AARON TAYLOR B.A., Mathematics, University of California, Santa Cruz, 2011 M.S., Physics, University of New Mexico, 2014 DISSERTATION Submitted in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy Physics The University of New Mexico Albuquerque, New Mexico May, 2017 ©2017, Aaron Taylor iii Acknowledgements I would like to thank Professor Sally Seidel, for her constant support and guidance in my research. I would also like to thank her for her patience in helping me to develop my technical writing and presentation skills; without her assistance, I would never have gained the skill I have in that field. I would like to thank Konstantin Toms, for his constant assistance with the ATLAS code, and for generally giving advice on how to handle data analysis. The Bs → 4μ analysis likely wouldn’t have gotten anywhere without him. I would like to deeply thank Pavel Reznicek, without whom I would never have gotten as great an understanding of ATLAS code as I currently have. It is no exaggeration to say that I would not have been half as successful as I have been without his constant patience and understanding. Thank you. Many thanks to Martin Hoeferkamp, who taught me much about instrumentation and physical measurements.
    [Show full text]
  • Slides Lecture 1
    Advanced Topics in Particle Physics Probing the High Energy Frontier at the LHC Ulrich Husemann, Klaus Reygers, Ulrich Uwer University of Heidelberg Winter Semester 2009/2010 CERN = European Laboratory for Partice Physics the world’s largest particle physics laboratory, founded 1954 Historic name: “Conseil Européen pour la Recherche Nucléaire” Lake Geneva Proton-proton2500 employees, collider almost 10000 guest scientists from 85 nations Jura Mountains 8.5 km Accelerator complex Prévessin site (approx. 100 m underground) (France) Meyrin site (Switzerland) Probing the High Energy Frontier at the LHC, U Heidelberg, Winter Semester 09/10, Lecture 1 2 Large Hadron Collider: CMS Experiment: Proton-Proton and Multi Purpose Detector Lead-Lead Collisions LHCb Experiment: B Physics and CP Violation ALICE-Experiment: ATLAS Experiment: Heavy Ion Physics Multi Purpose Detector Probing the High Energy Frontier at the LHC, U Heidelberg, Winter Semester 09/10, Lecture 1 3 The Lecture “Probing the High Energy Frontier at the LHC” Large Hadron Collider (LHC) at CERN: premier address in experimental particle physics for the next 10+ years LHC restart this fall: first beam scheduled for mid-November LHC and Heidelberg Experimental groups from Heidelberg participate in three out of four large LHC experiments (ALICE, ATLAS, LHCb) Theory groups working on LHC physics → Cornerstone of physics research in Heidelberg → Lots of exciting opportunities for young people Probing the High Energy Frontier at the LHC, U Heidelberg, Winter Semester 09/10, Lecture 1 4 Scope
    [Show full text]
  • Arxiv:2001.07837V2 [Hep-Ex] 4 Jul 2020 Scale Funding Will Be Requested at Different Stages Across the Globe
    Brazilian Participation in the Next-Generation Collider Experiments W. L. Aldá Júniora C. A. Bernardesb D. De Jesus Damiãoa M. Donadellic D. E. Martinsd G. Gil da Silveirae;a C. Henself H. Malbouissona A. Massafferrif E. M. da Costaa C. Mora Herreraa I. Nastevad M. Rangeld P. Rebello Telesa T. R. F. P. Tomeib A. Vilela Pereiraa aDepartamento de Física Nuclear e Altas Energias, Universidade do Estado do Rio de Janeiro (UERJ), Rua São Francisco Xavier, 524, CEP 20550-900, Rio de Janeiro, Brazil bUniversidade Estadual Paulista (Unesp), Núcleo de Computação Científica Rua Dr. Bento Teobaldo Ferraz, 271, 01140-070, Sao Paulo, Brazil cInstituto de Física, Universidade de São Paulo (USP), Rua do Matão, 1371, CEP 05508-090, São Paulo, Brazil dUniversidade Federal do Rio de Janeiro (UFRJ), Instituto de Física, Caixa Postal 68528, 21941-972 Rio de Janeiro, Brazil eInstituto de Física, Universidade Federal do Rio Grande do Sul , Av. Bento Gonçalves, 9550, CEP 91501-970, Caixa Postal 15051, Porto Alegre, Brazil f Centro Brasileiro de Pesquisas Físicas (CBPF), Rua Dr. Xavier Sigaud, 150, CEP 22290-180 Rio de Janeiro, RJ, Brazil E-mail: [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected], [email protected] Abstract: This proposal concerns the participation of the Brazilian High-Energy Physics community in the next-generation collider experiments.
