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The Institute of Physics
REGIONAL NEWS 21 The Institute of Physics The forerunner of the Institute of do involves physics - switching on a light, physicists in commerce and industry. The Physics, the Physical Society of London, making a phone call or even baking a Council has established several Profession was created in 1874 at a time when the potato in a microwave oven. In industry, al Groups in areas such as consultancy, understanding of the physical world had physicists are helping companies to devel engineering physics and advanced been given an enormous impetus with the op novel materials that have physical prop systems. publication by James Clerk Maxwell of his erties more versatile that those previously In these days of shrinking science theory of electromagnetism. The creation developed, and they are designing new budgets, the academic physics community of the Physical Society was the response of generations of microchips which are has turned increasingly to its professional the embryonic society of professional and smaller and hence faster. The information representative, the Institute of Physics, to amateur physicists in Britain to what they revolution within which we are currently lobby Government about the importance believed was a major progression of their being buffeted would have been impos and relevance of physics. In common with ideas. Indeed, one could say that it was at sible without physicists and their research other science subjects, calls to justify Gov this time that much of physics began to - transistors, liquid crystal displays, mag ernment expenditure have increased in take on the appearance we recognize netic discs, optical fibres, semiconductor recent years. -
Direct Search for Standard Model-Like Higgs Boson And
Facult´edes Sciences de Base Institut de Physique de l’Energie´ et des Particules Laboratoire de Physique des Hautes Energies´ Direct Search for Standard Model-Like Higgs Boson and Software Integration of Data Acquisition Cards Th`ese de Doctorat pr´esent´ee `ala Section de Physique de la Facult´edes Sciences de Base de l’Ecole´ Polytechnique F´ed´erale de Lausanne pour l’obtention du grade de Docteur `es Sciences par C´edric Potterat Ing´enieur Physicien diplˆom´ede l’Ecole´ Polytechnique F´ed´erale de Lausanne, Suisse CERN-THESIS-2010-074 06/05/2010 Jury Prof. Nadine Baluc, Pr´esidente du jury Prof. Aurelio Bay, Directeur de th`ese Prof. Minh Quang Tran, Rapporteur Dr. Niko Neufeld, Rapporteur Dr. Tara Shears, Rapporteur CH - Lausanne 2010 R´esum´e Le Grand Collisionneur de Hadrons (LHC) au CERN, pr`es de Gen`eve, est con¸cu pour faire entrer en collision des protons `aune ´energie dans le centre de masse de 14 TeV. Il a ´et´etest´e `aplus faible ´energie en novembre 2009. Durant ces premiers jours, le LHC a ´etabli un nouveau record du monde avec ces deux faiseaux de protons `al’´energie de 1180 MeV. Le LHC a quatre points d’interaction pour les quartes grandes exp´eriences que sont : ALICE, ATLAS, CMS et LHCb. Le d´etecteur LHCb est situ´eau point d’interaction P8 (France). C’est un spectrom`etre `abras unique d´edi´e`ala physique des hardons contenant un quark b. Son but est l’´etude des processus qui ne conservent pas la sym´etrie CP et ainsi que certaines d´esint´egrations rares. -
Review of Literature Relating to Lhcb 2 Sin (✓W ) Measurement
University of Liverpool Department of Physics Faculty of Science and Engineering Review of Literature Relating to LHCb 2 sin (✓W ) Measurement Author: Abbie Jane Chadwick Supervisors: Prof. Tara Shears Dr. Stephen Farry Areportconcludingthefirstyearof PhD June 2020 Contents 1 The Standard Model 1 1.1 TheBasics .................................................. 1 1.2 TheUnderlyingPhysics ........................................... 2 1.3 TheDownfalls ................................................ 2 2 Collider Physics 4 2.1 ProbingtheStandardModel ........................................ 