The Discovery of the Tau Lepton and the Changes in Elementary Particle Physics in 40 Years
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Decays of the Tau Lepton*
SLAC - 292 UC - 34D (E) DECAYS OF THE TAU LEPTON* Patricia R. Burchat Stanford Linear Accelerator Center Stanford University Stanford, California 94305 February 1986 Prepared for the Department of Energy under contract number DE-AC03-76SF00515 Printed in the United States of America. Available from the National Techni- cal Information Service, U.S. Department of Commerce, 5285 Port Royal Road, Springfield, Virginia 22161. Price: Printed Copy A07, Microfiche AOl. JC Ph.D. Dissertation. Abstract Previous measurements of the branching fractions of the tau lepton result in a discrepancy between the inclusive branching fraction and the sum of the exclusive branching fractions to final states containing one charged particle. The sum of the exclusive branching fractions is significantly smaller than the inclusive branching fraction. In this analysis, the branching fractions for all the major decay modes are measured simultaneously with the sum of the branching fractions constrained to be one. The branching fractions are measured using an unbiased sample of tau decays, with little background, selected from 207 pb-l of data accumulated with the Mark II detector at the PEP e+e- storage ring. The sample is selected using the decay products of one member of the r+~- pair produced in e+e- annihilation to identify the event and then including the opposite member of the pair in the sample. The sample is divided into subgroups according to charged and neutral particle multiplicity, and charged particle identification. The branching fractions are simultaneously measured using an unfold technique and a maximum likelihood fit. The results of this analysis indicate that the discrepancy found in previous experiments is possibly due to two sources. -
Introduction to Subatomic- Particle Spectrometers∗
IIT-CAPP-15/2 Introduction to Subatomic- Particle Spectrometers∗ Daniel M. Kaplan Illinois Institute of Technology Chicago, IL 60616 Charles E. Lane Drexel University Philadelphia, PA 19104 Kenneth S. Nelsony University of Virginia Charlottesville, VA 22901 Abstract An introductory review, suitable for the beginning student of high-energy physics or professionals from other fields who may desire familiarity with subatomic-particle detection techniques. Subatomic-particle fundamentals and the basics of particle in- teractions with matter are summarized, after which we review particle detectors. We conclude with three examples that illustrate the variety of subatomic-particle spectrom- eters and exemplify the combined use of several detection techniques to characterize interaction events more-or-less completely. arXiv:physics/9805026v3 [physics.ins-det] 17 Jul 2015 ∗To appear in the Wiley Encyclopedia of Electrical and Electronics Engineering. yNow at Johns Hopkins University Applied Physics Laboratory, Laurel, MD 20723. 1 Contents 1 Introduction 5 2 Overview of Subatomic Particles 5 2.1 Leptons, Hadrons, Gauge and Higgs Bosons . 5 2.2 Neutrinos . 6 2.3 Quarks . 8 3 Overview of Particle Detection 9 3.1 Position Measurement: Hodoscopes and Telescopes . 9 3.2 Momentum and Energy Measurement . 9 3.2.1 Magnetic Spectrometry . 9 3.2.2 Calorimeters . 10 3.3 Particle Identification . 10 3.3.1 Calorimetric Electron (and Photon) Identification . 10 3.3.2 Muon Identification . 11 3.3.3 Time of Flight and Ionization . 11 3.3.4 Cherenkov Detectors . 11 3.3.5 Transition-Radiation Detectors . 12 3.4 Neutrino Detection . 12 3.4.1 Reactor Neutrinos . 12 3.4.2 Detection of High Energy Neutrinos . -
The PLUTO Experiment at DORIS (DESY) and the Discovery of the Gluon (A Recollection]
