Intermediate Vector Bosons Production and Identification at the CERN Proton-Antiproton Collider G
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PRODUCTION of HIGH MASS Cv and E'e' PAIRS in the UA2
142 PRODUCTION OF HIGH MASS cv AND e'e' PAIRS IN THE UA2 EXPERIMENT AT THE CERN pp COLLIDER The UA2 Collaboration (Berne, CERN, CopenhagenT Orsay;" Pavía, Sacïay) Dî 84100S6163 presented by J. SCHACHER University of Berne, Switzerland ABSTRACT We present new results on intermediate vector boson production at the CERN pp collider. A comparison is made with the predictions of the standard model of the unified electroweak Glashow-Salam-Weinberg theory. - 143 - 1, INTRODUCTION We report here the results from a search for electrons with > 15 GeV/c produced at the CERN pp collider (Vs = 540 GeV) during its 1982 and 1983 periods of operation. Following a general discussion of the topology of the events containing an electron candidate, we shall compare the data with expectations in the framework of the electroweak standard model [1] for the reactions p + p - W~ + anything (1) - e" • v (?) p • p - Z° + anything (2) -* e* + e" or e* + e" + y where W~ and Z° are the postulated charged and neutral Intermediate Vector Bosonc (IVB), respectively, According to the amount of data collected we are now in the position to study some details of the IVB production, e.g. the influence of emission of gluon radiation on the distribution of the W transverse momentum (Fig.1). Fig.l Typical diagram for W and Z production, taking into account emission of gluon (g) radiation. 7T : parton in p or p. - 144 - Preliminary results from the study reported here have already been presented elsewhere [2] and a more complete discussion can be found in a recent publication [3]. -
Triple Vector Boson Production at the LHC
Triple Vector Boson Production at the LHC Dan Green Fermilab - CMS Dept. ([email protected]) Introduction The measurement of the interaction among vector bosons is crucial to understanding electroweak symmetry breaking. Indeed, data from LEP-II have already determined triple vector boson couplings and a first measurement of quartic couplings has been made [1]. It is important to explore what additional information can be supplied by future LHC experiments. One technique is to use “tag” jets to identify vector boson fusion processes leading to two vector bosons and two tag jets in the final state. [2] However, the necessity of two quarks simultaneously radiating a W boson means that the cross section is rather small. Another approach is to study the production of three vector bosons in the final state which are produced by the Drell- Yan mechanism. There is a clear tradeoff, in that valence-valence processes are not allowed, which limits the mass range which can be explored using this mechanism, although the cross sections are substantially larger than those for vector boson fusion. Triple Vector Boson Production A Z boson decaying into lepton pairs is required in the final state in order to allow for easy triggering at the LHC and to insure a clean sample of Z plus four jets. Possible final states are ZWW, ZWZ and ZZZ. Assuming that the second and third bosons are reconstructed from their decay into quark pairs, the W and Z will not be easily resolved given the achievable dijet mass resolution. Therefore, the final states of interest contain a Z which decays into leptons and four jets arising for the quark decays of the other two vector bosons. -
Fabiola Gianotti
Fabiola Gianotti Date of Birth 29 October 1960 Place Rome, Italy Nomination 18 August 2020 Field Physics Title Director-General of the European Laboratory for Particle Physics, CERN, Geneva Most important awards, prizes and academies Honorary Professor, University of Edinburgh; Corresponding or foreign associate member of the Italian Academy of Sciences (Lincei), the National Academy of Sciences of the United States, the French Academy of Sciences, the Royal Society London, the Royal Academy of Sciences and Arts of Barcelona, the Royal Irish Academy and the Russian Academy of Sciences. Honorary doctoral degrees from: University of Uppsala (2012); Ecole Polytechnique Federale de Lausanne (2013); McGill University, Montreal (2014); University of Oslo (2014); University of Edinburgh (2015); University of Roma Tor Vergata (2017); University of Chicago (2018); University Federico II, Naples (2018); Université de Paris Sud, Orsay (2018); Université Savoie Mont Blanc, Annecy (2018); Weizmann Institute, Israel (2018); Imperial College, London (2019). National honours: Cavaliere di Gran Croce dell'Ordine al Merito della Repubblica, awarded by the Italian President Giorgio Napolitano (2014). Special Breakthrough Prize in Fundamental Physics (shared, 2013); Enrico Fermi Prize of the Italian Physical Society (shared, 2013); Medal of Honour of the Niels Bohr Institute, Copenhagen (2013); Wilhelm Exner Medal, Vienna (2017); Tate Medal of the American Institute of Physics for International Leadership (2019). Summary of scientific research Fabiola Gianotti is a particle physicist working at high-energy accelerators. In her scientific career, she has made significant contributions to several experiments at CERN, including UA2 at the proton-antiproton collider (SpbarpS), ALEPH at the Large Electron-Positron collider (LEP) and ATLAS at the Large Hadron Collider (LHC). -
