The Higgs Boson

Total Page:16

File Type:pdf, Size:1020Kb

The Higgs Boson The Higgs Boson It could give mathematical consistency to the standard model-the theory that describes the intera ctions of fundam en tal particles. The search for the elusive particle will require new accelerators by MartinusJ. G. Veltman he truly fundamental problems dard model, making it applicable to generally make themselves felt by Tof physics can always be ex­ energy ranges beyond the capabilities means of the exchange of a mediating plained in simple terms without of the current generation of parti­ particle; the particle that mediates the the help of complicated equations or cle accelerators but that may soon be electromagnetic field, for example, is mathematical arguments. At least this reached by future accelerators. More­ the photon, or quantum of light. The was once told to me by Victor F. over, the Higgs boson is thought to mediating particles of the gravitation­ Weisskopf, an eminent physicist who generate the masses of all the funda­ al field, the weak field and the strong often engages in such explanations, mental particles; in a manner of speak­ field are respectively the graviton and he may very well be right. It cer­ ing, particles "eat" the Higgs boson to (which has not yet been detected), tainly holds for a proposed but un­ gain weight. three weak vector bosons, called the discovered particle called the Higgs The biggest drawback of the Higgs W+, W-and ZO particles, and eight boson and the so-called Higgs field as­ boson is that so far no evidence of gluons. In a somewhat analogous way sociated with it. its existence has been found. Instead the Higgs boson is the mediating parti­ The Higgs boson, which is named a fair amount of indirect evidence al­ cle of the proposed Higgs field. after Peter W. Higgs of the University ready suggests that the elusive particle It is now assumed that there is a con­ of Edinburgh, is the chief missing in­ does not exist. Indeed, modern theo­ stant Higgs field throughout all space, gredient in what is now called the stan­ retical physics is constantly filling the that is, the vacuum of outer space is dard model of elementary processes: vacuum with so many contraptions not empty but contains this constant the prevailing theory that describes the such as the Higgs boson that it is amaz­ field. The Higgs field is thought to gen­ basic constituents of matter and the ing a person can even see the stars on a erate mass by coupling to particles. fundamental forces by which they in­ clear night! Although future accelera­ Depending on the coupling strength, a teract. According to the standard mod­ tors may well find direct evidence of particle in space has a certain potential el, all matter is made up of quarks and the Higgs boson and show that the mo­ energy. By Einstein's famous equa­ leptons, which interact with one anoth­ tivations for postulating its existence tion, E = mc2 (energy equals mass er through four forces: gravity, elec­ are correct, I believe things will not be multiplied by the square of the speed tromagnetism, the weak force and the so simple. I must point out that this of light), the coupling energy is equiva­ strong force. The strong force, for in­ does not mean the entire standard lent to a mass. The stronger the cou­ stance, binds quarks together to make model is wrong. Rather, the standard pling, the greater the mass. protons and neutrons, and the residual model is probably only an approxima­ The way particles are thought to ac­ strong force binds protons and neu­ tion-albeit a good one-of reality. quire mass in their interactions with trons together into nuclei. The electro­ the Higgs field is somewhat analogous magnetic force binds nuclei and elec­ ven though the only legitimate rea­ to the way pieces of blotting paper ab­ trons, which are one kind of lepton, E son for introducing the Higgs bos­ sorb ink. In such an analogy the pieces into atoms, and the residual electro­ on is to make the standard model of paper represent individual parti­ magnetic force binds atoms into mole­ mathematically consistent, much at­ cles and the ink represents energy, or cules. The weak force is responsible tention has been given to the conceptu­ mass. Just as pieces of paper of differ­ for certain kinds of nuclear decay. The ally easier proposal that the particle ing size and thickness soak up vary­ influence of the weak force and the generates the masses of all the funda­ ing amounts of ink, different particles strong force extends only over a short mental particles. I shall therefore be­ "soak up" varying amounts of energy, range, no larger than the radius of an gin with that topic. or mass. The observed mass of a parti­ atomic nucleus; gravity and electro­ Central to an understanding of how cle depends on the particle's "energy­ magnetism have an unlimited range the Higgs boson would generate mass absorbing" ability and on the strength and are therefore the most familiar of is the concept of a field. A field is sim­ of the Higgs field in space. the forces. ply a quantity, such as temperature, In spite of all that is known about defined at every point throughout hat are the characteristics of the the standard model, there are reasons some region of space and time, such as Wproposed Higgs field? In or­ to think it is incomplete. That is where the surface of a frying pan. In physics der to endow particles with mass, the the Higgs boson comes in. Specifical­ the term "field" is usually reserved for Higgs field, if it exists, would have to ly, it is held that the Higgs boson gives such entities as the gravitational field