(9.46 GeV) and the gluon discovery (a critical recollection of PLUTO results)* Bruno R. Stella1,a and Hans-Jürgen Meyer2,b 1 Department of Physics of Roma Tre University and INFN; Rome, Italy 2 formerly at Department of Physics, Siegen University; Siegen, Germany Abstract. The hadronic decays of (9.46 GeV) were first studied by the PLUTO experiment at the DORIS e+e- storage ring (DESY). With the aim of determining the contribution of PLUTO to the discovery of the gluon, as members of this former collaboration we have reconsidered all the scientific material produced by PLUTO in 1978 and the first half of 1979. It results clearly that the experiment demonstrated the main decay of the (9.46 GeV) resonance to be mediated by 3 gluons, by providing evidence for the agreement of this hypothesis with average values and differential distributions of all possible experimental variables and by excluding all other possible alternative models. Jettiness resulted evident by the average transverse momentum <pT> with respect to the event thrust axis, which was the same as experimentally observed by PLUTO itself at nearby continuum c.m.s. energies for 2-quark jet events. On the contrary, the average sphericity <S> and more topological variables as well as the momentum distribution showed a net difference with the same data comparison, a result compatible with jettiness only in case of more than 2 jets. Flatness as consequence of a 3-body decay (therefore 3 jets) was indicated by the low average momentum out of the event plane <pout>, altogether a result being independent of models. -
Machine-Learning-Based Global Particle-Identification Algorithms At
Machine-Learning-based global particle-identification algorithms at the LHCb experiment Denis Derkach1;2, Mikhail Hushchyn1;2;3, Tatiana Likhomanenko2;4, Alex Rogozhnikov2, Nikita Kazeev1;2, Victoria Chekalina1;2, Radoslav Neychev1;2, Stanislav Kirillov2, Fedor Ratnikov1;2 on behalf of the LHCb collaboration 1 National Research University | Higher School of Economics, Moscow, Russia 2 Yandex School of Data Analysis, Moscow, Russia 3 Moscow Institute of Physics and Technology, Moscow, Russia 4 National Research Center Kurchatov Institute, Moscow, Russia E-mail: [email protected] Abstract. One of the most important aspects of data analysis at the LHC experiments is the particle identification (PID). In LHCb, several different sub-detectors provide PID information: two Ring Imaging Cherenkov (RICH) detectors, the hadronic and electromagnetic calorimeters, and the muon chambers. To improve charged particle identification, we have developed models based on deep learning and gradient boosting. The new approaches, tested on simulated samples, provide higher identification performances than the current solution for all charged particle types. It is also desirable to achieve a flat dependency of efficiencies from spectator variables such as particle momentum, in order to reduce systematic uncertainties in the physics results. For this purpose, models that improve the flatness property for efficiencies have also been developed. This paper presents this new approach and its performance. 1. Introduction Particle identification (PID) algorithms play a crucial part in any high-energy physics analysis. A higher performance algorithm leads to a better background rejection and thus more precise results. In addition, an algorithm is required to work with approximately the same efficiency in the full available phase space to provide good discrimination for various analyses. -
Jet Production and High Pt Phenomena in Photon-Photon Reactions*
JET PRODUCTION AND HIGH PT PHENOMENA IN PHOTON-PHOTON REACTIONS* NORBERT WERMES ~" Stanford Linear Accelerator Center Stanford University, Stanford, California 94305 ABSTRACT The status of experimental investigations of high PT phenomena and jet production in photon- photon collisions is reviewed. Taking the challenging questions on hard scattering processes in ~/ff reactions as a guide, the experimental approach to these questions is summarized. Results from the PETRA experiments CELLO, JADE, PLUTO, and TASSO are presented including preliminary results on the Q2-dependence of jet cross sections. Experimental limitations and background problems are discussed. Zusammenfassung -- Es wird ein Uberblick fiber den Stand experimenteller Untersuchungen yon high-PT Ph~nomenen und der Erzeugung von Jets in Photon-Photon Wechselwirkungen gegeben. Anhand der herausfordernden Fragen beziiglich harter Streuprozesse in ~/ff Reaktionen wird der experimentelle Ansatz zur Beantwortung dieser Fragen zusammengefasst. Ergebnisse der PETRA Experimente CELLO, JADE, PLUTO und TASSO werden presentiert. Vorli~ufige Untersuchungen der Q2-Abh~ngigkeit von Jet-Wirkungsquerschnitten sowie experimentelle Einschr~nkungen und Untergrundprobleme werden diskutiert. * Work supported by the Department of Energy, contract DE-AC03-76SF00515. ? Alexander yon Humboldt Fellow. 