4 2.2 WorldColliderOverview........................................... 4 + 2.2.1 e e− .................................................. 4 2.2.2 pp and pp ............................................... 4 2.2.3 e±p .................................................. 5 2.2.4 Heavyions .............................................. 5 2 3 Sin (✓w) Measurement Survey 6 3.1 CMS...................................................... 6 3.2 LEPandSLD................................................. 8 3.3 CDFandD0 ................................................. 9 3.4 ATLAS .................................................... 9 3.5 LHCb ..................................................... 10 1 1 The Standard Model 1.1 The Basics The Standard Model (SM) is the most complete description of known elementary particles and their interactions currently within physics. It combines electromagnetic, weak and strong interactions into a quantum field theory, with the notable -
2013 January
Online Newsletter January 2013 Issue no 24 Branch committee REMS At Home - An Environmental Miscellany Dr Mark Telling CPhys MInstP, Chair On 10 January 71 members and guests were educated and entertained E-mail [email protected] by 5 invited speakers. The meeting was organised and orchestrated by Bob Boutland CPhys MInstP George Freeman, who unfortunately could not attend during Treasurer recuperation following an operation. Mike Quinton, (pictured below) Education representative introduced the speakers. and online newsletter editor E-mail [email protected] David Parkes CPhys MInstP Berkshire Centre representative E-mail [email protected] Stephen Elsmere Berkshire Centre representative E-mail [email protected] Leonard Lewell CPhys MInstP, London Centre Representative E-mail [email protected] Prof. R Mackintosh CPhys FInstP Milton Keynes Centre representative E-mail [email protected] Dr Diane Crann MInstP Hertfordshire Centre representative E-mail [email protected] J A Belling MInstP REMS visit secretary E-mail [email protected] The Barometer and its early use in forecasting on land and on sea” Marta Caballero E-mail [email protected] Anita McConnell Provided a very detailed story from the early days. It Student Representative was Torricelli and Viviani who showed in 1643-4 that there is such a thing as a vacuum noting that the height of the column mercury varied James Kneller daily with changes in the weather, but also with temperature. Pascal E-mail [email protected] Student Representative noted that a barometer recorded a lower pressure when taken up a mountain, the Puy de Dôme. -
Peter Kalmus, Rubab Khan, Luca Matone, Szabolcs Márka
Search Method for Gravitational Wave Transients Associated with the SGR 1806-20 Giant Flare We describe a method for searching for transient gravitational waves associated with the SGR 1806-20 T Peter Kalmus, Rubab Khan, Luca Matone, Szabolcs Márka C giant flare of 27 December 2004 using data collected by the LIGO 4 km detector located at Hanford, WA. A We create an excess power time series from a time-frequency tiling by projecting elements in the R T frequency band of interest onto the time axis. This time series is calibrated with injections of known Columbia University Experimental Gravity Group S strength. An upper limit estimate can then be obtained by selecting the loudest event in the on-source B A region. Validations for the search and estimated sensitivity, obtained by performing the search on realistic simulated LIGO data, are presented. 7. Estimated Sensitivity From Simulated Data 5. The Search Algorithm Simulated Noise 1. An Extraordinary Event To create simulated noise, a segment of LIGO noise is taken as a model. The individual On 27 December 2004, SGR 1806-20, a 'Soft Gamma Repeater' located 6-15 kpc Creation of Tiling and Band Plot data samples are randomly shuffled. The amplitude spectral density of the result is then away [1, 2], emitted the brightest transient ever observed [1, 6, 8, 11, 15]. Data Conditioning Conditioned data is transformed into a spectrogram, which is a linear time- matched to the LIGO noise bin by bin in frequency space, and the resulting series is frequency tiling. We take the complex magnitude of the resulting matrix. -