assume a uniform, nonzero value even mathematical consistency to the stan- and the electromagnetic field. Fields in the vacuum. Moreover, the Higgs 76 © 1986 SCIENTIFIC AMERICAN, INC field would be a scalar field, which is what oversimplified way, the mass of The Higgs boson is called a scalar one of two kinds of field important in a person would change if he or she boson because it has a spin of O. Most describing the interactions of particles. turned around while standing in the other bosons associated with fields are A scalar field is a field in which each same place. In other words, the Higgs thought to be vector bosons: particles point has associated with it a single field is "spinless." that have a spin of l. The photon, magnitude, or number. The other im­ Because the Higgs field is spinless, gluon and W+, W-and ZO particles, portant field is a vector field: a field the Higgs boson must also be spinless. for instance, are spin-1 bosons. where at each point a vector, or arrow, Spin, as applied to elementary parti­ Since vector bosons are typically as­ is drawn. A vector has both a mag­ cles, is a quantum-mechanical proper­ sociated with the fundamental forces nitude, which is represented by the ty roughly equivalent to the classical of nature and the Higgs boson is a sca­ length of the arrow, and a direction. spin of a rotating ball. Elementary par­ lar boson, the force by which particles The electromagnetic, weak and strong ticles can take on only integer (0, 1, 2 couple to the Higgs field must be a fields are all vector fields. (The gravi­ and so on) and half-integer (1/2, 3/2 new force. It is introduced explicitly tational field is a special entity called a and so on) values of spin. Particles that and solely as a mechanism to improve tensor field.) have integral spin are called bosons the mathematical consistency of the The proposed Higgs field must be a and particles that have half-integral standard model. The Higgs force be­ scalar field, because if it were a vector spin are called fermions. Bosons and haves mathematically in a similar field, the mass of a particle would in fermions have sharply differing prop­ manner to the recently publicized general depend on the particle's align­ erties, but I shall not delve into that "fifth force" reported by Ephraim ment with the field. Stated in a some- topic here. Fischbach of Purdue University. The MAGNETIC MONOPOLES should exist if the Higgs boson ex­ monopoles could, however, be formed by sweeping magnetic field ists. Classically, of course, magnetic monopoles are not found be­ lines under the Higgs "rug" (top). The bottom illustration shows a cause when a bar magnet is cut in half, two smaller bar magnets pair of monopoles. Although there have been scattered reports of are created-not isolated "north" and "south" poles. Magnetic finding monopoles, none of them has been substantiated to date. 77 © 1986 SCIENTIFIC AMERICAN, INC proposed Higgs force is, however, known, for example, why the Higgs as the weak vector bosons, the energy weaker and has a much shorter range field should couple more strongly to density of the Higgs field in the vacu­ than the "fifth force." some particles than it does to others. um would be 10 trillion times greater The Higgs force is not a universal Nor do investigators understand how than the density of matter in an atomic force, because it couples differently the mass of the Higgs boson itself nucleus. If the earth were compressed to different particles. Specifically, if a (which is not known) comes about, al­ to this density, its volume would be ap­ particle is observed to have mass, the though it is generally presumed to be proximately 500 cubic centimeters, or strength of the coupling to the Higgs dominantly through a self-interaction a bit more than the size of a soft-drink field is assumed to be whatever quan­ with the Higgs field.
Recommended publications
  • 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.
    [Show full text]
  • The Particle World
    The Particle World ² What is our Universe made of? This talk: ² Where does it come from? ² particles as we understand them now ² Why does it behave the way it does? (the Standard Model) Particle physics tries to answer these ² prepare you for the exercise questions. Later: future of particle physics. JMF Southampton Masterclass 22–23 Mar 2004 1/26 Beginning of the 20th century: atoms have a nucleus and a surrounding cloud of electrons. The electrons are responsible for almost all behaviour of matter: ² emission of light ² electricity and magnetism ² electronics ² chemistry ² mechanical properties . technology. JMF Southampton Masterclass 22–23 Mar 2004 2/26 Nucleus at the centre of the atom: tiny Subsequently, particle physicists have yet contains almost all the mass of the discovered four more types of quark, two atom. Yet, it’s composite, made up of more pairs of heavier copies of the up protons and neutrons (or nucleons). and down: Open up a nucleon . it contains ² c or charm quark, charge +2=3 quarks. ² s or strange quark, charge ¡1=3 Normal matter can be understood with ² t or top quark, charge +2=3 just two types of quark. ² b or bottom quark, charge ¡1=3 ² + u or up quark, charge 2=3 Existed only in the early stages of the ² ¡ d or down quark, charge 1=3 universe and nowadays created in high energy physics experiments. JMF Southampton Masterclass 22–23 Mar 2004 3/26 But this is not all. The electron has a friend the electron-neutrino, ºe. Needed to ensure energy and momentum are conserved in ¯-decay: ¡ n ! p + e + º¯e Neutrino: no electric charge, (almost) no mass, hardly interacts at all.
