Measurement of Violation in the Decay → ∓ with Data
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The Moedal Experiment at the LHC. Searching Beyond the Standard
126 EPJ Web of Conferences , 02024 (2016) DOI: 10.1051/epjconf/201612602024 ICNFP 2015 The MoEDAL experiment at the LHC Searching beyond the standard model James L. Pinfold (for the MoEDAL Collaboration)1,a 1 University of Alberta, Physics Department, Edmonton, Alberta T6G 0V1, Canada Abstract. MoEDAL is a pioneering experiment designed to search for highly ionizing avatars of new physics such as magnetic monopoles or massive (pseudo-)stable charged particles. Its groundbreaking physics program defines a number of scenarios that yield potentially revolutionary insights into such foundational questions as: are there extra dimensions or new symmetries; what is the mechanism for the generation of mass; does magnetic charge exist; what is the nature of dark matter; and, how did the big-bang develop. MoEDAL’s purpose is to meet such far-reaching challenges at the frontier of the field. The innovative MoEDAL detector employs unconventional methodologies tuned to the prospect of discovery physics. The largely passive MoEDAL detector, deployed at Point 8 on the LHC ring, has a dual nature. First, it acts like a giant camera, comprised of nuclear track detectors - analyzed offline by ultra fast scanning microscopes - sensitive only to new physics. Second, it is uniquely able to trap the particle messengers of physics beyond the Standard Model for further study. MoEDAL’s radiation environment is monitored by a state-of-the-art real-time TimePix pixel detector array. A new MoEDAL sub-detector to extend MoEDAL’s reach to millicharged, minimally ionizing, particles (MMIPs) is under study Finally we shall describe the next step for MoEDAL called Cosmic MoEDAL, where we define a very large high altitude array to take the search for highly ionizing avatars of new physics to higher masses that are available from the cosmos. -
EPS-HEP 2017 Report of Contributions
EPS-HEP 2017 Report of Contributions https://indico.cern.ch/e/epshep2017 EPS-HEP 2017 / Report of Contributions Theory overview on FCNC B-decays Contribution ID: 10 Type: Parallel Talk Theory overview on FCNC B-decays Thursday, 6 July 2017 09:00 (30 minutes) LHCb experiment at CERN has recently reported a set of measurements on lepton flavour univer- sality in b to s transitions showing a departure from the Standard Model predictions. I will review the main ideas recently put forward to make sense out of these intriguing hints. Focusing on the new physics explanation, I will discuss the correlated signals expected in other low- and high- energy observables, that could help clarify the mysterious signal. Experimental Collaboration Primary author: GRELJO, Admir (University of Zurich) Presenter: GRELJO, Admir (University of Zurich) Session Classification: Flavour and symmetries Track Classification: Flavour Physics and Fundamental Symmetries October 6, 2021 Page 1 EPS-HEP 2017 / Report of Contributions Charm Quark Mass with Calibrate … Contribution ID: 11 Type: Parallel Talk Charm Quark Mass with Calibrated Uncertainty Friday, 7 July 2017 12:35 (13 minutes) We determine the charm quark mass mc(mc) from QCD sum rules of moments of the vector cur- rent correlator calculated in perturbative QCD. Only experimental data for the charm resonances below the continuum threshold are needed in our approach, while the continuum contribution is determined by requiring self-consistency between various sum rules, including the one for the ze- roth moment. Existing data from the continuum region can then be used to bound the theoretical error. Our result is mc(mc) = 1272 ± 8 MeV for αs(MZ ) = 0:1182. -
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 -
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 -
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.) 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. -
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. -
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. -
Arxiv:1405.7662V4 [Hep-Ph] 28 Aug 2014
