The Investigation of Fundamental Interactions with Cold Neutrons
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Michelson–Morley Experiment
Michelson–Morley experiment Figure 1. Michelson and Morley's interferometric setup, mounted on a stone slab that floats in an annular trough of mercury The Michelson–Morley experiment was an attempt to detect the existence of the luminiferous aether, a supposed medium permeating space that was thought to be the carrier of light waves. The experiment was performed between April and July 1887 by Albert A. Michelson and Edward W. Morley at what is now Case Western Reserve University in Cleveland, Ohio, and published in November of the same year.[1] It compared the speed of light in perpendicular directions in an attempt to detect the relative motion of matter through the stationary luminiferous aether ("aether wind"). The result was negative, in that Michelson and Morley found no significant difference between the speed of light in the direction of movement through the presumed aether, and the speed at right angles. This result is generally considered to be the first strong evidence against the then-prevalent aether theory, and initiated a line of research that eventually led to special relativity, which rules out a stationary aether.[A 1] Of this experiment, Einstein wrote, "If the Michelson–Morley experiment had not brought us into serious embarrassment, no one would have regarded the relativity theory as a (halfway) redemption."[A 2]:219 Michelson–Morley type experiments have been repeated many times with steadily increasing sensitivity. These include experiments from 1902 to 1905, and a series of experiments in the 1920s. More recent optical -
Implementation of the Fizeau Aether Drag Experiment for An
Implementation of the Fizeau Aether Drag Experiment for an Undergraduate Physics Laboratory by Bahrudin Trbalic Submitted to the Department of Physics in partial fulfillment of the requirements for the degree of Bachelor of Science in Physics at the MASSACHUSETTS INSTITUTE OF TECHNOLOGY May 2020 c Massachusetts Institute of Technology 2020. All rights reserved. ○ Author................................................................ Department of Physics May 8, 2020 Certified by. Sean P. Robinson Lecturer of Physics Thesis Supervisor Certified by. Joseph A. Formaggio Professor of Physics Thesis Supervisor Accepted by . Nergis Mavalvala Associate Department Head, Department of Physics 2 Implementation of the Fizeau Aether Drag Experiment for an Undergraduate Physics Laboratory by Bahrudin Trbalic Submitted to the Department of Physics on May 8, 2020, in partial fulfillment of the requirements for the degree of Bachelor of Science in Physics Abstract This work presents the description and implementation of the historically significant Fizeau aether drag experiment in an undergraduate physics laboratory setting. The implementation is optimized to be inexpensive and reproducible in laboratories that aim to educate students in experimental physics. A detailed list of materials, experi- mental setup, and procedures is given. Additionally, a laboratory manual, preparatory materials, and solutions are included. Thesis Supervisor: Sean P. Robinson Title: Lecturer of Physics Thesis Supervisor: Joseph A. Formaggio Title: Professor of Physics 3 4 Acknowledgments I gratefully acknowledge the instrumental help of Prof. Joseph Formaggio and Dr. Sean P. Robinson for the guidance in this thesis work and in my academic life. The Experimental Physics Lab (J-Lab) has been the pinnacle of my MIT experience and I’m thankful for the time spent there. -
Michou Interferometer
July 21st 2016 Michou interferometer Costel Munteanu Montreal, QC, Canada [email protected] Abstract: The speed of light c defined as a constant of nature is in fact the “twoway speed of light” calculated from the measured time of travel of light from a light source to a reflector and back to a detector situated next to the source. In a “twoway” experiment (like FizeauFoucault apparatus) the constant c is the harmonic mean of “forward” and “backward” speeds [13]. A simple MichelsonMorley interferometer with equal length arms detects a difference between the time of travel of light along its two perpendicular arms in certain frames of reference in motion or in gravitational field and this is interpreted as Lorentz–FitzGerald contraction of length in the direction of motion or along the gradient of gravitational field [5]. While no experiment seemed to allow the precise “oneway” measurement of speed of light, LorentzFitzGerald length contraction interpretation is preferred. In this article I present an interferometer that determines the difference between “forward” and “backward” speed of light in certain frames of reference the anisotropy of speed of light along one direction showing a flow of electromagnetic medium through the frame of reference of the device contradicting the LorentzFitzGerald length contraction hypothesis and bring proof for the first time of (local) preferred frame effects. The device determines the direction of the flow and allows to calculate the velocity of that flow using the measured (or calculated) value of canonical “twoway” speed of light c in that particular frame of reference and the anisotropy measured by the device presented herein. -