    [Show full text]
  • Lepton Flavor and Number Conservation, and Physics Beyond the Standard Model
    Lepton Flavor and Number Conservation, and Physics Beyond the Standard Model Andr´ede Gouv^ea1 and Petr Vogel2 1 Department of Physics and Astronomy, Northwestern University, Evanston, Illinois, 60208, USA 2 Kellogg Radiation Laboratory, Caltech, Pasadena, California, 91125, USA April 1, 2013 Abstract The physics responsible for neutrino masses and lepton mixing remains unknown. More ex- perimental data are needed to constrain and guide possible generalizations of the standard model of particle physics, and reveal the mechanism behind nonzero neutrino masses. Here, the physics associated with searches for the violation of lepton-flavor conservation in charged-lepton processes and the violation of lepton-number conservation in nuclear physics processes is summarized. In the first part, several aspects of charged-lepton flavor violation are discussed, especially its sensitivity to new particles and interactions beyond the standard model of particle physics. The discussion concentrates mostly on rare processes involving muons and electrons. In the second part, the sta- tus of the conservation of total lepton number is discussed. The discussion here concentrates on current and future probes of this apparent law of Nature via searches for neutrinoless double beta decay, which is also the most sensitive probe of the potential Majorana nature of neutrinos. arXiv:1303.4097v2 [hep-ph] 29 Mar 2013 1 1 Introduction In the absence of interactions that lead to nonzero neutrino masses, the Standard Model Lagrangian is invariant under global U(1)e × U(1)µ × U(1)τ rotations of the lepton fields. In other words, if neutrinos are massless, individual lepton-flavor numbers { electron-number, muon-number, and tau-number { are expected to be conserved.
    [Show full text]
  • A Discussion on Characteristics of the Quantum Vacuum
    A Discussion on Characteristics of the Quantum Vacuum Harold \Sonny" White∗ NASA/Johnson Space Center, 2101 NASA Pkwy M/C EP411, Houston, TX (Dated: September 17, 2015) This paper will begin by considering the quantum vacuum at the cosmological scale to show that the gravitational coupling constant may be viewed as an emergent phenomenon, or rather a long wavelength consequence of the quantum vacuum. This cosmological viewpoint will be reconsidered on a microscopic scale in the presence of concentrations of \ordinary" matter to determine the impact on the energy state of the quantum vacuum. The derived relationship will be used to predict a radius of the hydrogen atom which will be compared to the Bohr radius for validation. The ramifications of this equation will be explored in the context of the predicted electron mass, the electrostatic force, and the energy density of the electric field around the hydrogen nucleus. It will finally be shown that this perturbed energy state of the quan- tum vacuum can be successfully modeled as a virtual electron-positron plasma, or the Dirac vacuum. PACS numbers: 95.30.Sf, 04.60.Bc, 95.30.Qd, 95.30.Cq, 95.36.+x I. BACKGROUND ON STANDARD MODEL OF COSMOLOGY Prior to developing the central theme of the paper, it will be useful to present the reader with an executive summary of the characteristics and mathematical relationships central to what is now commonly referred to as the standard model of Big Bang cosmology, the Friedmann-Lema^ıtre-Robertson-Walker metric. The Friedmann equations are analytic solutions of the Einstein field equations using the FLRW metric, and Equation(s) (1) show some commonly used forms that include the cosmological constant[1], Λ.
    [Show full text]
  • The Masses of the First Family of Fermions and of the Higgs Boson Are Equal to Integer Powers of 2 Nathalie Olivi-Tran
    The masses of the first family of fermions and of the Higgs boson are equal to integer powers of 2 Nathalie Olivi-Tran To cite this version: Nathalie Olivi-Tran. The masses of the first family of fermions and of the Higgs boson are equal to integer powers of 2. QCD14, S.Narison, Jun 2014, MONTPELLIER, France. pp.272-275, 10.1016/j.nuclphysbps.2015.01.057. hal-01186623 HAL Id: hal-01186623 https://hal.archives-ouvertes.fr/hal-01186623 Submitted on 27 Aug 2015 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. See discussions, stats, and author profiles for this publication at: http://www.researchgate.net/publication/273127325 The masses of the first family of fermions and of the Higgs boson are equal to integer powers of 2 ARTICLE · JANUARY 2015 DOI: 10.1016/j.nuclphysbps.2015.01.057 1 AUTHOR: Nathalie Olivi-Tran Université de Montpellier 77 PUBLICATIONS 174 CITATIONS SEE PROFILE Available from: Nathalie Olivi-Tran Retrieved on: 27 August 2015 The masses of the first family of fermions and of the Higgs boson are equal to integer powers of 2 a, Nathalie Olivi-Tran ∗ aLaboratoire Charles Coulomb, UMR CNRS 5221, cc.