Vector Boson Scattering Processes: Status and Prospects
Vector Boson Scattering Processes: Status and Prospects Diogo Buarque Franzosi (ed.)g,d, Michele Gallinaro (ed.)h, Richard Ruiz (ed.)i, Thea K. Aarrestadc, Mauro Chiesao, Antonio Costantinik, Ansgar Dennert, Stefan Dittmaierf, Flavia Cetorellil, Robert Frankent, Pietro Govonil, Tao Hanp, Ashutosh V. Kotwala, Jinmian Lir, Kristin Lohwasserq, Kenneth Longc, Yang Map, Luca Mantanik, Matteo Marchegianie, Mathieu Pellenf, Giovanni Pellicciolit, Karolos Potamianosn,Jurgen¨ Reuterb, Timo Schmidtt, Christopher Schwanm, Michał Szlepers, Rob Verheyenj, Keping Xiep, Rao Zhangr aDepartment of Physics, Duke University, Durham, NC 27708, USA bDeutsches Elektronen-Synchrotron (DESY) Theory Group, Notkestr. 85, D-22607 Hamburg, Germany cEuropean Organization for Nuclear Research (CERN) CH-1211 Geneva 23, Switzerland dDepartment of Physics, Chalmers University of Technology, Fysikgården 1, 41296 G¨oteborg, Sweden eSwiss Federal Institute of Technology (ETH) Z¨urich, Otto-Stern-Weg 5, 8093 Z¨urich, Switzerland fUniversit¨atFreiburg, Physikalisches Institut, Hermann-Herder-Straße 3, 79104 Freiburg, Germany gPhysics Department, University of Gothenburg, 41296 G¨oteborg, Sweden hLaborat´oriode Instrumenta¸c˜aoe F´ısicaExperimental de Part´ıculas(LIP), Lisbon, Av. Prof. Gama Pinto, 2 - 1649-003, Lisboa, Portugal iInstitute of Nuclear Physics, Polish Academy of Sciences, ul. Radzikowskiego, Cracow 31-342, Poland jUniversity College London, Gower St, Bloomsbury, London WC1E 6BT, United Kingdom kCentre for Cosmology, Particle Physics and Phenomenology (CP3), Universit´eCatholique de Louvain, Chemin du Cyclotron, B-1348 Louvain la Neuve, Belgium lMilano - Bicocca University and INFN, Piazza della Scienza 3, Milano, Italy mTif Lab, Dipartimento di Fisica, Universit`adi Milano and INFN, Sezione di Milano, Via Celoria 16, 20133 Milano, Italy nDepartment of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, UK oDipartimento di Fisica, Universit`adi Pavia, Via A. -
Basic Ideas of the Standard Model
BASIC IDEAS OF THE STANDARD MODEL V.I. ZAKHAROV Randall Laboratory of Physics University of Michigan, Ann Arbor, Michigan 48109, USA Abstract This is a series of four lectures on the Standard Model. The role of conserved currents is emphasized. Both degeneracy of states and the Goldstone mode are discussed as realization of current conservation. Remarks on strongly interact- ing Higgs fields are included. No originality is intended and no references are given for this reason. These lectures can serve only as a material supplemental to standard textbooks. PRELIMINARIES Standard Model (SM) of electroweak interactions describes, as is well known, a huge amount of exper- imental data. Comparison with experiment is not, however, the aspect of the SM which is emphasized in present lectures. Rather we treat SM as a field theory and concentrate on basic ideas underlying this field theory. Th Standard Model describes interactions of fields of various spins and includes spin-1, spin-1/2 and spin-0 particles. Spin-1 particles are observed as gauge bosons of electroweak interactions. Spin- 1/2 particles are represented by quarks and leptons. And spin-0, or Higgs particles have not yet been observed although, as we shall discuss later, we can say that scalar particles are in fact longitudinal components of the vector bosons. Interaction of the vector bosons can be consistently described only if it is highly symmetrical, or universal. Moreover, from experiment we know that the corresponding couplings are weak and can be treated perturbatively. Interaction of spin-1/2 and spin-0 particles are fixed by theory to a much lesser degree and bring in many parameters of the SM. -
Three Lectures on Meson Mixing and CKM Phenomenology