120 1. INTRODUCTION This talk reviews experimental results on hard scattering reactions in qff collisions via high PT phenomena. The talk is divided into three parts. First I shall try to list the physics challenges for photon- photon experiments, in the context of hard scattering processes at high PT. In the main part the experimental approach to these challenging questions is discussed. It will be explained why we believe that hard scattering processes do exist. Then the explicit jet-searches performed by the different experiments are reviewed. -
J = Τ MASS Page 1
Citation: P.A. Zyla et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2020, 083C01 (2020) J 1 τ = 2 + + τ discovery paper was PERL 75. e e− → τ τ− cross-section threshold behavior and magnitude are consistent with pointlike spin- 1/2 Dirac particle. BRANDELIK 78 ruled out pointlike spin-0 or spin-1 particle. FELDMAN 78 ruled out J = 3/2. KIRKBY 79 also ruled out J=integer, J = 3/2. τ MASS VALUE (MeV) EVTS DOCUMENT ID TECN COMMENT 1776..86 0..12 OUR AVERAGE ± +0.10 1776.91 0.12 1171 1 ABLIKIM 14D BES3 23.3 pb 1, Eee = ± 0.13 − cm − 3.54–3.60 GeV 1776.68 0.12 0.41 682k 2 AUBERT 09AK BABR 423 fb 1, Eee =10.6 GeV ± ± − cm 1776.81+0.25 0.15 81 ANASHIN 07 KEDR 6.7 pb 1, Eee = 0.23 ± − cm − 3.54–3.78 GeV 1776.61 0.13 0.35 2 BELOUS 07 BELL 414 fb 1 Eee =10.6 GeV ± ± − cm 1775.1 1.6 1.0 13.3k 3 ABBIENDI 00A OPAL 1990–1995 LEP runs ± ± 1778.2 0.8 1.2 ANASTASSOV 97 CLEO Eee = 10.6 GeV ± ± cm . +0.18 +0.25 4 Eee . 1776 96 0.21 0.17 65 BAI 96 BES cm= 3 54–3 57 GeV − − 1776.3 2.4 1.4 11k 5 ALBRECHT 92M ARG Eee = 9.4–10.6 GeV ± ± cm +3 6 Eee 1783 4 692 BACINO 78B DLCO cm= 3.1–7.4 GeV − We do not use the following data for averages, fits, limits, etc. -
Particle Identification
Particle Identification Graduate Student Lecture Warwick Week Sajan Easo 28 March 2017 1 Outline Introduction • Main techniques for Particle Identification (PID) Cherenkov Detectors • Basic principles • Photodetectors • Example of large Cherenkov detector in HEP Detectors using Energy Loss (dE/dx) from ionization and atomic excitation Time of Flight (TOF) Detectors Transition Radiation Detectors (TRD) More Examples of PID systems • Astroparticle Physics . Not Covered : PID using Calorimeters . Focus on principles used in the detection methods. 2 Introduction . Particle Identification is a crucial part of several experiments in Particle Physics. • goal: identify long-lived particles which create signals in the detector : electrons, muons ,photons , protons, charged pions, charged kaons etc. • short-lived particles identified from their decays into long-lived particles • quarks, gluons : inferred from hadrons, jets of particles etc , that are created. In the experiments at the LHC: Tracking Detector : Directions of charged particles (from the hits they create in silicon detectors, wire chambers etc.) Tracking Detector + Magnet : Charges and momenta of the charged particles (Tracking system ) Electromagnetic Calorimeter (ECAL) : Energy of photons, electrons and positrons (from the energy deposited in the clusters of hits they create in the shape of showers ). Hadronic Calorimeter (HCAL) : Energy of hadrons : protons, charged pions etc. ( from the energy deposited in the clusters of hits they create in the shape of showers ) Muon Detector : Tracking detector for muons, after they have traversed the rest of the detectors 3 Introduction Some of the methods for particle identification: Electron : ECAL cluster has a charged track pointing to it and its energy from ECAL is close to its momentum from Tracking system. -
