James Beacham
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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. -
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. -
Observation of Structure in the J/Ψ-Pair Mass Spectrum
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH (CERN) CERN-EP-2020-115 LHCb-PAPER-2020-011 November 10, 2020 Observation of structure in the J= -pair mass spectrum LHCb collaboration† Abstract p Using proton-proton collision data at centre-of-mass energies of s = 7, 8 and 13 TeV recorded by the LHCb experiment at the Large Hadron Collider, corresponding to an integrated luminosity of 9 fb−1, the invariant mass spectrum of J= pairs is studied. A narrow structure around 6:9 GeV/c2 matching the lineshape of a resonance and a broad structure just above twice the J= mass are observed. The deviation of the data from nonresonant J= -pair production is above five standard deviations in the mass region between 6:2 and 7:4 GeV/c2, covering predicted masses of states composed of four charm quarks. The mass and natural width of the narrow X(6900) structure are measured assuming a Breit{Wigner lineshape. arXiv:2006.16957v2 [hep-ex] 10 Nov 2020 Keywords: QCD; exotics; tetraquark; spectroscopy; quarkonium; particle and resonance production Published in Science Bulletin 2020 65(23)1983-1993 © 2020 CERN for the benefit of the LHCb collaboration. CC BY 4.0 licence. †Authors are listed at the end of this paper. ii 1 Introduction The strong interaction is one of the fundamental forces of nature and it governs the dynamics of quarks and gluons. According to quantum chromodynamics (QCD), the theory describing the strong interaction, quarks are confined into hadrons, in agreement with experimental observations. The quark model [1,2] classifies hadrons into conventional mesons (qq) and baryons (qqq or qqq), and also allows for the existence of exotic hadrons such as tetraquarks (qqqq) and pentaquarks (qqqqq). -
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 -
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. -
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. -
Department of High Energy Physics: Overview
DEPARTMENT OF HIGH ENERGY PHYSICS 93 6 DEPARTMENT OF HIGH ENERGY PHYSICS PLO401707 Head of Department: Assoc. Professor Helena Balkowska phone: (22) 621-28-04 e-mail: Lena.Bialkowskafuw.edu.pl Overview The activities of the Department f Hgh Energy Physics are centered around experiments performed at accelerators in the following laboratories: • At CERN, the European Laboratory for Particle Physics in Geneva, Switzerland: DELPHI* at LEP ee- stora(Te rina - the tests of the Standard Model, b-quark physics, gamina-gami-na interactions and search for Higgs boson and supersymmetric particles - NA48 - the CP-violation and are K decays - COMPASS (Compact Muon and Proton Apparatus for Structure and Spectroscopy) - studies the gluon polarization in the nucleon - NA49* and WA98 - heavy ion physics, looking for possible effects of the phase transition to te quark- - gluon plasma state • At CELSIUS Storage Ring in Uppsala, Sweden: - WASA - a precise study of near threshold resonance poduction. • At RHIC - study of pp elastic scatterin.g. • At DESY in Hamburg, Germany: - ZEUS - deep inelastic scattering f elections and protons, proton structure functions, dffractive poton- proton interactions. • Super-Karniokande and K2K - a study of neutrino oscillations. The Groups fi-om our Department participated in the construction phase of te experiments, both in hardware and in development of the software used in data analysis. Presently they take part in te data collection, detector performance supervision and data analysis. The Department is also involved -
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. -
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. -
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]. -
Photon Detectors for the Ring Imaging Cherenkov Counters of the Lhcb Experiment
Photon Detectors for the Ring Imaging Cherenkov Counters of the LHCb Experiment Richard W. R. Plackett Imperial College, London A thesis submitted for the degree of Doctor of Philosophy in the University of London July 2006 c R. Plackett 2006 ABSTRACT This thesis reports on the author’s contribution to the development of the Ring Imaging Cherenkov(RICH) detectors in the LHCb experiment due to take data at the CERN Large Hadron Collider in 2007. The first chapter summarises the physics to be explored by the LHCb experiment; measurements of CP violating asymmetries and a study of rare B decay modes. A brief overview of other experiments studying B-physics is presented. The experiment itself is then described, focussing on the RICH system used for particle identification, with particular emphasis on the photon detectors. The thesis then reports on the work done by the author on the design of the RICH1 Magnetic Shield, that allows the photon detectors to operate in the fringe field of the LHCb dipole magnet, while fulfilling the conflicting requirement to provide additional magnetic bending power to aid the LHCb charged particle trigger. The design of all of the many sections of the shield are described in depth and the results of finite element simulations performed by the author are reported. The results of measurements the author took of the field produced by the completed magnetic shield are then evaluated and compared with the simulation. Next follows a study undertaken by the author on the electronic readout of the RICH Hybrid Photon Detectors (HPD). Two related mesurments were made, a novel series of timing tests on the HPD’s analogue readout in an assembled tube and a series of experiments using a pulsed laser to simulate the charge deposition of a photoelectron. -
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 .