    [Show full text]
  • Pion and Kaon Structure at 12 Gev Jlab and EIC
    Pion and Kaon Structure at 12 GeV JLab and EIC Tanja Horn Collaboration with Ian Cloet, Rolf Ent, Roy Holt, Thia Keppel, Kijun Park, Paul Reimer, Craig Roberts, Richard Trotta, Andres Vargas Thanks to: Yulia Furletova, Elke Aschenauer and Steve Wood INT 17-3: Spatial and Momentum Tomography 28 August - 29 September 2017, of Hadrons and Nuclei INT - University of Washington Emergence of Mass in the Standard Model LHC has NOT found the “God Particle” Slide adapted from Craig Roberts (EICUGM 2017) because the Higgs boson is NOT the origin of mass – Higgs-boson only produces a little bit of mass – Higgs-generated mass-scales explain neither the proton’s mass nor the pion’s (near-)masslessness Proton is massive, i.e. the mass-scale for strong interactions is vastly different to that of electromagnetism Pion is unnaturally light (but not massless), despite being a strongly interacting composite object built from a valence-quark and valence antiquark Kaon is also light (but not massless), heavier than the pion constituted of a light valence quark and a heavier strange antiquark The strong interaction sector of the Standard Model, i.e. QCD, is the key to understanding the origin, existence and properties of (almost) all known matter Origin of Mass of QCD’s Pseudoscalar Goldstone Modes Exact statements from QCD in terms of current quark masses due to PCAC: [Phys. Rep. 87 (1982) 77; Phys. Rev. C 56 (1997) 3369; Phys. Lett. B420 (1998) 267] 2 Pseudoscalar masses are generated dynamically – If rp ≠ 0, mp ~ √mq The mass of bound states increases as √m with the mass of the constituents In contrast, in quantum mechanical models, e.g., constituent quark models, the mass of bound states rises linearly with the mass of the constituents E.g., in models with constituent quarks Q: in the nucleon mQ ~ ⅓mN ~ 310 MeV, in the pion mQ ~ ½mp ~ 70 MeV, in the kaon (with s quark) mQ ~ 200 MeV – This is not real.
    [Show full text]
  • Lesson 1: the Single Electron Atom: Hydrogen
    Lesson 1: The Single Electron Atom: Hydrogen Irene K. Metz, Joseph W. Bennett, and Sara E. Mason (Dated: July 24, 2018) Learning Objectives: 1. Utilize quantum numbers and atomic radii information to create input files and run a single-electron calculation. 2. Learn how to read the log and report files to obtain atomic orbital information. 3. Plot the all-electron wavefunction to determine where the electron is likely to be posi- tioned relative to the nucleus. Before doing this exercise, be sure to read through the Ins and Outs of Operation document. So, what do we need to build an atom? Protons, neutrons, and electrons of course! But the mass of a proton is 1800 times greater than that of an electron. Therefore, based on de Broglie’s wave equation, the wavelength of an electron is larger when compared to that of a proton. In other words, the wave-like properties of an electron are important whereas we think of protons and neutrons as particle-like. The separation of the electron from the nucleus is called the Born-Oppenheimer approximation. So now we need the wave-like description of the Hydrogen electron. Hydrogen is the simplest atom on the periodic table and the most abundant element in the universe, and therefore the perfect starting point for atomic orbitals and energies. The compu- tational tool we are going to use is called OPIUM (silly name, right?). Before we get started, we should know what’s needed to create an input file, which OPIUM calls a parameter files. Each parameter file consist of a sequence of ”keyblocks”, containing sets of related parameters.
