Vision and Outlook: the Future of Particle Physics
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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. -
Pos(EPS-HEP 2013)161 ∗ [email protected] Speaker
Searches for Supersymmetry PoS(EPS-HEP 2013)161 Oliver Buchmueller∗ Imperial College London E-mail: [email protected] on behalf of the ATLAS and CMS Collaborations Since its first physics operation in 2010, the Large Hadron Collider at CERN has set a precedent in searches for supersymmetry. This proceeding report provides a brief overview on the current status of searches for supersymmetry at the LHC. The European Physical Society Conference on High Energy Physics -EPS-HEP2013 18-24 July 2013 Stockholm, Sweden ∗Speaker. c Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike Licence. http://pos.sissa.it/ Searches for Supersymmetry Oliver Buchmueller MSUGRA/CMSSM: tan() = 30, A = -2m0, µ > 0 Status: SUSY 2013 1000 0 SUSY 95% CL limits. theory not included. LSP [GeV] ATLAS Preliminary Expected 0-lepton, 2-6 jets h (122 GeV) 1/2 900 -1 Observed ATLAS-CONF-2013-047 L dt = 20.1 - 20.7 fb , s = 8 TeV m Expected 0-lepton, 7-10 jets Observed arXiv: 1308.1841 Expected 0-1 lepton, 3 b-jets 800 Observed ATLAS-CONF-2013-061 Expected 1-lepton + jets + MET Observed ATLAS-CONF-2013-062 h (124 GeV) Expected 1-2 taus + jets + MET 700 Observed ATLAS-CONF-2013-026 h (126 GeV) Expected 2-SS-leptons, 0 - 3 b-jets PoS(EPS-HEP 2013)161 Observed ATLAS-CONF-2013-007 600 ~g (1400 GeV) 500 ~g (1000 GeV) ~ 400 q ~ q (2000 GeV) (1600 GeV) 300 0 1000 2000 3000 4000 5000 6000 m0 [GeV] Figure 1: 95% C.L. -
The Five Common Particles
The Five Common Particles The world around you consists of only three particles: protons, neutrons, and electrons. Protons and neutrons form the nuclei of atoms, and electrons glue everything together and create chemicals and materials. Along with the photon and the neutrino, these particles are essentially the only ones that exist in our solar system, because all the other subatomic particles have half-lives of typically 10-9 second or less, and vanish almost the instant they are created by nuclear reactions in the Sun, etc. Particles interact via the four fundamental forces of nature. Some basic properties of these forces are summarized below. (Other aspects of the fundamental forces are also discussed in the Summary of Particle Physics document on this web site.) Force Range Common Particles It Affects Conserved Quantity gravity infinite neutron, proton, electron, neutrino, photon mass-energy electromagnetic infinite proton, electron, photon charge -14 strong nuclear force ≈ 10 m neutron, proton baryon number -15 weak nuclear force ≈ 10 m neutron, proton, electron, neutrino lepton number Every particle in nature has specific values of all four of the conserved quantities associated with each force. The values for the five common particles are: Particle Rest Mass1 Charge2 Baryon # Lepton # proton 938.3 MeV/c2 +1 e +1 0 neutron 939.6 MeV/c2 0 +1 0 electron 0.511 MeV/c2 -1 e 0 +1 neutrino ≈ 1 eV/c2 0 0 +1 photon 0 eV/c2 0 0 0 1) MeV = mega-electron-volt = 106 eV. It is customary in particle physics to measure the mass of a particle in terms of how much energy it would represent if it were converted via E = mc2. -
A Search for Supersymmetry in Events with Photons and Jets from Proton-Proton Collisions at √S = 7 Tev with the CMS Detector R
A Search for Supersymmetry in Events with Photons and Jets from Proton-Proton Collisions at ps = 7 TeV with the CMS Detector Robin James Nandi High Energy Physics Blackett Laboratory Imperial College London A thesis submitted to Imperial College London for the degree of Doctor of Philosophy and the Diploma of Imperial College. May 2012 Abstract An exclusion of Gauge Mediated Supersymmetry Breaking at 95% confidence level is 1 made in the squark mass vs gluino mass parameter space using 1:1 fb− of proton-proton collisions data from the Large Hadron Collider. The event selection is based on the strong production signature of photons, jets and missing transverse energy. Missing transverse energy is used to distinguish signal from background. The background is estimated with a data driven technique. The CLs method is used to exclude models with squark mass and gluino mass up to around 1 TeV. 1 Declaration This thesis is my own work. Information taken from other sources is appropriately refer- enced. Robin J. Nandi 2 Acknowledgements I would like to thank my supervisors Jonathan Hays and Chris Seez for their help and guidance. I would also like to thank the high energy physics group at Imperial College for taking me on as a PhD student and giving me support. I also acknowledge STFC for their financial support. I would also like to thank my friends and fellow PhD students: Paul Schaack, Arlo Bryer, Michael Cutajar, Zoe Hatherell and Alex Sparrow for helping me out, being with me in the office and making my time in Geneva and London more enjoyable. -