    [Show full text]
  • Arxiv:2003.07868V3 [Hep-Ph] 21 Jul 2020 Ejmnc Allanach, C
    CERN-LPCC-2020-001, FERMILAB-FN-1098-CMS-T, Imperial/HEP/2020/RIF/01 Reinterpretation of LHC Results for New Physics: Status and Recommendations after Run 2 We report on the status of efforts to improve the reinterpretation of searches and mea- surements at the LHC in terms of models for new physics, in the context of the LHC Reinterpretation Forum. We detail current experimental offerings in direct searches for new particles, measurements, technical implementations and Open Data, and provide a set of recommendations for further improving the presentation of LHC results in order to better enable reinterpretation in the future. We also provide a brief description of existing software reinterpretation frameworks and recent global analyses of new physics that make use of the current data. Waleed Abdallah,1, 2 Shehu AbdusSalam,3 Azar Ahmadov,4 Amine Ahriche,5, 6 Gaël Alguero,7 Benjamin C. Allanach,8, ∗ Jack Y. Araz,9 Alexandre Arbey,10, 11 Chiara Arina,12 Peter Athron,13 Emanuele Bagnaschi,14 Yang Bai,15 Michael J. Baker,16 Csaba Balazs,13 Daniele Barducci,17, 18 Philip Bechtle,19, ∗ Aoife Bharucha,20 Andy Buckley,21, † Jonathan Butterworth,22, ∗ Haiying Cai,23 Claudio Campagnari,24 Cari Cesarotti,25 Marcin Chrzaszcz,26 Andrea Coccaro,27 Eric Conte,28, 29 Jonathan M. Cornell,30 Louie D. Corpe,22 Matthias Danninger,31 Luc Darmé,32 Aldo Deandrea,10 Nishita Desai,33, ∗ Barry Dillon,34 Caterina Doglioni,35 Matthew J. Dolan,16 Juhi Dutta,1, 36 John R. Ellis,37 Sebastian Ellis,38 Farida Fassi,39 Matthew Feickert,40 Nicolas Fernandez,40 Sylvain Fichet,41 Thomas Flacke,42 Benjamin Fuks,43, 44, ∗ Achim Geiser,45 Marie-Hélène Genest,7 Akshay Ghalsasi,46 Tomas Gonzalo,13 Mark Goodsell,43 Stefania Gori,46 Philippe Gras,47 Admir Greljo,11 Diego Guadagnoli,48 Sven Heinemeyer,49, 50, 51 Lukas A.
    [Show full text]
  • MIT at the Large Hadron Collider—Illuminating the High-Energy Frontier
    Mit at the large hadron collider—Illuminating the high-energy frontier 40 ) roland | klute mit physics annual 2010 gunther roland and Markus Klute ver the last few decades, teams of physicists and engineers O all over the globe have worked on the components for one of the most complex machines ever built: the Large Hadron Collider (LHC) at the CERN laboratory in Geneva, Switzerland. Collaborations of thousands of scientists have assembled the giant particle detectors used to examine collisions of protons and nuclei at energies never before achieved in a labo- ratory. After initial tests proved successful in late 2009, the LHC physics program was launched in March 2010. Now the race is on to fulfill the LHC’s paradoxical mission: to complete the Stan- dard Model of particle physics by detecting its last missing piece, the Higgs boson, and to discover the building blocks of a more complete theory of nature to finally replace the Standard Model. The MIT team working on the Compact Muon Solenoid (CMS) experiment at the LHC stands at the forefront of this new era of particle and nuclear physics. The High Energy Frontier Our current understanding of the fundamental interactions of nature is encap- sulated in the Standard Model of particle physics. In this theory, the multitude of subatomic particles is explained in terms of just two kinds of basic building blocks: quarks, which form protons and neutrons, and leptons, including the electron and its heavier cousins. From the three basic interactions described by the Standard Model—the strong, electroweak and gravitational forces—arise much of our understanding of the world around us, from the formation of matter in the early universe, to the energy production in the Sun, and the stability of atoms and mit physics annual 2010 roland | klute ( 41 figure 1 A photograph of the interior, central molecules.
    [Show full text]
  • What Is Next for the Lhc?