    [Show full text]
  • 1.1. Introduction the Phenomenon of Positron Annihilation Spectroscopy
    PRINCIPLES OF POSITRON ANNIHILATION Chapter-1 __________________________________________________________________________________________ 1.1. Introduction The phenomenon of positron annihilation spectroscopy (PAS) has been utilized as nuclear method to probe a variety of material properties as well as to research problems in solid state physics. The field of solid state investigation with positrons started in the early fifties, when it was recognized that information could be obtained about the properties of solids by studying the annihilation of a positron and an electron as given by Dumond et al. [1] and Bendetti and Roichings [2]. In particular, the discovery of the interaction of positrons with defects in crystal solids by Mckenize et al. [3] has given a strong impetus to a further elaboration of the PAS. Currently, PAS is amongst the best nuclear methods, and its most recent developments are documented in the proceedings of the latest positron annihilation conferences [4-8]. PAS is successfully applied for the investigation of electron characteristics and defect structures present in materials, magnetic structures of solids, plastic deformation at low and high temperature, and phase transformations in alloys, semiconductors, polymers, porous material, etc. Its applications extend from advanced problems of solid state physics and materials science to industrial use. It is also widely used in chemistry, biology, and medicine (e.g. locating tumors). As the process of measurement does not mostly influence the properties of the investigated sample, PAS is a non-destructive testing approach that allows the subsequent study of a sample by other methods. As experimental equipment for many applications, PAS is commercially produced and is relatively cheap, thus, increasingly more research laboratories are using PAS for basic research, diagnostics of machine parts working in hard conditions, and for characterization of high-tech materials.
    [Show full text]
  • 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 .
    [Show full text]
  • 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..
    [Show full text]
  • First Determination of the Electric Charge of the Top Quark
    First Determination of the Electric Charge of the Top Quark PER HANSSON arXiv:hep-ex/0702004v1 1 Feb 2007 Licentiate Thesis Stockholm, Sweden 2006 Licentiate Thesis First Determination of the Electric Charge of the Top Quark Per Hansson Particle and Astroparticle Physics, Department of Physics Royal Institute of Technology, SE-106 91 Stockholm, Sweden Stockholm, Sweden 2006 Cover illustration: View of a top quark pair event with an electron and four jets in the final state. Image by DØ Collaboration. Akademisk avhandling som med tillst˚and av Kungliga Tekniska H¨ogskolan i Stock- holm framl¨agges till offentlig granskning f¨or avl¨aggande av filosofie licentiatexamen fredagen den 24 november 2006 14.00 i sal FB54, AlbaNova Universitets Center, KTH Partikel- och Astropartikelfysik, Roslagstullsbacken 21, Stockholm. Avhandlingen f¨orsvaras p˚aengelska. ISBN 91-7178-493-4 TRITA-FYS 2006:69 ISSN 0280-316X ISRN KTH/FYS/--06:69--SE c Per Hansson, Oct 2006 Printed by Universitetsservice US AB 2006 Abstract In this thesis, the first determination of the electric charge of the top quark is presented using 370 pb−1 of data recorded by the DØ detector at the Fermilab Tevatron accelerator. tt¯ events are selected with one isolated electron or muon and at least four jets out of which two are b-tagged by reconstruction of a secondary decay vertex (SVT). The method is based on the discrimination between b- and ¯b-quark jets using a jet charge algorithm applied to SVT-tagged jets. A method to calibrate the jet charge algorithm with data is developed. A constrained kinematic fit is performed to associate the W bosons to the correct b-quark jets in the event and extract the top quark electric charge.
    [Show full text]
  • The Making of the Standard Theory
    August 11, 2016 9:28 The Standard Theory of Particle Physics - 9.61in x 6.69in b2471-ch02 page 29 Chapter 2 The Making of the Standard Theory John Iliopoulos Laboratoire de Physique Th´eorique, Ecole´ Normale Sup´erieure, 24 rue Lhomond, 75005 Paris, France 1. Introduction The construction of the Standard Model, which became gradually the Standard Theory of elementary particle physics, is, probably, the most remarkable achieve- ment of modern theoretical physics. In this Chapter we shall deal mostly with the weak interactions. It may sound strange that a revolution in particle physics was initiated by the study of the weakest among them (the effects of the gravitational interactions are not measurable in high energy physics), but we shall see that the weak interactions triggered many such revolutions and we shall have the occasion to meditate on the fundamental significance of “tiny” effects. We shall outline the various steps, from the early days of the Fermi theory to the recent experimental discoveries, which confirmed all the fundamental predictions of the Theory. We shall follow a phenomenological approach, in which the introduction of every new concept is motivated by the search of a consistent theory which agrees with experiment. As we shall explain, this is only part of the story, the other part being the requirement of mathematical consistency. Both went in parallel and the real history requires the understanding of both. In fact, as we intend to show, the initial motivation was not really phenomenological. It is one of these rare cases in which a revolution in physics came from theorists trying to go beyond a simple phenomenological model, The Standard Theory of Particle Physics Downloaded from www.worldscientific.com not from an experimental result which forced them to do so.
    [Show full text]