NEW ENTITIES, OLD PARADIGMS: ELEMENTARY PARTICLES in the 1930S1
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The Neutrino Theory of Light
THE NEUTRINO THEORY OF LIGHT. BY MAx BORN AND N. ~. I~AGENDRA N/kT~I. (From the Department of Physics, Indian Institute o[ Science, Bangalore.) Received March 18, 1936. 7. Introduction. TI~E most important contribution during the last years to the fundamental conceptions of theoretical physics seems to be the development of a new theory of light which contains the acknowledged one as a limiting case, but connects the optical phenomena with those of a very different kind, radio- activity. The idea that the photon is not an elementary particle but a secondary one, composed of simpler particles, has been first mentioned by p. Jordan 1. His argument was a statistical one, based on the fact, that photons satisfy the Bose-Einstein statistics. It is known from the theory of composed particles as nuclei, atoms or molecules, that this statistics may appear for such systems, which are compounds of elementary particles satisfying the Fermi-Dirac statistics (e.g., electrons or protons). After the discovery of the neutrino, de Broglie2 suggested that a photon hv is composed of a " neutrino " and an " anti-neutrino," each having the energy He has developed some interesting mathematical relations between the wave equation of a neutrino (which he assumed to be Dirac's equation for a vanish- {ngly small rest;mass) and Maxwell's field equations. But de Broglie has not touched the central problem, namely, as to how the Bose-Einstein statistics of the photons arises from the Fermi-statistics of the neutrinos. This ques- tion cannot be solved in the same way as in the cases mentioned above (material particles) Where it is a consequence of considering the composed system as a whole neglecting internal motions. -
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 -
MIT at the Large Hadron Collider—Illuminating the High-Energy Frontier
Mit at the large hadron collider—Illuminating the high-energy frontier 40 ) roland | klute mit physics annual 2010 gunther roland and Markus Klute ver the last few decades, teams of physicists and engineers O all over the globe have worked on the components for one of the most complex machines ever built: the Large Hadron Collider (LHC) at the CERN laboratory in Geneva, Switzerland. Collaborations of thousands of scientists have assembled the giant particle detectors used to examine collisions of protons and nuclei at energies never before achieved in a labo- ratory. After initial tests proved successful in late 2009, the LHC physics program was launched in March 2010. Now the race is on to fulfill the LHC’s paradoxical mission: to complete the Stan- dard Model of particle physics by detecting its last missing piece, the Higgs boson, and to discover the building blocks of a more complete theory of nature to finally replace the Standard Model. The MIT team working on the Compact Muon Solenoid (CMS) experiment at the LHC stands at the forefront of this new era of particle and nuclear physics. The High Energy Frontier Our current understanding of the fundamental interactions of nature is encap- sulated in the Standard Model of particle physics. In this theory, the multitude of subatomic particles is explained in terms of just two kinds of basic building blocks: quarks, which form protons and neutrons, and leptons, including the electron and its heavier cousins. From the three basic interactions described by the Standard Model—the strong, electroweak and gravitational forces—arise much of our understanding of the world around us, from the formation of matter in the early universe, to the energy production in the Sun, and the stability of atoms and mit physics annual 2010 roland | klute ( 41 figure 1 A photograph of the interior, central molecules. -
Elementary Particle Physics from Theory to Experiment
Elementary Particle Physics From Theory to Experiment Carlos Wagner Physics Department, EFI and KICP, Univ. of Chicago HEP Division, Argonne National Laboratory Society of Physics Students, Univ. of Chicago, Nov. 10, 2014 Particle Physics studies the smallest pieces of matter, 1 1/10.000 1/100.000 1/100.000.000 and their interactions. Friday, November 2, 2012 Forces and Particles in Nature Gravitational Force Electromagnetic Force Attractive force between 2 massive objects: Attracts particles of opposite charge k e e F = 1 2 d2 1 G = 2 MPl Forces within atoms and between atoms Proportional to product of masses + and - charges bind together Strong Force and screen each other Assumes interaction over a distance d ==> comes from properties of spaceAtoms and timeare made fromElectrons protons, interact with protons via quantum neutrons and electrons. Strong nuclear forceof binds e.m. energy together : the photons protons and neutrons to form atoms nuclei Strong nuclear force binds! togethers! =1 m! = 0 protons and neutrons to form nuclei protonD. I. S. of uuelectronsd formedwith Modeled protons by threeor by neutrons a theoryquarks, based bound on together Is very weak unless one ofneutron theat masses high energies is huge,udd shows by thatthe U(1)gluons gauge of thesymmetry strong interactions like the earth protons and neutrons SU (3) c are not fundamental Friday,p November! u u d 2, 2012 formed by three quarks, bound together by n ! u d d the gluons of the strong interactions Modeled by a theory based on SU ( 3 ) C gauge symmetry we see no free quarks Very strong at large distances confinement " in nature ! Weak Force Force Mediating particle transformations Observation of Beta decay demands a novel interaction Weak Force Short range forces exist only inside the protons 2 and neutrons, with massive force carriers: gauge bosons ! W and Z " MW d FW ! e / d Similar transformations explain the non-observation of heavier elementary particles in our everyday experience. -
