35. Particle Detectors at Accelerators
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CERN Courier–Digital Edition
CERNMarch/April 2021 cerncourier.com COURIERReporting on international high-energy physics WELCOME CERN Courier – digital edition Welcome to the digital edition of the March/April 2021 issue of CERN Courier. Hadron colliders have contributed to a golden era of discovery in high-energy physics, hosting experiments that have enabled physicists to unearth the cornerstones of the Standard Model. This success story began 50 years ago with CERN’s Intersecting Storage Rings (featured on the cover of this issue) and culminated in the Large Hadron Collider (p38) – which has spawned thousands of papers in its first 10 years of operations alone (p47). It also bodes well for a potential future circular collider at CERN operating at a centre-of-mass energy of at least 100 TeV, a feasibility study for which is now in full swing. Even hadron colliders have their limits, however. To explore possible new physics at the highest energy scales, physicists are mounting a series of experiments to search for very weakly interacting “slim” particles that arise from extensions in the Standard Model (p25). Also celebrating a golden anniversary this year is the Institute for Nuclear Research in Moscow (p33), while, elsewhere in this issue: quantum sensors HADRON COLLIDERS target gravitational waves (p10); X-rays go behind the scenes of supernova 50 years of discovery 1987A (p12); a high-performance computing collaboration forms to handle the big-physics data onslaught (p22); Steven Weinberg talks about his latest work (p51); and much more. To sign up to the new-issue alert, please visit: http://comms.iop.org/k/iop/cerncourier To subscribe to the magazine, please visit: https://cerncourier.com/p/about-cern-courier EDITOR: MATTHEW CHALMERS, CERN DIGITAL EDITION CREATED BY IOP PUBLISHING ATLAS spots rare Higgs decay Weinberg on effective field theory Hunting for WISPs CCMarApr21_Cover_v1.indd 1 12/02/2021 09:24 CERNCOURIER www. -
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. -
The Muon Range Detector at Sciboone Joseph Walding
The Muon Range Detector at SciBooNE Joseph Walding High Energy Physics Department, Blackett Laboratory, Imperial College, London Abstract. SciBooNE is a new neutrino experiment at Fermilab. The detector will undertake a number of measurements, principally sub-GeV neutrino cross-section measurements applicable to T2K. The detector consists of 3 sub-detectors; SciBar and the Electron-Catcher were both used in the K2K experiment at KEK, Japan, whilst the Muon Range Detector is a new detector constructed at Fermilab using recycled materials from previous Fermilab experiments. A description of the detector, its construction and software is presented here. Keywords: neutrino, neutrino detector, SciBooNE PACS: 01.30.Cc, 13.15.+g, 95.55.Vj SCIBOONE SciBooNE’s principal measurements are sub-GeV neutrino cross-section measurements applicable to T2K [1]. SciBooNE sits in the Booster neutrino beam 100 m downstream from the beam target. As well as carrying out sub-GeV cross-section measurements SciBooNE will also be used as a near detector for the MiniBooNE experiment [2]. The Muon Range Detector (MRD) is one of 3 sub-detectors that make up the SciBooNE detector [3]. It sits downstream of both SciBar and the Electron-Catcher (EC) both originally used in the K2K experiment [4] at KEK, Japan. The Muon Range Detector is made up largely from recycled materials from previous Fermilab experiments including all the PMTs, scintillator, iron absorber and data acquisition (DAQ) electronics. THE MUON RANGE DETECTOR The role of the Muon Range Detector is to confine the muons produced in charge-current quasi-elastic (CCQE) interactions, which is the dominant process in SciBooNE. -
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 -
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 . -
Flavour Physics