Tau (Or No) Leptons in Top Quark Decays at Hadron Colliders
Tau (or no) leptons in top quark decays at hadron colliders Michele Gallinaro for the CDF, D0, ATLAS, and CMS collaborations Laborat´oriode Instrumenta¸c˜aoe F´ısicaExperimental de Part´ıculas LIP Lisbon, Portugal DOI: http://dx.doi.org/10.3204/DESY-PROC-2014-02/12 Measurements in the final states with taus or with no-leptons are among the most chal- lenging as they are those with the smallest signal-to-background ratio. However, these final states are of particular interest as they can be important probes of new physics. Tau identification techniques and cross section measurements in top quark decays in these final states are discussed. The results, limited by systematical uncertainties, are consistent with standard model predictions, and are used to set stringent limits on new physics searches. The large data samples available at the Fermilab and at the Large Hadron Collider may help further improving the measurements. 1 Introduction Many years after its discovery [1, 2], the top quark still plays a fundamental role in the program of particle physics. The study of its properties has been extensively carried out in high energy hadron collisions. The production cross section has been measured in many different final states. Deviation of the cross section from the predicted standard model (SM) value may indicate new physics processes. Top quarks are predominantly produced in pairs, and in each top quark pair event, there are two W bosons and two bottom quarks. From the experimental point of view, top quark pair events are classified according to the decay mode of the two W bosons: the all-hadronic final state, in which both W bosons decay into quarks, the “lepton+jet” final state, in which one W decays leptonically and the other to quarks, and the dilepton final state, in which both W bosons decay leptonically. -
A Historical Review of the Discovery of the Quark and Gluon Jets
EPJ manuscript No. (will be inserted by the editor) JETS AND QCD: A Historical Review of the Discovery of the Quark and Gluon Jets and its Impact on QCD⋆ A.Ali1 and G.Kramer2 1 DESY, D-22603 Hamburg (Germany) 2 Universit¨at Hamburg, D-22761 Hamburg (Germany) Abstract. The observation of quark and gluon jets has played a crucial role in establishing Quantum Chromodynamics [QCD] as the theory of the strong interactions within the Standard Model of particle physics. The jets, narrowly collimated bundles of hadrons, reflect configurations of quarks and gluons at short distances. Thus, by analysing energy and angular distributions of the jets experimentally, the properties of the basic constituents of matter and the strong forces acting between them can be explored. In this review, which is primarily a description of the discovery of the quark and gluon jets and the impact of their obser- vation on Quantum Chromodynamics, we elaborate, in particular, the role of the gluons as the carriers of the strong force. Focusing on these basic points, jets in e+e− collisions will be in the foreground of the discussion and we will concentrate on the theory that was contempo- rary with the relevant experiments at the electron-positron colliders. In addition we will delineate the role of jets as tools for exploring other particle aspects in ep and pp/pp¯ collisions - quark and gluon densi- ties in protons, measurements of the QCD coupling, fundamental 2-2 quark/gluon scattering processes, but also the impact of jet decays of top quarks, and W ±, Z bosons on the electroweak sector. -
Sensitivity Physics. D KAONS, Or