Interpreted History of Neutrino Theory of Light and Its Futureprovided by CERN Document Server
View metadata, citation and similar papers at core.ac.uk brought to you by CORE Interpreted History Of Neutrino Theory Of Light And Its Futureprovided by CERN Document Server W. A. Perkins Perkins Advanced Computing Systems, 12303 Hidden Meadows Circle, Auburn, CA 95603, USA E-mail: [email protected] De Broglie's original idea that a photon is composed of a neutrino- antineutrino pair bound by some interaction was severely modified by Jor- dan. Although Jordan addressed an important problem (photon statistics) that de Broglie had not considered, his modifications may have been detri- mental to the development of a composite photon theory. His obsession with obtaining Bose statistics for the composite photon made it easy for Pryce to prove his theory untenable. Pryce also indicated that forming transversely- polarized photons from neutrino-antineutrino pairs was impossible, but oth- ers have shown that this is not a problem. Following Pryce, Berezinskii has proven that any composite photon theory (using fermions) is impossible if one accepts five assumptions. Thus, any successful composite theory must show which of Berezinskii's assumptions is not valid. A method of forming composite particles based on Fermi and Yang's model will be discussed. Such composite particles have properties similar to conventional photons. However, unlike the situation with conventional photon theory, Lorentz invariance can be satisfied without the need for gauge invariance or introducing non-physical photons. PACS numbers: 14.70.Bh,12.60.Rc,12.20.Ds I. INTRODUCTION The theoretical development of a composite photon theory (based on de Broglie’s idea that the photon is composed of a neutrino-antineutrino pair [1] bound by some interaction) has had a stormy history with many negative papers. -
The Higgs Boson in the Periodic System of Elementary Particles
Southern Adventist University KnowledgeExchange@Southern Faculty Works Physics and Engineering Department 3-2013 The iH ggs Boson in the Periodic System of Elementary Particles Ding-Yu Chung Ray Hefferlin Follow this and additional works at: https://knowledge.e.southern.edu/facworks_physics Part of the Elementary Particles and Fields and String Theory Commons Recommended Citation Chung, Ding-Yu and Hefferlin, Ray, "The iH ggs Boson in the Periodic System of Elementary Particles" (2013). Faculty Works. 12. https://knowledge.e.southern.edu/facworks_physics/12 This Article is brought to you for free and open access by the Physics and Engineering Department at KnowledgeExchange@Southern. It has been accepted for inclusion in Faculty Works by an authorized administrator of KnowledgeExchange@Southern. For more information, please contact [email protected]. Journal of Modern Physics, 2013, 4, 21-26 doi:10.4236/jmp.2013.44A004 Published Online April 2013 (http://www.scirp.org/journal/jmp) The Higgs Boson in the Periodic System of Elementary Particles Ding-Yu Chung1, Ray Hefferlin2 1Utica, Michigan, USA 2Department of Physics, Southern Adventist University, Collegedale, USA Email: [email protected], [email protected] Received February 12, 2013; revised March 15, 2013; accepted March 27, 2013 Copyright © 2013 Ding-Yu Chung, Ray Hefferlin. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. ABSTRACT It is proposed that the observed Higgs Boson at the LHC is the Standard Model Higgs boson that adopts the existence of the hidden lepton condensate. The hidden lepton is in the forbidden lepton family, outside of the three lepton families of the Standard Model. -
New Elementary Particle Evidence Found, 'Sterile Neutrino' Long
New elementary particle evidence found, ‘sterile neutrino’ long suspected June 6, 2018 Los Alamos experiment at Fermilab explores potential ‘dark matter’ link, confirms earlier experiment LOS ALAMOS, N.M., June 6, 2018—New research results have potentially identified a fourth type of neutrino, a “sterile neutrino” particle. This particle provides challenges for the Standard Model of particle physics, if found to be a valid result in future experiments. The work, conducted by a multi-institutional team at Fermi National Accelerator Laboratory (Fermilab) near Chicago, confirms results found in the 1990s in the Los Alamos Liquid Scintillator Neutrino Detector (LSND). “This is a fascinating step forward for particle physics,” said Los Alamos National Laboratory Director Terry Wallace. “Of course, this needs to be tempered by #the fact that future observations are required to really clinch this beyond any shadow of doubt. Modifications to the Standard Model, including dark matter, new particles and other interpretations of this result are still speculative. What stands with high confidence is that two experiments with completely different approaches observe the same effect.” 1:22 The Sterile Neutrino Discovery Neutrinos, traditionally understood to come in three “flavors,” electron, muon and tau, have been measured by the Mini Booster Neutrino Experiment (MiniBooNE) for some 15 years. The key to the current result is the existence of more electron-flavored neutrinos than expected. Neutrinos normally oscillate between the three types, but the overpopulation of the electron-flavored ones leads to a theory that some of the muon neutrinos became sterile neutrinos for a time during the regular oscillations. The sterile neutrinos could reasonably be assumed to have transitioned into electron neutrinos in their next oscillation phase, thus explaining the higher electron numbers. -
Supersymmetry: What? Why? When?