Fundamentals of Particle Physics
Fundamentals of Par0cle Physics Particle Physics Masterclass Emmanuel Olaiya 1 The Universe u The universe is 15 billion years old u Around 150 billion galaxies (150,000,000,000) u Each galaxy has around 300 billion stars (300,000,000,000) u 150 billion x 300 billion stars (that is a lot of stars!) u That is a huge amount of material u That is an unimaginable amount of particles u How do we even begin to understand all of matter? 2 How many elementary particles does it take to describe the matter around us? 3 We can describe the material around us using just 3 particles . 3 Matter Particles +2/3 U Point like elementary particles that protons and neutrons are made from. Quarks Hence we can construct all nuclei using these two particles -1/3 d -1 Electrons orbit the nuclei and are help to e form molecules. These are also point like elementary particles Leptons We can build the world around us with these 3 particles. But how do they interact. To understand their interactions we have to introduce forces! Force carriers g1 g2 g3 g4 g5 g6 g7 g8 The gluon, of which there are 8 is the force carrier for nuclear forces Consider 2 forces: nuclear forces, and electromagnetism The photon, ie light is the force carrier when experiencing forces such and electricity and magnetism γ SOME FAMILAR THE ATOM PARTICLES ≈10-10m electron (-) 0.511 MeV A Fundamental (“pointlike”) Particle THE NUCLEUS proton (+) 938.3 MeV neutron (0) 939.6 MeV E=mc2. Einstein’s equation tells us mass and energy are equivalent Wave/Particle Duality (Quantum Mechanics) Einstein E -
Introduction to Particle Physics
SFB 676 – Projekt B2 Introduction to Particle Physics Christian Sander (Universität Hamburg) DESY Summer Student Lectures – Hamburg – 20th July '11 Outline ● Introduction ● History: From Democrit to Thomson ● The Standard Model ● Gauge Invariance ● The Higgs Mechanism ● Symmetries … Break ● Shortcomings of the Standard Model ● Physics Beyond the Standard Model ● Recent Results from the LHC ● Outlook Disclaimer: Very personal selection of topics and for sure many important things are left out! 20th July '11 Introduction to Particle Physics 2 20th July '11 Introduction to Particle PhysicsX Files: Season 2, Episode 233 … für Chester war das nur ein Weg das Geld für das eigentlich theoretische Zeugs aufzubringen, was ihn interessierte … die Erforschung Dunkler Materie, …ähm… Quantenpartikel, Neutrinos, Gluonen, Mesonen und Quarks. Subatomare Teilchen Die Geheimnisse des Universums! Theoretisch gesehen sind sie sogar die Bausteine der Wirklichkeit ! Aber niemand weiß, ob sie wirklich existieren !? 20th July '11 Introduction to Particle PhysicsX Files: Season 2, Episode 234 The First Particle Physicist? By convention ['nomos'] sweet is sweet, bitter is bitter, hot is hot, cold is cold, color is color; but in truth there are only atoms and the void. Democrit, * ~460 BC, †~360 BC in Abdera Hypothesis: ● Atoms have same constituents ● Atoms different in shape (assumption: geometrical shapes) ● Iron atoms are solid and strong with hooks that lock them into a solid ● Water atoms are smooth and slippery ● Salt atoms, because of their taste, are sharp and pointed ● Air atoms are light and whirling, pervading all other materials 20th July '11 Introduction to Particle Physics 5 Corpuscular Theory of Light Light consist out of particles (Newton et al.) ↕ Light is a wave (Huygens et al.) ● Mainly because of Newtons prestige, the corpuscle theory was widely accepted (more than 100 years) Sir Isaac Newton ● Failing to describe interference, diffraction, and *1643, †1727 polarization (e.g. -
Quantum Field Theory*
Quantum Field Theory y Frank Wilczek Institute for Advanced Study, School of Natural Science, Olden Lane, Princeton, NJ 08540 I discuss the general principles underlying quantum eld theory, and attempt to identify its most profound consequences. The deep est of these consequences result from the in nite number of degrees of freedom invoked to implement lo cality.Imention a few of its most striking successes, b oth achieved and prosp ective. Possible limitation s of quantum eld theory are viewed in the light of its history. I. SURVEY Quantum eld theory is the framework in which the regnant theories of the electroweak and strong interactions, which together form the Standard Mo del, are formulated. Quantum electro dynamics (QED), b