Elementary Particle
Total Page:16
File Type:pdf, Size:1020Kb
Load more
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. -
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. -
Associated Charged Higgs Boson and Squark Production in the NUHM Model
UPTEC F10 010 Examensarbete 30 hp Februari 2010 Associated charged Higgs boson and squark production in the NUHM model Gustav Lund Abstract Associated charged Higgs boson and squark production in the NUHM model Gustav Lund Teknisk- naturvetenskaplig fakultet UTH-enheten Conventional searches for the charged Higgs boson using its production in association with Standard Model (SM) quarks is notoriously weak in the mid-tanB range. Hoping Besöksadress: to find an alternate channel to fill this gap, the production of the charged Higgs boson Ångströmlaboratoriet Lägerhyddsvägen 1 in association with supersymmetric squarks is studied. Using Monte Carlo generators Hus 4, Plan 0 the production at the LHC is simulated within the non universal Higgs mass model (NUHM). If the six parameters of the model (m0, m1/2, A0, tanB, u, mA) induce small Postadress: masses of the stop, sbottom and charged Higgs, the production cross section can be Box 536 751 21 Uppsala of the order pb. Through scans of the input parameter the cross section is maximized, with the requirement that the stop decays directly to a neutralino - Telefon: simplifying detection, in the point (m0, m1/2, A0, tanB, u, mA) = (190, 187, -1147, 018 – 471 30 03 179, 745, 13.2) where the cross section is 559 fb. Telefax: 018 – 471 30 00 The production is compared to the irreducible backgrounds stop, stop, t, tbar and t, tbar + 2 jets. The former poses no severe constraints and can be easily removed Hemsida: using appropriate cuts. The latter, SM background, has a cross section almost 1000 http://www.teknat.uu.se/student times larger and strong cuts must be imposed to suppress it. -
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. -
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. -
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. -
Do About Half the Top Quarks at FNAL Come from Gluino Decays?
ANL–HEP–PR–96–43 UM–TH–96–06 May 1996 Do About Half the Top Quarks at FNAL Come From Gluino Decays? G. L. Kane† Randall Laboratory of Physics University of Michigan Ann Arbor, MI 48104 and S. Mrenna‡ High Energy Physics Division Argonne National Laboratory Argonne, IL 60439 Abstract We argue that it is possible to make a consistent picture of FNAL data including the production and decay of gluinos and squarks. The additional cross section is several pb, about the size of that for Standard Model (SM) top quark pair production. If the stop squark mass is small enough, about half of the top quarks decay to stop squarks, and the loss of SM top quark pair production rate is compensated by the supersymmet- ric processes. This behavior is consistent with the reported top quark decay rates in various modes and other aspects of the data, and suggests several other possible decay signatures. This picture can be tested easily with more data, perhaps even with the data in hand, and demonstrates the potential power of a hadron collider to determine supersymmetric parameters. It also has implications for the top mass measurement and the interpretation of the LEP Rb excess. PAC codes: 12.60.Jv, 12.15.Mm, 14.65.Ha, 14.80.L †[email protected] ‡[email protected] 1 Introduction While there is still no compelling experimental evidence that nature is supersymmetric on the weak scale, there have been recent reports of data that encourage this view. The most explicit is an event in CDF [1] that does not have a probable SM interpretation, and can naturally be explained as selectron pair production[2, 3]. -
Two Tests of New Physics Using Top Quarks at the CMS Experiment