May 21, 2015 0:29 World Scientific Review Volume - 9in x 6in submit page 1 TASI Lectures on Flavor Physics Zoltan Ligeti Ernest Orlando Lawrence Berkeley National Laboratory, University of California, Berkeley, CA 94720 ∗E-mail: [email protected] These notes overlap with lectures given at the TASI summer schools in 2014 and 2011, as well as at the European School of High Energy Physics in 2013. This is primarily an attempt at transcribing my hand- written notes, with emphasis on topics and ideas discussed in the lec- tures. It is not a comprehensive introduction or review of the field, nor does it include a complete list of references. I hope, however, that some may find it useful to better understand the reasons for excitement about recent progress and future opportunities in flavor physics. Preface There are many books and reviews on flavor physics (e.g., Refs. [1; 2; 3; 4; 5; 6; 7; 8; 9]). The main points I would like to explain in these lectures are: • CP violation and flavor-changing neutral currents (FCNC) are sen- sitive probes of short-distance physics, both in the standard model (SM) and in beyond standard model (BSM) scenarios. • The data taught us a lot about not directly seen physics in the past, and are likely crucial to understand LHC new physics (NP) signals. • In most FCNC processes BSM/SM ∼ O(20%) is still allowed today, the sensitivity will improve to the few percent level in the future. arXiv:1502.01372v2 [hep-ph] 19 May 2015 • Measurements are sensitive to very high scales, and might find unambiguous signals of BSM physics, even outside the LHC reach. -
Incomplete Document
Improved measurement of the Pseudoscalar Decay Constants fDS from D∗+ γµ+ ν data sample s → Abstract + − Determination of fDS using 14 million e e cc¯ events obtained with the CLEO → II and CLEO II.V detector is presented. New measurement of the branching ratio gives Γ (D+ µ+ν)/Γ (D+ φπ+) = 0.137 0.013 0.022. Using Γ (D+ µ+ν) = 0.036 S → S → ± ± S → 0.09, fDS was calculated and found to be (247 12 20 31) MeV. Comparison ± ± ± ± of these results with other theoretical and experimental results are also presented. 1 Introduction Purely leptonic decay modes of heavy mesons predict their decay constants, which is connected with measured quantities such as CKM matrix elements. Currently it is not possible to measure fB experimentally, but measurements of the Cabibbo-flavor pseudoscalar decay constants such as fDS is possible. This measurement provides a check of these theoretical calculations and helps to establish different theoretical models. + The decay width of Ds is given by [1] G2 m2 Γ(D+ ℓ+ν)= F f 2 m2M 1 ℓ V 2 (1) s 6π DS ℓ DS 2 cs → − MDS ! | | where MDS is the Ds mass, mℓ is the mass of the final state lepton, Vcs is a CKM matrix element equal to 0.974 [2] and GF is the Fermi coupling constant. Various theoretical predictions of fDS range from 190 MeV to 350 MeV. The relative widths of three lepton flavors are 10 : 1 : 10−5 for tau, muon and electron respectively. Helicity suppression reduces smaller width for low mass electron. -
Searches for Dark Matter with Icecube and Deepcore
Matthias Danninger Searches for Dark Matter with IceCube and DeepCore New constraints on theories predicting dark-matter particles Department of Physics Stockholm University 2013 Doctoral Dissertation 2013 Oskar Klein Center for Cosmoparticle Physics Fysikum Stockholm University Roslagstullsbacken 21 106 91 Stockholm Sweden ISBN 978-91-7447-716-0 (pp. i-xii, 1-112) (pp. i-xii, 1-112) c Matthias Danninger, Stockholm 2013 Printed in Sweden by Universitetsservice US-AB, Stockholm 2013 Distributor: Department of Physics, Stockholm University Abstract The cubic-kilometer sized IceCube neutrino observatory, constructed in the glacial ice at the South Pole, searches indirectly for dark matter via neutrinos from dark matter self-annihilations. It has a high discovery potential through striking signatures. This thesis presents searches for dark matter annihilations in the center of the Sun using experimental data collected with IceCube. The main physics analysis described here was performed for dark matter in the form of weakly interacting massive particles (WIMPs) with the 79-string configuration of the IceCube neutrino telescope. For the first time, the Deep- Core sub-array was included in the analysis, lowering the energy threshold and extending the search to the austral summer. Data from 317 days live- time are consistent with the expected background from atmospheric muons and neutrinos. Upper limits were set on the dark matter annihilation rate, with conversions to limits on the WIMP-proton scattering cross section, which ini- tiates the WIMP capture process in the Sun. These are the most stringent spin- dependent WIMP-proton cross-sections limits to date above 35 GeV for most WIMP models. -
Current Status and Future Developments of Micromegas Detectors for Physics and Applications