esides providing a com- plete foundation for atomic physics and chemistry, has supp orted calculations of physical quantities with unparalleled precision. The exp erimentally measured value of the magnetic dip ole moment of the muon, 11 (g 2) = 233 184 600 (1680) 10 ; (1) exp: for example, should b e compared with the theoretical prediction 11 (g 2) = 233 183 478 (308) 10 : (2) theor: In quantum chromo dynamics (QCD) we cannot, for the forseeable future, aspire to to comparable accuracy.Yet QCD provides di erent, and at least equally impressive, evidence for the validity of the basic principles of quantum eld theory. Indeed, b ecause in QCD the interactions are stronger, QCD manifests a wider variety of phenomena characteristic of quantum eld theory. These include esp ecially running of the e ective coupling with distance or energy scale and the phenomenon of con nement. -
Autumn Department of Physics Newsletter Issue
Autumn 2018, Number 13 Department of Physics Newsletter BEECROFT BUILDING OFFICIAL OPENING BEAUTIFUL HIGGS BOSON DECAYS MAGNETIC PINWHEELS EXTREME BEAM CONTROL COSMIC SHOCKS IN THE LABORATORY PEOPLE, EVENTS AND MORE www.physics.ox.ac.uk PROUD WINNERS OF: SCIENCE NEWS SCIENCE NEWS www.physics.ox.ac.uk/research www.physics.ox.ac.uk/research BEAUTIFUL HIGGS BOSON EXTREME BEAM CONTROL An Oxford team has succeeded in stabilising the arrival time of a ‘relativistic’ beam of electrons, travelling at almost the speed of light, to 50 femtoseconds. This overcomes one of the major challenges facing the proposed DECAYS Compact Linear Collider (CLIC). On 28 August 2018 the ATLAS and Higgs from the background. These Standard Model, the prevailing theory CMS collaborations announced, with results were used in the final Tevatron of particle physics. If this prediction had a seminar at CERN, the observation of combination, which reached almost turned out to be incorrect, it would have the Higgs boson decaying into pairs of three standard deviations in 2012, not shaken the foundations of the Standard beauty (b) quarks. Both experiments enough for a discovery. Model and pointed to new physics. at the Large Hadron Collider (LHC) Instead, this is an important milestone had surpassed the five standard and a beautiful confirmation of the EXPERIMENTAL CONFIRMATION deviations (sigma) mark for this process, so-called 'Yukawa couplings', which in Prof Daniela Bortoletto which is the convention in particle Goethe said: ‘Not art and science the Standard Model give masses to all Head of Particle Physics physics to claim a discovery. Five- serve alone; patience must in the quarks and leptons, the building blocks sigma corresponds to a probability of work be shown.’ It was with patience, of matter. -
1 Standard Model: Successes and Problems
Searching for new particles at the Large Hadron Collider James Hirschauer (Fermi National Accelerator Laboratory) Sambamurti Memorial Lecture : August 7, 2017 Our current theory of the most fundamental laws of physics, known as the standard model (SM), works very well to explain many aspects of nature. Most recently, the Higgs boson, predicted to exist in the late 1960s, was discovered by the CMS and ATLAS collaborations at the Large Hadron Collider at CERN in 2012 [1] marking the first observation of the full spectrum of predicted SM particles. Despite the great success of this theory, there are several aspects of nature for which the SM description is completely lacking or unsatisfactory, including the identity of the astronomically observed dark matter and the mass of newly discovered Higgs boson. These and other apparent limitations of the SM motivate the search for new phenomena beyond the SM either directly at the LHC or indirectly with lower energy, high precision experiments. In these proceedings, the successes and some of the shortcomings of the SM are described, followed by a description of the methods and status of the search for new phenomena at the LHC, with some focus on supersymmetry (SUSY) [2], a specific theory of physics beyond the standard model (BSM). 1 Standard model: successes and problems The standard model of particle physics describes the interactions of fundamental matter particles (quarks and leptons) via the fundamental forces (mediated by the force carrying particles: the photon, gluon, and weak bosons). The Higgs boson, also a fundamental SM particle, plays a central role in the mechanism that determines the masses of the photon and weak bosons, as well as the rest of the standard model particles. -
7. Gamma and X-Ray Interactions in Matter