UC San Diego UC San Diego Electronic Theses and Dissertations Title Two Tests of New Physics Using Top Quarks at the CMS Experiment Permalink https://escholarship.org/uc/item/4118h880 Author Klein, Daniel Publication Date 2018 Peer reviewed|Thesis/dissertation eScholarship.org Powered by the California Digital Library University of California UNIVERSITY OF CALIFORNIA SAN DIEGO Two Tests of New Physics Using Top Quarks at the CMS Experiment A dissertation submitted in partial satisfaction of the requirements for the degree Doctor of Philosophy in Physics by Daniel Stuart Klein Committee in charge: Professor Frank Wurthwein,¨ Chair Professor Avraham Yagil, Co-Chair Professor Rommie Amaro Professor Pamela Cosman Professor Benjam´ın Grinstein 2018 Copyright Daniel Stuart Klein, 2018 All rights reserved. The dissertation of Daniel Stuart Klein is approved, and it is acceptable in quality and form for publication on microfilm and electronically: Co-Chair Chair University of California San Diego 2018 iii DEDICATION This dissertation is dedicated to the memory of my grandmother, Dr. Isabelle Rapin (1927-2017). To everyone else, a titan of pediatric neurology. To me, one of my staunchest supporters. iv EPIGRAPH Now you see why your father and I call it ’gradual school’. —Mom v TABLE OF CONTENTS Signature Page....................................... iii Dedication.......................................... iv Epigraph...........................................v Table of Contents...................................... vi List of Figures....................................... -
Introduction to Elementary Particle Physics
Introduction to Elementary Particle Physics Joachim Meyer DESY Lectures DESY Summer Student Program 2009 Preface ● This lecture is not a powerpoint show ● This lecture does not substitute an university course ● I know that your knowledge about the topic varies a lot ● So we have to make compromises in simplicity and depth ● Still I hope that all of you may profit somehow ● The viewgraphs shown are only for illustrations ● We will develop things together in discussion and at blackboard ● I hope there are lots of questions. I shall ask you a lot 2 Structures at different sizes Elementary Particle Physics 3 3 Fermion Generations Interactions through Gauge Boson Exchange This lecture is going to tell you something about HOW we arrived at this picture 4 Content of this lectures . Its only a sketch : Depending on your preknowledge we will go more or less in detail in the different subjects 5 6 WHY High Energies ? 7 The very basic minimum you have to know about Relativistic Kinematics 8 Which CM-energy do we reach at HERA ? 9 HEP 100 Years ago : Radioactive Decay Energy region : MeV =He−nucleus....=electron...= photon 10 Today : Some more particles : 11 The Particle Zoo I can't spare you this chapter. Quarks are nice to EXPLAIN observed phenomena. But, what we OBSERVE are particles like protons, muons, pions,.......... 12 'Artificial' Production of New Particles (Resonances): − p scattering 13 Particle classification Hadrons : strongly interacting Leptons : not Strongly interacting 14 All these particles are listed in the Particle Data Booklet -
Fermilab Today
Fermilab Today Thursday, March 5, 2009 Calendar Feature Fermilab Result of the Week Thursday, March 5 Public lecture opportunity: Fact You can’t top stop 11 a.m. or fiction? The science behind Presentations to the Physics Search, search, search for squarks, They’re what we’d like to see, Advisory Committee - Curia II "Angels and Demons" And so we hunt and hunt and hunt for 11 a.m. Supersymmetry… Theoretical Physics Seminar - - To the tune of “Row, row, row your boat” One West (NOTE TIME and LOCATION) Speaker: Spencer Chang, University of California, Davis Title: Discovering Nonstandard Dark Matter THERE WILL BE NO PHYSICS AND DETECTOR SEMINAR THIS WEEK 3:30 p.m. DIRECTOR'S COFFEE BREAK - 2nd Flr X-Over "Angels & Demons" actors Tom Hanks and Ayelet Zurer with film director Ron Howard stand in front 4 p.m. of the Globe at CERN. DZero scientists used several variables to look