The Large Hadron Collider (LHC)
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Chips for Discovering the Higgs Boson and Other Particles at CERN: Present and Future
Chips for discovering the Higgs boson and other particles at CERN: present and future W. Snoeys CERN PH-ESE-ME, Geneva, Switzerland [email protected] Abstract – Integrated circuits and devices revolutionized particle physics experiments, and have been essential in the recent discovery of the Higgs boson by the ATLAS and CMS experiments at the Large Hadron Collider at CERN [1,2]. Particles are accelerated and brought into collision at specific interaction points where detectors, giant cameras of about 40 m long by 20 m in diameter, take pictures of the collision products as they fly away from the collision point. These detectors contain millions of channels, often implemented as reverse biased silicon pin diode arrays covering areas of up to 200 m2 in the center of the experiment, generating a small (~1fC) electric charge upon particle traversals. Integrated circuits provide the readout, and accept collision rates of about 40 MHz with on-line selection of potentially interesting events before data storage. Important limitations are power consumption, radiation tolerance, data rates, and system issues like robustness, redundancy, channel-to-channel uniformity, timing distribution and safety. The already predominant role of Figure 1. Aerial view of CERN indicating the location of the 27 silicon devices and integrated circuits in these detectors km LHC ring with the position of the main experimental areas the is only expected to increase in the future. ring. The city of Geneva, its airport, the lake and Mont Blanc are visible © 2015 CERN. Keywords-particle detection; silicon pin diodes; charge sensitive readout II. MAIN CONSTRAINTS AND LIMITATIONS I. -
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. -
Phonon Spectroscopy of the Electron-Hole-Liquid W
PHONON SPECTROSCOPY OF THE ELECTRON-HOLE-LIQUID W. Dietsche, S. Kirch, J. Wolfe To cite this version: W. Dietsche, S. Kirch, J. Wolfe. PHONON SPECTROSCOPY OF THE ELECTRON- HOLE-LIQUID. Journal de Physique Colloques, 1981, 42 (C6), pp.C6-447-C6-449. 10.1051/jphyscol:19816129. jpa-00221192 HAL Id: jpa-00221192 https://hal.archives-ouvertes.fr/jpa-00221192 Submitted on 1 Jan 1981 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. JOURNAI, DE PHYSIQUE CoZZoque C6, suppZe'ment au nOl2, Tome 42, de'cembre 1981 page C6-447 PHONON SPECTROSCOPY OF THE ELECTRON-HOLE-LIQUID W. ~ietschejS.J. Kirch and J.P. Wolfe Physics Department and Materials Research ihboratory, University of IZZinois at Urbana-Champaign, Urbana, IL. 61 801, U. S. A. Abstract.-We have observed the 2kF cut-off in the phonon absorption of electron-hole droplets in Ge and measured the deformation potential. Photoexcited carriers in Ge at low temperatures condense into metallic drop- lets of electron-hole liquid (EHL).' These droplets provide a unique, tailorable system for studying the electron-phonon interaction in a Fermi liquid. The inter- 2 action of phonons with EHL was considered theoretically by Keldysh and has been studied experimentally using heat In contrast, we have employed mono- chromatic phonons5 to examine the frequency dependence of the absorption over the range of 150 - 500 GHz. -
Ity in the Topological Weyl Semimetal Nbp
Extremely large magnetoresistance and ultrahigh mobil- ity in the topological Weyl semimetal NbP Chandra Shekhar1, Ajaya K. Nayak1, Yan Sun1, Marcus Schmidt1, Michael Nicklas1, Inge Leermakers2, Uli Zeitler2, Yurii Skourski3, Jochen Wosnitza3, Zhongkai Liu4, Yulin Chen5, Walter Schnelle1, Horst Borrmann1, Yuri Grin1, Claudia Felser1, & Binghai Yan1;6 ∗ 1Max Planck Institute for Chemical Physics of Solids, 01187 Dresden, Germany 2High Field Magnet Laboratory (HFML-EMFL), Radboud University, Toernooiveld 7, 6525 ED Nijmegen, The Netherlands 3Dresden High Magnetic Field Laboratory (HLD-EMFL), Helmholtz-Zentrum Dresden- Rossendorf, 01328 Dresden, Germany 4Diamond Light Source, Harwell Science and Innovation Campus, Fermi Ave, Didcot, Oxford- shire, OX11 0QX, UK 5Physics Department, Oxford University, Oxford, OX1 3PU, UK 6Max Planck Institute for the Physics of Complex Systems, 01187 Dresden, Germany Recent experiments have revealed spectacular transport properties of conceptually simple 1 semimetals. For example, normal semimetals (e.g., WTe2) have started a new trend to realize a large magnetoresistance, which is the change of electrical resistance by an external magnetic field. Weyl semimetal (WSM) 2 is a topological semimetal with massless relativistic arXiv:1502.04361v2 [cond-mat.mtrl-sci] 22 Jun 2015 electrons as the three-dimensional analogue of graphene 3 and promises exotic transport properties and surface states 4–6, which are different from those of the famous topological 1 insulators (TIs) 7, 8. In this letter, we choose to utilize NbP in magneto-transport experiments because its band structure is on assembly of a WSM 9, 10 and a normal semimetal. Such a combination in NbP indeed leads to the observation of remarkable transport properties, an extremely large magnetoresistance of 850,000% at 1.85 K (250% at room temperature) in a magnetic field of 9 T without any signs of saturation, and ultrahigh carrier mobility of 5×106 cm2 V−1 s−1 accompanied by strong Shubnikov–de Hass (SdH) oscillations. -