Photon interactions in matter Gamma- and X-Ray • Compton effect • Photoelectric effect Interactions in Matter • Pair production • Rayleigh (coherent) scattering Chapter 7 • Photonuclear interactions F.A. Attix, Introduction to Radiological Kinematics Physics and Radiation Dosimetry Interaction cross sections Energy-transfer cross sections Mass attenuation coefficients 1 2 Compton interaction A.H. Compton • Inelastic photon scattering by an electron • Arthur Holly Compton (September 10, 1892 – March 15, 1962) • Main assumption: the electron struck by the • Received Nobel prize in physics 1927 for incoming photon is unbound and stationary his discovery of the Compton effect – The largest contribution from binding is under • Was a key figure in the Manhattan Project, condition of high Z, low energy and creation of first nuclear reactor, which went critical in December 1942 – Under these conditions photoelectric effect is dominant Born and buried in • Consider two aspects: kinematics and cross Wooster, OH http://en.wikipedia.org/wiki/Arthur_Compton sections http://www.findagrave.com/cgi-bin/fg.cgi?page=gr&GRid=22551 3 4 Compton interaction: Kinematics Compton interaction: Kinematics • An earlier theory of -ray scattering by Thomson, based on observations only at low energies, predicted that the scattered photon should always have the same energy as the incident one, regardless of h or • The failure of the Thomson theory to describe high-energy photon scattering necessitated the • Inelastic collision • After the collision the electron departs -
A Young Physicist's Guide to the Higgs Boson
A Young Physicist’s Guide to the Higgs Boson Tel Aviv University Future Scientists – CERN Tour Presented by Stephen Sekula Associate Professor of Experimental Particle Physics SMU, Dallas, TX Programme ● You have a problem in your theory: (why do you need the Higgs Particle?) ● How to Make a Higgs Particle (One-at-a-Time) ● How to See a Higgs Particle (Without fooling yourself too much) ● A View from the Shadows: What are the New Questions? (An Epilogue) Stephen J. Sekula - SMU 2/44 You Have a Problem in Your Theory Credit for the ideas/example in this section goes to Prof. Daniel Stolarski (Carleton University) The Usual Explanation Usual Statement: “You need the Higgs Particle to explain mass.” 2 F=ma F=G m1 m2 /r Most of the mass of matter lies in the nucleus of the atom, and most of the mass of the nucleus arises from “binding energy” - the strength of the force that holds particles together to form nuclei imparts mass-energy to the nucleus (ala E = mc2). Corrected Statement: “You need the Higgs Particle to explain fundamental mass.” (e.g. the electron’s mass) E2=m2 c4+ p2 c2→( p=0)→ E=mc2 Stephen J. Sekula - SMU 4/44 Yes, the Higgs is important for mass, but let’s try this... ● No doubt, the Higgs particle plays a role in fundamental mass (I will come back to this point) ● But, as students who’ve been exposed to introductory physics (mechanics, electricity and magnetism) and some modern physics topics (quantum mechanics and special relativity) you are more familiar with.. -
Comparing LHC Searches for Heavy Mediators of Dark Matter Production in Visible and Invisible Decay Channels
CERN-LPCC-2017-01 Recommendations of the LHC Dark Matter Working Group: Comparing LHC searches for heavy mediators of dark matter production in visible and invisible decay channels Andreas Albert,1;∗ Mihailo Backovi´c,2 Antonio Boveia,3;∗ Oliver Buchmueller,4;∗ Giorgio Busoni,5;∗ Albert De Roeck,6;7 Caterina Doglioni,8;∗ Tristan DuPree,9;∗ Malcolm Fairbairn,10;∗ Marie-H´el`eneGenest,11 Stefania Gori,12 Giuliano Gustavino,13 Kristian Hahn,14;∗ Ulrich Haisch,15;16;∗ Philip C. Harris,7 Dan Hayden,17 Valerio Ippolito,18 Isabelle John,8 Felix Kahlhoefer,19;∗ Suchita Kulkarni,20 Greg Landsberg,21 Steven Lowette,22 Kentarou Mawatari,11 Antonio Riotto,23 William Shepherd,24 Tim M.P. Tait,25;∗ Emma Tolley,3 Patrick Tunney,10;∗ Bryan Zaldivar,26;∗ Markus Zinser24 ∗Editor 1III. Physikalisches Institut A, RWTH Aachen University, Aachen, Germany 2Center for Cosmology, Particle Physics and Phenomenology - CP3, Universite Catholique de Louvain, Louvain-la-neuve, Belgium 3Ohio State University, 191 W. Woodruff Avenue Columbus, OH 43210 4High Energy Physics Group, Blackett Laboratory, Imperial College, Prince Consort Road, London, SW7 2AZ, United Kingdom arXiv:1703.05703v2 [hep-ex] 17 Mar 2017 5ARC Centre of Excellence for Particle Physics at the Terascale, School of Physics, Uni- versity of Melbourne, 3010, Australia 6Antwerp University, B2610 Wilrijk, Belgium. 7CERN, EP Department, CH-1211 Geneva 23, Switzerland 8Fysiska institutionen, Lunds universitet, Lund, Sweden 9Nikhef, Science Park 105, NL-1098 XG Amsterdam, The Netherlands 10Physics, King's College