for Accelerator Physics and the presence of a stop squark signal. In this plot, Technology Seminar - One It’s not every day that a major motion picture the distribution of reconstructed top quark mass for West places particle physics in the spotlight. events in which top quarks were made (red), stop Speaker: Aida Todri, University squarks were made (blue) and unrelated of California, Santa Barbara But this May, Sony Pictures will release background (green) are compared to data. “Angels and Demons,” an action-packed Title: Power Network Supersymmetry is a scientific principle Distribution for IC Designs and thriller based on Dan Brown’s best-selling novel, which focuses on an apparent plot to proposed as a likely extension of the Standard Its Challenges in Deep Model. -
Supersymmetric Particle Searches
Citation: K.A. Olive et al. (Particle Data Group), Chin. Phys. C38, 090001 (2014) (URL: http://pdg.lbl.gov) Supersymmetric Particle Searches A REVIEW GOES HERE – Check our WWW List of Reviews A REVIEW GOES HERE – Check our WWW List of Reviews SUPERSYMMETRIC MODEL ASSUMPTIONS The exclusion of particle masses within a mass range (m1, m2) will be denoted with the notation “none m m ” in the VALUE column of the 1− 2 following Listings. The latest unpublished results are described in the “Supersymmetry: Experiment” review. A REVIEW GOES HERE – Check our WWW List of Reviews CONTENTS: χ0 (Lightest Neutralino) Mass Limit 1 e Accelerator limits for stable χ0 − 1 Bounds on χ0 from dark mattere searches − 1 χ0-p elastice cross section − 1 eSpin-dependent interactions Spin-independent interactions Other bounds on χ0 from astrophysics and cosmology − 1 Unstable χ0 (Lighteste Neutralino) Mass Limit − 1 χ0, χ0, χ0 (Neutralinos)e Mass Limits 2 3 4 χe ,eχ e(Charginos) Mass Limits 1± 2± Long-livede e χ± (Chargino) Mass Limits ν (Sneutrino)e Mass Limit Chargede Sleptons e (Selectron) Mass Limit − µ (Smuon) Mass Limit − e τ (Stau) Mass Limit − e Degenerate Charged Sleptons − e ℓ (Slepton) Mass Limit − q (Squark)e Mass Limit Long-livede q (Squark) Mass Limit b (Sbottom)e Mass Limit te (Stop) Mass Limit eHeavy g (Gluino) Mass Limit Long-lived/lighte g (Gluino) Mass Limit Light G (Gravitino)e Mass Limits from Collider Experiments Supersymmetrye Miscellaneous Results HTTP://PDG.LBL.GOV Page1 Created: 8/21/2014 12:57 Citation: K.A. Olive et al. -
Search for Long-Lived Stopped R-Hadrons Decaying out of Time with Pp Collisions Using the ATLAS Detector
PHYSICAL REVIEW D 88, 112003 (2013) Search for long-lived stopped R-hadrons decaying out of time with pp collisions using the ATLAS detector G. Aad et al.* (ATLAS Collaboration) (Received 24 October 2013; published 3 December 2013) An updated search is performed for gluino, top squark, or bottom squark R-hadrons that have come to rest within the ATLAS calorimeter, and decay at some later time to hadronic jets and a neutralino, using 5.0 and 22:9fbÀ1 of pp collisions at 7 and 8 TeV, respectively. Candidate decay events are triggered in selected empty bunch crossings of the LHC in order to remove pp collision backgrounds. Selections based on jet shape and muon system activity are applied to discriminate signal events from cosmic ray and beam-halo muon backgrounds. In the absence of an excess of events, improved limits are set on gluino, stop, and sbottom masses for different decays, lifetimes, and neutralino masses. With a neutralino of mass 100 GeV, the analysis excludes gluinos with mass below 832 GeV (with an expected lower limit of 731 GeV), for a gluino lifetime between 10 s and 1000 s in the generic R-hadron model with equal branching ratios for decays to qq~0 and g~0. Under the same assumptions for the neutralino mass and squark lifetime, top squarks and bottom squarks in the Regge R-hadron model are excluded with masses below 379 and 344 GeV, respectively. DOI: 10.1103/PhysRevD.88.112003 PACS numbers: 14.80.Ly R-hadrons may change their properties through strong I.