THE PHYSICS PROGRAMME OF THE MoEDAL EXPERIMENT AT THE LHC B. ACHARYA1;2; J. ALEXANDRE1, J. BERNABEU´ 3, M. CAMPBELL4, S. CECCHINI5, J. CHWASTOWSKI6, M. DE MONTIGNY7, D. DERENDARZ6, A. DE ROECK4, J. R. ELLIS1;4, M. FAIRBAIRN1, D. FELEA8, M. FRANK9, D. FREKERS10, C. GARCIA3, G. GIACOMELLI5;5ay, J. JAKUBEK˚ 11, A. KATRE12, D-W KIM13, M.G.L. KING3, K. KINOSHITA14, D. LACARRERE4, S. C. LEE11, C. LEROY15, A. MARGIOTTA5, N. MAURI5;5a, N. E. MAVROMATOS1;4, P. MERMOD12, V. A. MITSOU3, R. ORAVA16, L. PASQUALINI5;5a, L. PATRIZII5, G. E. PAV˘ ALAS¸˘ 8, J. L. PINFOLD7∗, M. PLATKEVICˇ 11, V. POPA8, M. POZZATO5, S. POSPISIL11, A. RAJANTIE17, Z. SAHNOUN5;5b, M. SAKELLARIADOU1, S. SARKAR1, G. SEMENOFF18, G. SIRRI5, K. SLIWA19, R. SOLUK7, M. SPURIO5;5a, Y.N. SRIVASTAVA20, R. STASZEWSKI6, J. SWAIN20, M. TENTI5;5a, V. TOGO5, M. TRZEBINSKI6, J. A. TUSZYNSKI´ 7, V. VENTO3, O. VIVES3, Z. VYKYDAL11, and A. WIDOM20, J. H. YOON21. (for the MoEDAL Collaboration) 1Theoretical Particle Physics and Cosmology Group, Physics Department, King's College London, UK 2International Centre for Theoretical Physics, Trieste, Italy 3IFIC, Universitat de Val`encia- CSIC, Valencia, Spain 4Physics Department, CERN, Geneva, Switzerland 5 INFN, Section of Bologna, 40127, Bologna , Italy 5a Department of Physics & Astronomy, University of Bologna, Italy 5b Centre on Astronomy, Astrophysics and Geophysics, Algiers, Algeria 6 Institute of Nuclear Physics Polish Academy of Sciences, Cracow, Poland 7Physics Department, University of Alberta, Edmonton Alberta, Canada 8Institute of Space -
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. -
Study and Design of the Readout Unit Module for the Lhcb Experiment CERN-THESIS-2002-036 31/12/2001 José Francisco Toledo Alarcón
Study and Design of the Readout Unit Module for the LHCb Experiment CERN-THESIS-2002-036 31/12/2001 José Francisco Toledo Alarcón Under the direction of Dr. Francisco José Mora Más Doctoral Thesis Electronics Engineering Department Universidad Politécnica de Valencia, 2001 To Hans, with gratitude. I couldn’t have got this far without your experience, support and leading. i List of acronyms xi Preface 1 Introduction 1 Objectives 2 Thesis structure 4 Contributions by other engineers and physicists 6 CHAPTER 1 Data acquisition in high-energy physics experiments 9 Particle accelerators 9 Particle detectors 11 Particle detector readout 12 Evolution of DAQ systems 13 Instrumentation buses for HEP in the 60’s and in the 70’s 14 DAQ and trigger systems in the 80’s 16 New trends in the 90’s 18 Trends in DAQ systems for the 21st century 20 The PCI Flexible I/O Card (PCI-FLIC) 22 Conclusions 24 CHAPTER 2 DAQ and Trigger systems in LHCb 27 The LHCb experiment at CERN 27 LHC: A new accelerator for new physics 27 A Large Hadron Collider Beauty Experiment (LHCb) 28 Front-end electronics overview 30 LHCb trigger and DAQ architecture 31 Trigger system 32 Data Acquisition (DAQ) system 34 Flow control in LHCb 35 CHAPTER 3 The Readout Unit for the LHCb experiment 39 Target applications in the LHCb experiment 39 The Readout Unit as input stage to the LHCb DAQ system 40 The Readout Unit as Front-end Multiplexer for the Level-1 Electronics 43 The Readout Unit as readout module for the Level-1 Vertex Locator Trigger 45 Design criteria and parameters 47 DAQ Readout -
Lhcb Results on Penta(Tetra)-Quark Search
LHCb results on penta(tetra)-quark search Marcin Kucharczyk1 (on behalf of the LHCb collaboration) 1Henryk Niewodniczanski Institute of Nuclear Physics PAN, Krakow, Poland E-mail: [email protected] (Received October 17, 2016) The LHCb experiment is designed to study the properties and decays of heavy flavored hadrons produced in pp collisions at the LHC. The data collected in the LHC Run I enables precision spec- troscopy studies of beauty and charm hadrons. The latest results on spectroscopy of conventional and exotic hadrons are reviewed, such as the discovery of the first charmonium pentaquark states in the J/ψp system or the confirmation of resonant nature of the Z(4430)− mesonic state. LHCb has also made significant contributions to determination of the quantum numbers for the X(3872) state and to exclude the existence of the X(5568) tetraquark candidate. The LHCb results described in the present document have dramatically increased the interest on spectroscopy of heavy hadrons. KEYWORDS: pentaquarks, heavy flavor spectroscopy, exotic states 1. Introduction In the simple quark model, only two types of quark combinations are required to account for the existing hadrons, i.e. qq¯ combinations form mesons, while baryons are made up of three quarks. How- ever, in the quark model proposed by Gell-Mann and Zweig in 1960s [1] other SU(3) color-neutral combinations of quarks and gluons such as gg glueballs, qqg¯ hybrids, qqq¯ q¯ tetraquarks,qqqqq ¯ pen- taquarks etc. were predicted. The world’s largest data sample of beauty and charm hadrons collected by LHCb during LHC Run I provides great opportunities for studying the production and properties of heavy hadrons.