The Higgs Boson
The Higgs Boson Introduction: The standard model of Particle Physics is a set of mathematical formula, observations and measurements which describe the elementary particles and their interactions. Its purpose is to create a quantum theory of matter so we can predict quantum behaviour accurately. The standard model also presented a gap in the model that predicted the existence of the Higgs Boson. The standard model is composed of two types of particles: Matter particles (fermions) and the particles which mediate the forces that allow the matter particles to interact which are called Bosons. The W Boson and Z Boson (the electrically neutral boson of the W boson) are both responsible for mediating the Weak Nuclear Force (which is responsible for the change in flavour of quarks). The Higgs Boson is responsible for giving matter particles and the Gauge Bosons (W and Z Bosons) their mass.1 The Standard model:2 The Higgs Boson’s origin: In the 1970’s the standard model was finalised and allowed the Electromagnetic Force and the Weak Nuclear Force to be unified in the same theory of the Electroweak Force. However, this theory first predicted that electromagnetisms gauge boson (the photon) and the weak nuclear forces gauge boson ( W and Z bosons) must both have 0 mass in order to compliment the symmetry requirements in gauge theory. However, this was an issue as W 1 Tara Shears (2012) Philosophical Transactions: Mathematical, Physical and Engineering Sciences. 2 https://www.bing.com/images/search?view=detailV2&ccid=LHDm1cNr&id=4369541D8F9C168E0CCF97D7C5C 666865A769921&thid=OIP.LHDm1cNr5Jeajxvg4Q04EAHaFk&mediaurl=https%3a%2f%2fwww.abc.net.au%2fc m%2flb%2f7864318%2fdata%2fstandard-model-of-physics- data.jpg&exph=526&expw=700&q=the+standard+model&simid=608046680252745529&selectedIndex=2&adl t=strict&ajaxhist=0 and Z bosons have been both proven to have the corresponding masses of: 80.385 GeV and 91.1876 GeV, both discovered in 1983 at CERN. -
Symposium Celebrating CERN's Discoveries and Looking Into the Future
CERN–EP–2003–073 CERN–TH–2003–281 December 1st, 2003 Proceedings Symposium celebrating the Anniversary of CERN’s Discoveries and a Look into the Future 111999777333::: NNNeeeuuutttrrraaalll CCCuuurrrrrreeennntttsss 111999888333::: WWW±±± &&& ZZZ000 BBBooosssooonnnsss Tuesday 16 September 2003 CERN, Geneva, Switzerland Editors: Roger Cashmore, Luciano Maiani & Jean-Pierre Revol Table of contents Table of contents 2 Programme of the Symposium 4 Foreword (L. Maiani) 7 Acknowledgements 8 Selected Photographs of the Event 9 Contributions: Welcome (L. Maiani) 13 The Making of the Standard Model (S. Weinberg) 16 CERN’s Contribution to Accelerators and Beams (G. Brianti) 30 The Discovery of Neutral Currents (D. Haidt) 44 The Discovery of the W & Z, a personal recollection (P. Darriulat) 57 W & Z Physics at LEP (P. Zerwas) 70 Physics at the LHC (J. Ellis) 85 Challenges of the LHC: – the accelerator challenge (L. Evans) 96 – the detector challenge (J. Engelen) 103 – the computing challenge (P. Messina) 110 Particle Detectors and Society (G. Charpak) 126 The future for CERN (L. Maiani) 136 – 2 – Table of contents (cont.) Panel discussion on the Future of Particle Physics (chaired by Carlo Rubbia) 145 Participants: Robert Aymar, Georges Charpak, Pierre Darriulat, Luciano Maiani, Simon van der Meer, Lev Okun, Donald Perkins, Carlo Rubbia, Martinus Veltman, and Steven Weinberg. Statements from the floor by: Fabiola Gianotti, Ignatios Antoniadis, S. Glashow, H. Schopper, C. Llewellyn Smith, V. Telegdi, G. Bellettini, and V. Soergel. Additional contributions: Comment on the occasion (S. L. Glashow) 174 Comment on Perturbative QCD in early CERN experiments (D. H. Perkins) 175 Personal remarks on the discovery of Neutral Currents (A. -
Newsletter, November 2017