Three Lectures on Meson Mixing and CKM phenomenology Ulrich Nierste Institut f¨ur Theoretische Teilchenphysik Universit¨at Karlsruhe Karlsruhe Institute of Technology, D-76128 Karlsruhe, Germany I give an introduction to the theory of meson-antimeson mixing, aiming at students who plan to work at a flavour physics experiment or intend to do associated theoretical studies. I derive the formulae for the time evolution of a neutral meson system and show how the mass and width differences among the neutral meson eigenstates and the CP phase in mixing are calculated in the Standard Model. Special emphasis is laid on CP violation, which is covered in detail for K−K mixing, Bd−Bd mixing and Bs−Bs mixing. I explain the constraints on the apex (ρ, η) of the unitarity triangle implied by ǫK ,∆MBd ,∆MBd /∆MBs and various mixing-induced CP asymmetries such as aCP(Bd → J/ψKshort)(t). The impact of a future measurement of CP violation in flavour-specific Bd decays is also shown. 1 First lecture: A big-brush picture 1.1 Mesons, quarks and box diagrams The neutral K, D, Bd and Bs mesons are the only hadrons which mix with their antiparticles. These meson states are flavour eigenstates and the corresponding antimesons K, D, Bd and Bs have opposite flavour quantum numbers: K sd, D cu, B bd, B bs, ∼ ∼ d ∼ s ∼ K sd, D cu, B bd, B bs, (1) ∼ ∼ d ∼ s ∼ Here for example “Bs bs” means that the Bs meson has the same flavour quantum numbers as the quark pair (b,s), i.e.∼ the beauty and strangeness quantum numbers are B = 1 and S = 1, respectively. -
Phenomenology Lecture 6: Higgs
Phenomenology Lecture 6: Higgs Daniel Maître IPPP, Durham Phenomenology - Daniel Maître The Higgs Mechanism ● Very schematic, you have seen/will see it in SM lectures ● The SM contains spin-1 gauge bosons and spin- 1/2 fermions. ● Massless fields ensure: – gauge invariance under SU(2)L × U(1)Y – renormalisability ● We could introduce mass terms “by hand” but this violates gauge invariance ● We add a complex doublet under SU(2) L Phenomenology - Daniel Maître Higgs Mechanism ● Couple it to the SM ● Add terms allowed by symmetry → potential ● We get a potential with infinitely many minima. ● If we expend around one of them we get – Vev which will give the mass to the fermions and massive gauge bosons – One radial and 3 circular modes – Circular modes become the longitudinal modes of the gauge bosons Phenomenology - Daniel Maître Higgs Mechanism ● From the new terms in the Lagrangian we get ● There are fixed relations between the mass and couplings to the Higgs scalar (the one component of it surviving) Phenomenology - Daniel Maître What if there is no Higgs boson? ● Consider W+W− → W+W− scattering. ● In the high energy limit ● So that we have Phenomenology - Daniel Maître Higgs mechanism ● This violate unitarity, so we need to do something ● If we add a scalar particle with coupling λ to the W ● We get a contribution ● Cancels the bad high energy behaviour if , i.e. the Higgs coupling. ● Repeat the argument for the Z boson and the fermions. Phenomenology - Daniel Maître Higgs mechanism ● Even if there was no Higgs boson we are forced to introduce a scalar interaction that couples to all particles proportional to their mass. -
Standard Model and Measurements of Its Parameters (Like the Mass of the Top Quark) at Hadron Colliders Are Presented
Title: Physics at Hadron Colliders Lecturer: Dr Karl Jakobs Date and Times: 1st August at 11:15 2nd August at 10:15 3rd August at 10:15 3rd August at 11:15 Summary of the proposed talk: Present and future hadron colliders play an important role in the investigation of fundamental questions of particle physics. After an introductory lecture, tests of the Standard Model and measurements of its parameters (like the mass of the top quark) at hadron colliders are presented. In addition, it will be discussed how the Higgs boson can be searched for at hadron colliders and how "New Physics", i.e. physics beyond the Standard Model, can be explored. Results are presented from the currently ongoing run at the Tevatron proton antiproton collider at the US research lab Fermilab. In addition, the rich physics potential of the experiments at the CERN Large Hadron Collider is discussed. Prerequisite knowledge and references: - The Standard Model (Lecture by A. Pich) - Beyond the Standard Model (Lecture by E. Kiritsis) Biography- Brief CV: Dr Karl JAKOBS -Studied Physics at the University of Bonn, Germany - Summer student at CERN in 1984 - PhD at the University of Heidelberg, in 1988 Thesis on the UA2-Experiment at the CERN Proton-Antiproton Collider (already Hadron Collider physics at that time) - Fellow and staff position at CERN, UA2 experiment - 1992 - 1996 Max-Planck-Institute for Physics, Munich ALEPH and ATLAS experiments - 1996 - 2003 Prof. of physics at the University of Mainz ALEPH and ATLAS experiments - Since 2000: participation in the D0-Experiment at the Tevatron HR-RFA 07/06 - Since 2003: Prof. -
Antiprotons in the Big Machine