A PERIODICAL OF PARTICLE PHYSICS WINTER 1995 VOL. 25, NUMBER 4 Editors RENE DONALDSON, BILL KIRK Contributing Editor MICHAEL RIORDAN Editorial Advisory Board JAMES BJORKEN, GEORGE BROWN, ROBERT N. CAHN, DAVID HITLIN, JOEL PRIMACK, NATALIE ROE, ROBERT SIEMANN Illustrations page 4 TERRY ANDERSON Distribution CRYSTAL TILGHMAN The Beam Line is published quarterly by the Stanford Linear Accelerator Center, PO Box 4349, Stanford, CA 94309. Telephone: (415) 926-2585 INTERNET: [email protected] FAX: (415) 926-4500 Issues of the Beam Line are accessible electronically on uayc ou the World Wide Web at http://www.slac.stanford.edu/ pubs/beamline/beamline.html SLAC is operated by Stanford University under contract with the U.S. Department of Energy. The opinions of the authors do not necessarily reflect the policy of the Stanford Linear Accelerator Center. Cover: Martin Perl (left) and Frederick Reines (center) receive the 1995 Nobel Prize in physics from His Majesty the King of Sweden at the awards ceremony last December. (Photograph courtesy of Joseph Peri) Printed on recycled paper tj) . CONTENTS FEATURES "We conclude that the signature e-/. events cannot be explained either by the production and decay of any presently known particles 4 Discovery of the Tau or as coming from any of the well- THE ROLE OF MOTIVATION & understood interactions which can TECHNOLOGY IN EXPERIMENTAL conventionally lead to an e and a PARTICLE PHYSICS gu in the final state. A possible ex- One of this year's Nobel Prize in physics planation for these events is the recipients describes the discovery production and decay of a pair of of the tau lepton in his 1975 new particles, each having a mass SLAC experiment. -
Search for Rare Multi-Pion Decays of the Tau Lepton Using the Babar Detector
SEARCH FOR RARE MULTI-PION DECAYS OF THE TAU LEPTON USING THE BABAR DETECTOR DISSERTATION Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of The Ohio State University By Ruben Ter-Antonyan, M.S. * * * * * The Ohio State University 2006 Dissertation Committee: Approved by Richard D. Kass, Adviser Klaus Honscheid Adviser Michael A. Lisa Physics Graduate Program Junko Shigemitsu Ralph von Frese ABSTRACT A search for the decay of the τ lepton to rare multi-pion final states is performed + using the BABAR detector at the PEP-II asymmetric-energy e e− collider. The anal- 1 ysis uses 232 fb− of data at center-of-mass energies on or near the Υ(4S) resonance. + 0 In the search for the τ − 3π−2π 2π ν decay, we observe 10 events with an ex- ! τ +2:0 pected background of 6:5 1:4 events. In the absence of a signal, we calculate the − + 0 6 decay branching ratio upper limit (τ − 3π−2π 2π ν ) < 3:4 10− at the 90 % B ! τ × confidence level. This is more than a factor of 30 improvement over the previously established limit. In addition, we search for the exclusive decay mode τ − 2!π−ν ! τ + 0 +1:0 with the further decay of ! π−π π . We observe 1 event, expecting 0.4 0:4 back- ! − 7 ground events, and calculate the upper limit (τ − 2!π−ν ) < 5:4 10− at the B ! τ × 90 % confidence level. This is the first upper limit for this mode. -
Detection of the Tau-Neutrino at The
DETECTION OF THE TAIPNEIITRINO AT me LI·IC* Klaus Winter CERN. Geneva. Switzerland I. Introduction Following the discovery of the tau-lepton in e+e` collisions by M. Perl and collabo rators [1 ], all evidence today favours the hypothesis that it is a sequential heavy lepton belonging to a third lepton Family [2]. From measurements of the forward-bacl< ward angular asymmetry of tau produced in e+e` annihilations [3], [4] e+e* +* ft a value of the axial-vector neutral current coupling constant of ga = — 0.—l5 1 0.05 was deduced in agreement with ga = -1 /2 for the assignment of lel’t—handed tau leptons as the "down" state (I3 = -1 /2) of a weak isospin doublet. Hence, the most natural assignment of the "up" state (I3 = +1/2) would be to a neutrino with the same lepton flavour. the tau-neutrino. Further indirect evidence about the tau—neutrino can be obtained from leptonic tau decays [4]. e.g. 1:- Q u_v,,X. The muon energy spectrum has the familiar [2] Michel shape suggesting that the par ticle X is a spin l /2 particle. Its mass has been constrained to less than 35 MeV by analysing semi-leptonic tau—deca)s with multipion final states [5]. Hence, the particle Xmay be a neutrino. Is it a sequential neutrino, with a flavour property which distin guishes it from the electron- and the muon-neutrino? The possibility of a complete identity with we or uu can indeed be excluded. Searches for charged current neutrino reactions which produce a tau-lepton UN ·=* T_X have given negative results.