applied sciences Review Current Status and Future Developments of Micromegas Detectors for Physics and Applications David Attié , Stephan Aune, Eric Berthoumieux , Francesco Bossù , Paul Colas, Alain Delbart, Emmeric Dupont, Esther Ferrer Ribas , Ioannis Giomataris , Aude Glaenzer , Hector Gómez , Frank Gunsing, Fanny Jambon, Fabien Jeanneau , Marion Lehuraux, Damien Neyret, Thomas Papaevangelou * , Emanuel Pollacco , Sébastien Procureur , Maxence Revolle , Philippe Schune, Laura Segui , Lukas Sohl * , Maxence Vandenbroucke and Zhibo Wu † CEA, Institut de Recherche sur les Lois Fondamentales de l’Univers, Université Paris-Saclay, 91191 Gif-sur-Yvette, France; [email protected] (D.A.); [email protected] (S.A.); [email protected] (E.B.); [email protected] (F.B.); [email protected] (P.C.); [email protected] (A.D.); [email protected] (E.D.); [email protected] (E.F.R.); [email protected] (I.G.); [email protected] (A.G.); [email protected] (H.G.); [email protected] (F.G.); [email protected] (F.J.); [email protected] (F.J.); [email protected] (M.L.); [email protected] (D.N.); [email protected] (E.P.); [email protected] (S.P.); [email protected] (M.R.); [email protected] (P.S.); [email protected] (L.S.); [email protected] (M.V.); [email protected] (Z.W.) * Correspondence: [email protected] (T.P.); [email protected] (L.S.) † Also: Department of Modern Physics, University of Science and Technology of China, Hefei 230026, China. Abstract: Micromegas (MICRO-MEsh GAseous Structure) detectors have found common use in Citation: Attié, D.; Aune, S.; different applications since their development in 1996 by the group of I. -
Design and Application of the Reconstruction Software for the Babar Calorimeter
Design and application of the reconstruction software for the BaBar calorimeter Philip David Strother Imperial College, November 1998 A thesis submitted for the degree of Doctor of Philosophy of the University of London, and Diploma of Imperial College 2 Abstract + The BaBar high energy physics experiment will be in operation at the PEP-II asymmetric e e− collider in Spring 1999. The primary purpose of the experiment is the investigation of CP violation in the neutral B meson system. The electromagnetic calorimeter forms a central part of the experiment and new techniques are employed in data acquisition and reconstruction software to maximise the capability of this device. The use of a matched digital filter in the feature extraction in the front end electronics is presented. The performance of the filter in the presence of the expected high levels of soft photon background from the machine is evaluated. The high luminosity of the PEP-II machine and the demands on the precision of the calorimeter require reliable software that allows for increased physics capability. BaBar has selected C++ as its primary programming language and object oriented analysis and design as its coding paradigm. The application of this technology to the reconstruction software for the calorimeter is presented. The design of the systems for clustering, cluster division, track matching, particle identification and global calibration is discussed with emphasis on the provisions in the design for increased physics capability as levels of understanding of the detector increase. The CP violating channel Bo J=ΨKo has been studied in the two lepton, two π0 final state. -
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. -
Improved Measurement of Neutral Current Coherent
Improved measurement of neutral current coherent The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Kurimoto, Y., et al. “Improved Measurement of Neutral Current Coherent π 0 Production on Carbon in a Few-GeV Neutrino Beam.” Physical Review D, vol. 81, no. 11, June 2010. © 2010 The American Physical Society As Published http://dx.doi.org/10.1103/PhysRevD.81.111102 Publisher American Physical Society (APS) Version Final published version Citable link http://hdl.handle.net/1721.1/116670 Terms of Use Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. RAPID COMMUNICATIONS PHYSICAL REVIEW D 81, 111102(R) (2010) Improved measurement of neutral current coherent 0 production on carbon in a few-GeV neutrino beam Y. Kurimoto,5 J. L. Alcaraz-Aunion,1 S. J. Brice,4 L. Bugel,13 J. Catala-Perez,18 G. Cheng,3 J. M. Conrad,13 Z. Djurcic,3 U. Dore,15 D. A. Finley,4 A. J. Franke,3 C. Giganti,15,* J. J. Gomez-Cadenas,18 P. Guzowski,6 A. Hanson,7 Y. Hayato,8 K. Hiraide,10,† G. Jover-Manas,1 G. Karagiorgi,13 T. Katori,7 Y.K. Kobayashi,17 T. Kobilarcik,4 H. Kubo,10 W. C. Louis,11 P.F. Loverre,15 L. Ludovici,15 K. B. M. Mahn,3,‡ C. Mariani,3 S. Masuike,17 K. Matsuoka,10 V.T. McGary,13 W. Metcalf,12 G.