ISSN 1756-168X (Print) ISSN 2516-3353 (Online) Newsletter No. 35 November 2017 Published by the History of Physics Group of the Institute of Physics (UK & Ireland) ISSN 1756-168X IOP History of Physics Newsletter November 2017 Contents Editorial 2 Meeting Reports Chairman’s Report 3 Rutherford’s chemists - abstracts 5 ‘60 Years on from ZETA’ by Chris Warrick 10 Letters to the editor 13 Obituary John W Warren by Stuart Leadstone 15 Features Anti-matter or anti-substance? by John W Warren 16 A Laboratory in the Clouds - Horace-Bénédict de Saussure by Peter Tyson 18 On Prof. W.H.Bragg’s December 1914 Letter to the Vice- Chancellor of the University of Leeds by Chris Hammond 34 Book Reviews Crystal Clear - Autobiographies of Sir Lawrence and Lady Bragg by Peter Ford 54 Forthcoming Meetings 69 Committee and contacts 70 61 2 Editorial A big ‘Thank you’! Around 45 people attended the Bristol meeting on the History of Particle Colliders, in April. It was a joint meeting between the History of Physics Group, the High Energy Physics Group, and the Particle Accelerators and Beams Group. With a joint membership of around 2000, that works out at well under 3% - and that was a good turnout. The Rutherford’s Chemists meeting held in Glasgow attracted probably a similar percentage - not very high you might think. But time and travel costs to attend come at a premium so any means by which the content of our meetings may be promulgated - reports in our newsletter and in those of the other groups - is a very worthwhile task. -
Status of the Standard Model
Status of the Standard Model Tara Shears 1. Overview 2. Tests of the Standard Model 3. Shortcomings 4. Conclusions Overview • What is the Standard Model? – What does it describe? – What does it need as inputs? • Experimental tests – Verification of theory – Adding the missing parameters – Check internal consistency • Shortcomings – Experimental problems – Philosophical problems See also pp plenaries and parallel sessions for more details 1. Overview 2. Tests of the Standard Model 3. Shortcomings 4. Conclusions What does the Standard Model describe? SM describes matter – force interactions; – 12 types of matter particle (fermion) – 3 forces, mediated by force carrying particle (boson) We use the SM to predict experimental observations space boson Quarks (3 generations) fermion Leptons (3 generations) Force carriers time 1. Overview 2. Tests of the Standard Model 3. Shortcomings 4. Conclusions Constructing the Standard Model SM is a field theory. Describe force - matter interactions by Lagrangians _ µνµνµν µµµ L = -1/4F µνµνµν F +ΨΨΨ(i γγγ Dµµµ –m) ΨΨΨ Field strength Boson-fermion of force field F Fermion mass interaction, fermion movement Lagrangian L obeys local gauge invariance Doesn’t change as a function of space and time: ΨΨΨ→e-iθθθ(x,t) ΨΨΨ Consequence that bosons must be massless Each force described by L of similar form (details of F, D, Ψ vary) 1. Overview 2. Tests of the Standard Model 3. Shortcomings 4. Conclusions Constructing the Standard Model LSM = L EM + L WEAK + L STRONG EM force Weak force Strong force Electric charge (1) Weak charge (2) Colour charge (3) Massless photon Massive W±,Z 8 massless gluons Coupling g Coupling gW Coupling gs Value unknown/ not predicted 1. -
Peter Kalmus, Rubab Khan, Luca Matone, Szabolcs Márka Columbia
Search Method for Gravitational Wave Transients Associated with the SGR 1806-20 Giant Flare We describe a method for searching for transient gravitational waves associated with the SGR 1806-20 giant T Peter Kalmus, Rubab Khan, Luca Matone, Szabolcs Márka C flare of 27 December 2004 using data collected by the LIGO 4 km detector located at Hanford, WA. We create A an excess power time series from a time-frequency tiling by projecting elements in the frequency band of R T interest onto the time axis. This time series is calibrated with injections of known strength. An upper limit Columbia University Experimental Gravity Group S estimate can then be obtained by selecting the loudest event in the on-source region. Validations for the search B A and estimated sensitivity, obtained by performing the search on realistic simulated LIGO data, are presented. 