    Building new technologies Fuelling industry Particle accelerators, like those at the heart of the and economy LHC, are now being adopted for cancer therapies using WHAT IS NEXT protons which, unlike current therapies, deposit all their energy in the same place, making them ideal for treating FOR THE LHC? STFC funds the UK membership to CERN, which gives tumours near to delicate organs. UK scientists and engineers access to the vast amount of data and research that takes place. New technology and systems are still being developed around the LHC, allowing us to ask new questions and Since the LHC became operational, UK industry make exciting discoveries and progress in a range of has won valuable contracts at CERN worth different fields. £102 million (2010-2015). Of these, £15 million were awarded in 2015. Inspiring the next generation Engineering success This exciting science is prompting more young people to consider careers in physics and engineering, fields that Many engineering disciplines were involved in the are highly prized throughout the UK economy (during design, construction and maintenance of the LHC. the academic year that the Higgs boson was discovered, More than 1,600 superconducting magnets were British universities received 2,000 more applications for installed, with most weighing in excess of 27 tonnes, physics degrees than in previous years). in a collaborative effort involving more than 10,000 scientists and engineers from over 100 countries. CERN provides opportunities for both apprentices and graduates to visit and work at the site, so more Universities across the UK helped build the highly young people have the chance to build the career that sensitive detectors at the heart of the LHC’s they want.
    [Show full text]
  • First Results from ATLAS Experiment on Production of W and Z Bosons In
    1 First results from ATLAS experiment on production of W 2 Z s = 7 and bosons in proton-proton collisions at √ TeV ∗ † 3 PawelMalecki 4 Henryk Niewodniczanski Inst. of Nucl. Physics, PAN, Cracow, Poland 5 First results for the W and Z boson production cross-sections at √s = 6 7 TeV obtained with the ATLAS detector are presented. The measure- 7 ments are performed in electron and muon channels, with a data sample of −1 8 around 320 nb collected between March and July 2010. Methods of signal 9 extraction and background estimation are briefly presented. The measured 10 values of W production cross-sections in electron and muon channels are 11 σW BR(W eν)=10.51 1.45 nb and σW BR(W µν)=9.58 × → ± × → ± 12 1.20 nb. The Z cross-section measurements yield σZ BR(Z ee) = × → 13 0.75 0.14 nb and σZ BR(Z µµ)=0.87 0.14 nb. The obtained 14 results± are in good agreement× with→ theoretical predictions.± A preliminary 15 measurement of the W boson charge asymmetry is also presented. 16 1. Introduction 17 A very important point in the ATLAS program of first physics measure- 18 ments is the observation of W and Z bosons and their properties. The- 19 oretical predictions for W/Z production cross-sections are nowadays very 20 precise [1], so a fine measurement is needed to test these predictions, which 21 are sensitive to higher-order (NNLO) QCD corrections as well as Parton Dis- 22 tribution Functions (P DF ) of the proton [2].
    [Show full text]
  • The ATLAS Experiment at the CERN Large Hadron Collider
    The ATLAS Experiment at the CERN Large Hadron Collider A 30 minute tour Peter Krieger University of Toronto P.Krieger, University of Toronto WNPPC'08, Banff, February 2008 0 The Standard Model of Particle Physics SU(3)C SU(2)L U(1)Y e μ Consistent with all existing experimental data BUT e L μ L L No Higgs yet u c t 19 free parameters (masses, couplings etc) three (?) generations of fundamental fermions d s b L L L Hierarchy problem (need Supersymmetry) Charge ratios of quarks and leptons (GUTs) No gravity (need string theory ?) ± 0 0 W ,Z Higgs H A Number candidates for physics beyond the SM g Expected mass scale for new physics ~ 1 TeV P.Krieger, University of Toronto WNPPC'08, Banff, February 2008 1 Beyond the Standard Model Hierarchy problem: there are two fundamental energy scales that we know -17 of: the electroweak scale and the Planck scale: MEW / Mplanck 10 Naturalness problem: radiative corrections to the mass of a fundamental scalar (e.g. the Higgs) scale like 2 where is the energy scale to which the theory remains valid. This yields a fine-tuning problem for the Higgs mass unless: Could be gravity if there a) There is new physics at the ~ TeV energy scale are extra dimensions b) There is some symmetry protecting the Higgs mass against large radiative corrections (Supersymmetry) If the Higgs is not discovered with a mass < 800 GeV, expect the dynamics of WW, ZZ scattering to reveal new physics at this energy scale We MUST see something at LHC energies P.Krieger, University of Toronto WNPPC'08, Banff, February 2008 2 Vector Boson Scattering 2 Cross-section grows with s E CM .