Contemporary Physics, 2000, volume41, number6, pages359± 367 Supersymmetry:what? why? when? GORDON L. KANE This article is acolloquium-level review of the idea of supersymmetry and why so many physicists expect it to soon be amajor discovery in particle physics. Supersymmetry is the hypothesis, for which there is indirect evidence, that the underlying laws of nature are symmetric between matter particles (fermions) such as electrons and quarks, and force particles (bosons) such as photons and gluons. 1. Introduction (B) In addition, there are anumber of questions we The Standard Model of particle physics [1] is aremarkably hope will be answered: successful description of the basic constituents of matter (i) Can the forces of nature be uni® ed and (quarks and leptons), and of the interactions (weak, simpli® ed so wedo not have four indepen- electromagnetic, and strong) that lead to the structure dent ones? and complexity of our world (when combined with gravity). (ii) Why is the symmetry group of the Standard It is afull relativistic quantum ®eld theory. It is now very Model SU(3) ´SU(2) ´U(1)? well tested and established. Many experiments con® rmits (iii) Why are there three families of quarks and predictions and none disagree with them. leptons? Nevertheless, weexpect the Standard Model to be (iv) Why do the quarks and leptons have the extendedÐ not wrong, but extended, much as Maxwell’s masses they do? equation are extended to be apart of the Standard Model. (v) Can wehave aquantum theory of gravity? There are two sorts of reasons why weexpect the Standard (vi) Why is the cosmological constant much Model to be extended. -
B Meson Decays Marina Artuso1, Elisabetta Barberio2 and Sheldon Stone*1
Review Open Access B meson decays Marina Artuso1, Elisabetta Barberio2 and Sheldon Stone*1 Address: 1Department of Physics, Syracuse University, Syracuse, NY 13244, USA and 2School of Physics, University of Melbourne, Victoria 3010, Australia Email: Marina Artuso - [email protected]; Elisabetta Barberio - [email protected]; Sheldon Stone* - [email protected] * Corresponding author Published: 20 February 2009 Received: 20 February 2009 Accepted: 20 February 2009 PMC Physics A 2009, 3:3 doi:10.1186/1754-0410-3-3 This article is available from: http://www.physmathcentral.com/1754-0410/3/3 © 2009 Stone et al This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/ licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. Abstract We discuss the most important Physics thus far extracted from studies of B meson decays. Measurements of the four CP violating angles accessible in B decay are reviewed as well as direct CP violation. A detailed discussion of the measurements of the CKM elements Vcb and Vub from semileptonic decays is given, and the differences between resulting values using inclusive decays versus exclusive decays is discussed. Measurements of "rare" decays are also reviewed. We point out where CP violating and rare decays could lead to observations of physics beyond that of the Standard Model in future experiments. If such physics is found by directly observation of new particles, e.g. in LHC experiments, B decays can play a decisive role in interpreting the nature of these particles. -
A Conjectural Preon Theory and Its Implications
A Conjectural Preon Theory and its Implications Rupert Gerritsen Copyright © - Rupert Gerritsen Batavia Online Publishing A Conjectural Preon Theory and its Implications Batavia Online Publishing Canberra, Australia Published by Batavia Online Publishing 2012 Copyright © Rupert Gerritsen National Library of Australia Cataloguing-in-Publication Data Author: Gerritsen, Rupert, 1953- Title: A Conjectural Preon Theory ISBN: 978-0-9872141-5-7 (pbk.) Notes: Includes bibliographic references Subjects: Particles (Nuclear physics) Dewey Number: 539.72 Copyright © - Rupert Gerritsen 1 A Conjectural Preon Theory and its Implications At present the dominant paradigm in particle physics is the Standard Model. This theory has taken hold over the last 30 years as its predictions of new particles have been dramatically borne out in increasingly sophisticated experiments. Despite this it would seem