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 -
Properties of Liquid Argon Scintillation Light Emission
Properties of Liquid Argon Scintillation Light Emission Ettore Segreto∗ Instituto de F´ısica \Gleb Wataghin" Universidade Estadual de Campinas - UNICAMP Rua S´ergio Buarque de Holanda, No 777, CEP 13083-859 Campinas, S~aoPaulo, Brazil (Dated: December 14, 2020) Liquid argon is used as active medium in a variety of neutrino and Dark Matter experiments thanks to its excellent properties of charge yield and transport and as a scintillator. Liquid argon scintillation photons are emitted in a narrow band of 10 nm centered around 127 nm and with a characteristic time profile made by two components originated by the decay of the lowest lying 1 + 3 + ∗ singlet, Σu , and triplet states, Σu , of the excimer Ar2 to the dissociative ground state. A model is proposed which takes into account the quenching of the long lived triplet states through the + self-interaction with other triplet states or through the interaction with molecular Ar2 ions. The model predicts the time profile of the scintillation signals and its dependence on the intensity of an external electric field and on the density of deposited energy, if the relative abundance of the unquenched fast and slow components is know. The model successfully explains the experimentally observed dependence of the characteristic time of the slow component on the intensity of the applied electric field and the increase of photon yield of liquid argon when doped with small quantities of xenon (at the ppm level). The model also predicts the dependence of the pulse shape parameter, Fprompt, for electron and nuclear recoils on the recoil energy and the behavior of the relative light yield of nuclear recoils in liquid argon, Leff . -
Search for New Physics in Same-Sign Dilepton Channel Using 35 Pb-1 of the CMS Data
CERN-THESIS-2011-276 SHARIF UNIVERSITY OF TECHNOLOGY PHYSICS DEPARTMENT Ph.D. Thesis Search for new physics in same-sign dilepton channel 1 using 35 pb− of the CMS data By: Hamed BAKHSHIANSOHI Supervisor: Professor Farhad ARDALAN Co-Supervisor: Professor Luc PAPE October 2011 Contents Contents Contentsa Acknowledgementj Introductionk 1 Standard Model and Supersymmetry1 1.1 The Standard Model and Gauge symmetries . .1 1.1.1 Spontaneous Symmetry Breaking and the Higgs mechanism . .3 1.1.2 Shortcomings of the Standard Model . .5 1.2 Supersymmetry . .8 1.2.1 How SUSY solves the problems of Standard Model . 10 1.3 The MSSM . 12 1.3.1 Supersymmetric Lagrangians . 12 1.3.2 The Minimal Supersymmetric Standard Model . 14 1.3.3 Supersymmetry Breaking . 16 1.3.4 Spontaneous Symmetry Breaking . 17 1.3.5 Minimal gravity mediated super symmetry breaking (mSUGRA) 19 2 The Large Hadron Collider (LHC) 22 2.1 Colliders in general . 22 2.1.1 LEP . 24 2.1.2 Tevatron . 25 2.2 LHC . 27 2.2.1 Motivations for LHC . 27 2.2.2 2008 incident . 30 2.2.3 2010 Data taking . 30 3 The Compact Muon Solenoid (CMS) experiment 34 3.1 The tracker . 38 3.1.1 Pixel detectors . 38 3.1.2 Silicon microstrip detectors . 41 3.1.3 Commissioning and performance with data . 42 3.2 The electromagnetic calorimeter (ECal) . 44 a Contents 3.2.1 Commissioning and performance with 2010 data . 45 3.2.2 Anomalous Energy Deposits (Spikes) . 46 3.3 The hadronic calorimeter (HCal) . 48 3.3.1 Commissioning and performance . -
Charge Separation and Dissipation in Molecular Wires Under a Light Radiation
Charge Separation and Dissipation in Molecular Wires under a Light Radiation Hang Xie*1, Yu Zhang2, Yanho Kwok 3, Wei E.I. Sha4 1 Department of Physics, Chongqing University, Chongqing, China 2Department of Chemistry, Northwestern University, Evanston, Illinois, United States 3Department of Chemistry, the University of Hong Kong, Hong Kong, China 4 College of Information Science & Electronic Engineering, Zhejiang University, Hangzhou 310027, P. R. China Photo-induced charge separation in nanowires or molecular wires had been studied in previous experiments and simulations. Most researches deal with the carrier diffusions with the classical phenomenological models, or the static energy levels by quantum mechanics calculations. Here we give a dynamic quantum investigation on the charge separation and dissipation in molecule wires. The method is based on the time-dependent non-equilibrium Green’s function theory. Polyacetylene chain and poly-phenylene are used as model systems with a tight-binding Hamiltonian and the wide band limit approximation in this study. A light pulse with the energy larger than the band gap is radiated on the system. The evolution and dissipation of the non-equilibrium carriers in the open nano systems are studied. With an external electric potentials or impurity atoms, the charge separation is observed. Our calculations show that the separation behaviors of the electron/hole wave packets are related to the Coulomb interaction, light intensity and the effective masses of electron/hole in the molecular wire. I. INTRODUCTION In the development of photovoltaic devices, some nanostructures such as graphene, silicon-nanowires, and 2D materials have gained a lot of interest [1, 2].