Antiprotons in the big machine Right the beam line which injects 26 GeV antiprotons into the SPS. Centre, the beam fine which sends high energy protons from the SPS towards the West Experimental Area. The main ring is on the left. (Photo CERN 38.4.81) On 7 July a pulse of antiprotons was sent to the CERN Super Proton Synchrotron, accelerated to 270 GeV and (briefly) stored. Two days later the exercise was repeated with greater success and the first evi dence obtained for proton-antipro ton collisions at 540 GeV — by far the highest collision energies ever achieved. Although there is still much to be done before the scheme becomes fully operational, this achievement is a major milestone in the CERN antiproton story. The origins of the project Antiprotons, since they presuma bly have the same properties as protons except for the sign of their electric charge, can be accelerated and stored in the same magnet ring as protons. Thus colliding beam sys tems, like the familiar electron-posi tron machines, are, in principle, fea sible. However until recently it was not possible to produce antiproton tion, the antiprotons emerge with a for colliding beam physics. It in beams of sufficient intensity and wide range of momenta, distinctly volves using electron beams travel density to give sufficient collisions in unsuitable for a magnet system in a ling along with the antiproton beam a reasonable enough time for useful beam transfer line, an accelerator or at the same velocity. The electron physics to be done. a storage ring which is designed to beam, which is much easier to con This situation has changed with handle a well defined particle mo trol, has particles at precisely the the invention of 'beam cooling'. -
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 ........................... -
The Standard Model 30 Years of Glory
FR0107537 LAX66-128 March 2001 The Standard Model 30 Years of Glory Jacques Lefrangois Laboratoire de l'Accelerateur Lineaire IN2P3-CNRS et Universite de Paris-Sud, BP 34, F-91898 Orsay Cedex Lectures given at the 11th Advanced Study Institute on Techniques and Concepts in High Energy Physics, St. Croix, Virgin Islands, USA, June 15-26, 2000 U.E.R Institut National de de Physique Nucleaire 1'Universite Paris-Sud et de Physique des Particules 5 2/ § 8 B.P. 34 ~ Bailment 200 ~ 91898 ORSAY CEDEX LAL 00-128 March 2001 Doc. Enreg. ie. THE STANDARD MODEL 30 YEARS OF GLORY Jacques Lefrangois Laboratoire de VAccelerateur Lineaire IN2P3-CNRS et Universite PARIS-SUD Centre Scientifique d'Orsay - Bat. 200 - B.P. 34 91898 ORSAY Cedex (France) [email protected] In these three lectures, I will try to give a flavour of the achievements of the past 30 years, which saw the birth, and the detailed confirma- tion of the Standard Model (SM). However I have to start with three disclaimers: B Most of the subject is now history, but I am not an historian, I hope the main core will be exact but I may err on some details. • Being an experimentalist, I will mostly focus on the main exper- imental results, giving, when appropriate, some emphasis to the role of well conceived apparatus. This does not mean that I min- imise the key role of theorist, it only reflects the fact that the same story told by a theorist would correspond to another interesting series of lectures. • Finally, in some cases, I may show a bias coming from the fact that I have seen from closer what has happened in Europe. -
CERN Courier – Digital Edition Welcome to the Digital Edition of the December 2014 Issue of CERN Courier
I NTERNATIONAL J OURNAL OF H IGH -E NERGY P HYSICS CERNCOURIER WELCOME V OLUME 5 4 N UMBER 1 0 D ECEMBER 2 0 1 4 CERN Courier – digital edition Welcome to the digital edition of the December 2014 issue of CERN Courier. As CERN’s 60th-anniversary year comes to an end, CERN Courier gives a voice to some of the organization’s pioneers who are no longer with us. Extracts from audio recordings in CERN’s archives bring to life the spirit of adventure of the early CERN. One of the studies that CERN pioneered was the measurement of the “g-2” parameter of the muon – an experiment that in its latest incarnation is setting up in Fermilab. The year also saw the 50th anniversary of the International Centre for Theoretical Physics in Trieste, and an interview with the centre’s current director reveals interesting similarities and contrasts between the two organizations. The end of the year also offers the traditional seasonal Bookshelf. Happy reading! To sign up to the new-issue alert, please visit: http://cerncourier.com/cws/sign-up. To subscribe to the magazine, the e-mail new-issue alert, please visit: http://cerncourier.com/cws/how-to-subscribe. IceCube: neutrinos and more DETECTORS PEOPLE THE ICTP CUORE: the coldest CERN Council heart in the selects the next AT 50 EDITOR: CHRISTINE SUTTON, CERN known universe director-general An interview with DIGITAL EDITION CREATED BY JESSE KARJALAINEN/IOP PUBLISHING, UK p5 p5 Fernando Quevedo p37 CERNCOURIER www. V OLUME 5 4 N UMBER 1 0 D ECEMBER 2 0 1 4 CERN Courier December 2014 High Vacuum Contents Covering current developments in high-energy physics and related fi elds worldwide CERN Courier is distributed to member-state governments, institutes and laboratories Monitoring and Control affi liated with CERN, and to their personnel.