    [Show full text]
  • Super Symmetry
    MILESTONES DOI: 10.1038/nphys868 M iles Tone 1 3 Super symmetry The way that spin is woven into the in 1015. However, a form of symmetry very fabric of the Universe is writ between fermions and bosons called large in the standard model of supersymmetry offers a much more particle physics. In this model, which elegant solution because the took shape in the 1970s and can quantum fluctuations caused by explain the results of all particle- bosons are naturally cancelled physics experiments to date, matter out by those caused by fermions and (and antimatter) is made of three vice versa. families of quarks and leptons, which Symmetry plays a central role in are all fermions, whereas the physics. The fact that the laws of electromagnetic, strong physics are, for instance, symmetric in and weak forces that act on these time (that is, they do not change with particles are carried by other time) leads to the conservation of particles, such as photons and gluons, energy. These laws are also symmetric The ATLAS experiment under construction at the which are all bosons. with respect to space, rotation and Large Hadron Collider. Image courtesy of CERN. Despite its success, the standard relative motion. Initially explored in model is unsatisfactory for a number the early 1970s, supersymmetry is a of reasons. First, although the less obvious kind of symmetry, which, graviton. Searching for electromagnetic and weak forces if it exists in nature, would mean that supersymmetric particles will be a have been unified into a single force, the laws of physics do not change priority when the Large Hadron a ‘grand unified theory’ that brings when bosons are replaced by Collider comes into operation at the strong interaction into the fold fermions, and fermions are replaced CERN, the European particle-physics remains elusive.
    [Show full text]
  • Top Quark and Heavy Vector Boson Associated Production at the Atlas Experiment
    ! "#$ "%&'" (' ! ) #& *+ & , & -. / . , &0 , . &( 1, 23)!&4 . . . & & 56 & , "#7 #'6 . & #'6 & . , & . .3(& ( & 8 !10 92&4 . ) *)+ . : ./ *)#+ . *) +& . , & "#$ :;; &&;< = : ::: #>$ ? 4@!%$5%#$?>%'>'> 4@!%$5%#$?>%'>># ! #"?%# TOP QUARK AND HEAVY VECTOR BOSON ASSOCIATED PRODUCTION AT THE ATLAS EXPERIMENT Olga Bessidskaia Bylund Top quark and heavy vector boson associated production at the ATLAS experiment Modelling, measurements and effective field theory Olga Bessidskaia Bylund ©Olga Bessidskaia Bylund, Stockholm University 2017 ISBN print 978-91-7649-343-4 ISBN PDF 978-91-7649-344-1 Printed in Sweden by Universitetsservice US-AB, Stockholm 2017 Distributor: Department of Physics, Stockholm University Cover image by Henrik Åkerstedt Contents 1 Preface 5 1.1 Introduction ............................ 5 1.2Structureofthethesis...................... 5 1.3 Contributions of the author . ................. 6 2 Theory 8 2.1TheStandardModelandQuantumFieldTheory....... 8 2.1.1 Particle content of the Standard Model ........ 8 2.1.2 S-matrix expansion .................... 11 2.1.3 Cross sections ....................... 13 2.1.4 Renormalisability and gauge invariance ........ 15 2.1.5 Structure of the Lagrangian ............... 16 2.1.6 QED ...........................
    [Show full text]
  • Historical Milestones for the ATLAS Experiment
    Symposium 25 Years of LHC Experimental Programme CERN, 15th December 2017 Historical Milestones for Peter Jenni, CERN and the ATLAS Experiment Albert-Ludwigs-Universität Freiburg The plan is to comment a bit on: - History of the LHC experiment studies in general - Some early milestones leading to ATLAS as it is now - Some milestones of the ATLAS construction (pictures…) - Costs and funding, growth of the Collaboration - Note: Physics will be covered by Valerio Dao - And in all cases, these are only examples Drawing by Sergio Cittolin After the 1979 LEP White Book (ECFA-LEP WG chaired by A Zichichi) which mentioned the possibility of a far future LHC, and discoveries of the W and Z bosons by UA1 and UA2 in the early 1980s … 1984 For the community it all started with the CERN - ECFA Workshop in Lausanne on the feasibility of a hadron collider in the future LEP tunnel 1986 LAA R&D on new detector technologies started, later followed by the DRDC 1987 La Thuile Workshop Many LHC colleagues were already involved in this WS set up by Carlo Rubbia as part of the Long Range Planning Committee 25y LHC Exp. Prog. 15-12-2017 ATLAS History 3 Peter Jenni (CERN and Freiburg) Arguing after the mid-1980s of being ambitious and design a general purpose detector … 25y LHC Exp. Prog. 15-12-2017 ATLAS History 4 Peter Jenni (CERN and Freiburg) From an early talk about the LHC, must have been around 1986/7 … 25y LHC Exp. Prog. 15-12-2017 ATLAS History 5 Peter Jenni (CERN and Freiburg) 1989 ECFA Study Week in Barcelona for LHC instrumentation (forming of first proto-Collaboration) 1990 Large Hadron Collider Workshop Aachen (CERN - ECFA) 1992 CERN – ECFA meeting ‘Towards the LHC Experimental Programme’ in Evian 25y LHC Exp.
    [Show full text]