7. Estimated Sensitivity From Simulated Data 5. The Search Algorithm Simulated Noise 1. An Extraordinary Event To create simulated noise, a segment of LIGO noise is taken as a model. This noise On 27 December 2004, SGR 1806-20, a 'Soft Gamma Repeater' located 6-15 kpc Creation of Tiling and Band Plot vector is randomized. The amplitude spectral density of the result is then matched to the away [1, 2], emitted the brightest transient ever observed [1, 6, 8, 11, 15]. Data Conditioning Conditioned data is transformed into a spectrogram, which is a linear time- LIGO noise bin by bin in frequency space, and the resulting series is inverse transformed frequency tiling. We take the complex magnitude of the resulting matrix. -
Why the Universe Exists How Particle Physics Unlocks the Secrets of Everything
Why the Universe Exists How particle physics unlocks the secrets of everything NEW SCIENTIST Contents Series introduction Contributors Introduction 1 Fantastic particles and where to find them 2 Boson power 3 The Higgs maker 4 Quark tales 5 Antimatter 6 The little neutral ones 7 The lethal lightweight 8 Superparticles and beyond 9 Pieces of gravity 10 After the Large Hadron Collider 11 Practical particles 12 Conclusion Fifty ideas Glossary Picture credits Series introduction New Scientist’s Instant Expert books shine light on the subjects that we all wish we knew more about: topics that challenge, engage enquiring minds and open up a deeper understanding of the world around us. Instant Expert books are definitive and accessible entry points for curious readers who want to know how things work and why. Look out for the other titles in the series: The End of Money How Evolution Explains Everything about Life How Your Brain Works Machines That Think The Quantum World Where the Universe Came From Your Conscious Mind Contributors Editor: Stephen Battersby is a physics writer and consultant for New Scientist. Series editor: Alison George is Instant Expert editor for New Scientist. Articles in this book are based on talks at the 2016 New Scientist masterclass ‘Mysteries of particle physics’ and articles previously published in New Scientist. Academic contributors Jon Butterworth is a professor of physics at University College London, and a member of the ATLAS collaboration at CERN’s Large Hadron Collider, who researches the mechanism of electroweak symmetry breaking, which explains why some things have mass. He wrote ‘Why do we need the Higgs?’ in Chapter 2, and Detector story plus ‘The big discovery’ in Chapter 3. -
Summer Students 2020.Pdf
A brief tour of the Particle World (and your lecture programme) Tara Shears, University of Liverpool1 Overview • What particle physics describes • What we know (and what we don’t) • The Standard Model: matter; forces; Higgs. • Experiments; performing research • Outstanding questions and mysteries … … just a taster of what’s waiting in your lectures 2 The Universe BIG BANG NOW 3 Cosmology LHC Nuclear physics Q&A: 23/7/20 Q&A: 21/7/20 Cosmic rays Astrophysics Quark/gluon plasma Plus …. Heavy ions Q&A: 29/7/20 Antimatter Q&A: 20/7/20 Astroparticle physics Q&A: 16/7/20 4 Matter u c t e μ τ d s b νe νμ ντ quarks leptons 5 Mass 2.4 MeV/c2 1.27 GeV/c2 171.2 GeV/c2 Charge 2/3 u 2/3 c 2/3 t Spin 1/2 1/2 1/2 up charm top quarks 4.8 MeV/c2 104 MeV/c2 4.2 GeV/c2 -1/3 d -1/3 -1/3 1/2 1/2 s 1/2 b down strange bottom 0.511 MeV/c2 105.7 MeV/c2 1.777 GeV/c2 -1 e -1 -1 1/2 1/2 m 1/2 t electron muon tau leptons < 2.2 eV/c2 < 0.17 MeV/c2 < 15.5 MeV/c2 (more about the 0 0 0 discoveries in ne nm nt Lecture 1, 1/2 1/2 1/2 Particle World) e neutrino m neutrino t neutrino 6 and … antimatter … 2 2 2 2 4 Einstein’s equation of motion*: E = p c + m c Two energy solutions for the same mass; • Matter • Antimatter Every fermion has an antimatter version.