that the Standard Model has some shortcomings and leaves a number of questions unanswered. The number of arbitrary constants and parameters incorporated in the Model is one unsatisfactory aspect, as is its inability to explain the masses of the quarks and leptons. Another problematic area often cited is the Model’s failure to account for the number of generations of quarks and leptons. The plethora of “fundamental” particles also appears to represent a major weakness in the Standard Model. There are 16 “fundamental” or “elementary” particles, as well as their anti-particles, engendered in the Standard Model, along with 8 types of gluons. This difficulty may be further compounded by theorizing based on supersymmetry, as an extension of the Standard Model, because it requires heavier twins for the known particles. Furthermore the Higgs mechanism, postulated to generate mass in particles, has not as yet been validated experimentally. -
Birth of the Neutrino, from Pauli to the Reines-Cowan Experiment 1
Birth of the neutrino, from Pauli to the Reines-Cowan experiment C. Jarlskog Division of Mathematical Physics, LTH, Lund University Box 118, S-22100 Lund, Sweden Fifty years after the introduction of the neutrino hypothesis, Bruno Pontecorvo praised its inventor stating 1: \It is difficult to find a case where the word \intuition" characterizes a human achievement better than in the case of the neutrino invention by Pauli". The neutrino a hypothesis generated a huge amount of excitement in physics. Several hundred papers were written about the neutrino before its discovery in the Reines-Cowan experiment. My task here is to share some of that excitement with you. 1 Introduction I would like to start by expressing my gratitude to the organizers for having invited me to give this talk. Indeed I am \Super Glad" to be here because of a very special reason. A few years ago I produced a book in honor of my supervisor Professor Gunnar K¨all´en (1926-1968) 2. Because I lacked the necessary experience, it took me about three years to produce the book. First I had to locate K¨all´en'sscholarly belongings, among them his scientific correspondence. Due to tragic events that took place after his death, the search took some time. Eventually, I found 18 boxes which had been deposited at the Manuscripts & Archives section of the Lund University's Central Library. To my great surprise, this “K¨all´enCollection" contained about 160 letters exchanged between him and Pauli - almost all in German. After Pauli's death in 1958 his widow Franziska (called Franka) collected his scientific belongings and donated them to CERN and not to ETH in Z¨urich, where Pauli had been a professor since 1928, i.e., for 30 years. -
Supersymmetry
Supersymmetry Physics Colloquium University of Virginia January 28, 2011 Stephen P. Martin Northern Illinois University 1 The Standard Model of particle physics • The “Hierarchy Problem”: why is the Higgs mass so • small? Supersymmetry as a solution • New particles predicted by supersymmetry • Supersymmetry is spontaneously broken • How to find supersymmetry • 2 The Standard Model of Particle Physics Quarks (spin=1/2): Name: down up strange charm bottom top − 1 2 − 1 2 − 1 2 Charge: 3 3 3 3 3 3 Mass: 0.005 0.002 0.1 1.5 5 173.1 Leptons (spin=1/2): − − − Name: e νe µ νµ τ ντ Charge: −1 0 −1 0 −1 0 Mass: 0.000511 ∼ 0 0.106 ∼ 0 1.777 ∼ 0 Gauge bosons (spin=1): ± 0 Name: photon (γ) W Z gluon (g) Charge: 0 ±1 0 0 Mass: 0 80.4 91.2 0 All masses in GeV. (Proton mass = 0.938 GeV.) Not shown: antiparticles of quarks, leptons. 3 There is a last remaining undiscovered fundamental particle in the Standard Model: the Higgs boson. What we know about it: Charge: 0 Spin: 0 Mass: Greaterthan 114 GeV, and not between 158 and 175 GeV ( in most simple versions) Less than about 215 GeV ( indirect, very fuzzy, simplest model only) Fine print: There might be more than one Higgs boson. Or, it might be a composite particle, made of other more basic objects. Or, it might be an “effective” phenomenon, described more fundamentally by other unknown physics. But it must exist in some form, because... 4 The Higgs boson is the source of all mass.