Search for the Process E+E−→Η′(958) with the CMD-3 Detector
Physics Letters B 740 (2015) 273–277 Contents lists available at ScienceDirect Physics Letters B www.elsevier.com/locate/physletb + − Search for the process e e → η (958) with the CMD-3 detector R.R. Akhmetshin a,b, A.V. Anisenkov a,b, V.M. Aulchenko a,b, V.Sh. Banzarov a, N.S. Bashtovoy a, D.E. Berkaev a,b, A.E. Bondar a,b, A.V. Bragin a, S.I. Eidelman a,b, D.A. Epifanov a,e, L.B. Epshteyn a,c, A.L. Erofeev a, G.V. Fedotovich a,b, S.E. Gayazov a,b, A.A. Grebenuk a,b, D.N. Grigoriev a,b,c, E.N. Gromov a, F.V. Ignatov a,b, S.V. Karpov a, V.F. Kazanin a,b, B.I. Khazin a,b,1, I.A. Koop a,b, O.A. Kovalenko a,b, A.N. Kozyrev a, E.A. Kozyrev a,b, P.P. Krokovny a,b, A.E. Kuzmenko a,b, A.S. Kuzmin a,b, I.B. Logashenko a,b, P.A. Lukin a,b, K.Yu. Mikhailov a, N.Yu. Muchnoi a,b, V.S. Okhapkin a, Yu.N. Pestov a, E.A. Perevedentsev a,b, A.S. Popov a,b, G.P. Razuvaev a,b, Yu.A. Rogovsky a, A.L. Romanov a, A.A. Ruban a, N.M. Ryskulov a, A.E. Ryzhenenkov a,b, V.E. Shebalin a,b, D.N. Shemyakin a,b, B.A. Shwartz a,b, D.B. Shwartz a,b, A.L. Sibidanov a,d, P.Yu. Shatunov a, Yu.M. -
The Fizeau Experiment – the Experiment That Led Physics the Wrong Path for One Century
The Fizeau Experiment – the Experiment that Led Physics the Wrong Path for One Century Henok Tadesse, Electrical Engineer, BSc. Ethiopia, Debrezeit, P.O Box 412 Mobile: +251 910 751339; email: [email protected] or [email protected] 01December 2017 Abstract Although Fresnel's ether drag coefficient was ad hoc, its curious confirmation by the Fizeau experiment forced physicists to accept and adopt it as the main guide in the development of theories of the speed of light. Lorentz's 'local-time' , which evolved into the Lorentz transformations, was developed to explain the Fizeau experiment and stellar aberration. Given the logical, theoretical and experimental counter- evidences against the theory of relativity today, it turns out that the Fresnel's drag coefficient may not exist at all. The Fizeau experiment and the phenomenon of stellar aberration have no common physical basis. The result of the Fizeau experiment can be explained in a simple, classical way. It is as if nature conspired to lead physicists astray for more than one century. Alternative theories and interpretations for the ether drift experiments and invariance of Maxwell's equations will be proposed. Physicists rightly assumed the invariance of Maxwell's equations, but their deeply flawed conception of light as ordinary local phenomenon led them unnecessarily to seek an 'explanation' for this invariance, which was the Lorentz transformation. Einstein went down the wrong path when he sought an 'explanation' for the light postulate, when none was needed. The invariance of Maxwell's equations for light is a direct consequence of non-existence of the ether and there is no explanation for it for the same reason that there is no explanation for light being a wave when there is no medium for its propagation. -
Summary of the Second Workshop on Liquid Argon Time Projection Chamber Research and Development in the United States
FERMILAB-CONF-15-149-ND Preprint typeset in JINST style - HYPER VERSION Summary of the Second Workshop on Liquid Argon Time Projection Chamber Research and Development in the United States R. Acciarria, M. Adamowskia, D. Artripb, B. Ballera, C. Brombergc, F. Cavannaa;d, B. Carlsa, H. Chene, G. Deptucha, L. Epprecht f , R. Dharmapalang W. Foremanh A. Hahna, M. Johnsona, B. J. P. Jones i, T. Junka, K. Lang j, S. Lockwitza, A. Marchionnia, C. Maugerk, C. Montanaril, S. Mufsonm, M. Nessin, H. Olling Backo, G. Petrillop, S. Pordesa, J. Raafa, B. Rebela, G. Sininsk, M. Soderberga;q, N. Spoonerr, M. Stancaria, T. Strausss, K. Teraot , C. Thorne, T. Topea, M. Toupsi, J. Urheimm, R. Van de Waterk, H. Wangu, R. Wassermanv, M. Webers, D. Whittingtonm, T. Yanga aFermi National Accelerator Laboratory, Batavia, IL 60510, USA bResearch Catalytics, USA cMichigan State University, East Lansing, MI 48824, USA dYale University, New Haven, CT 06520, USA eBrookhaven National Laboratory, Upton, NY 11973, USA f ETH Zürich, 8092 Zürich, Switzerland gArgonne National Laboratory, Argonne, IL, 60439, USA hUniversity of Chicago, Chicago, IL 60637, USA iMassachusetts Institute of Technology, Cambridge, MA 02139, USA jUniversity of Texas at Austin, TX 78712, USA kLos Alamos National Laboratory, Los Alamos, NM 87545, USA lIstituto Nazionale di Fisica Nucleare, Pavia 6-27100, Italy mIndiana University, Bloomington, IN 47405, USA nCERN, 1217 Meyrin, Switzerland oPrinceton University, Princeton, NJ 08544, USA pUniversity of Rochester, Rochester, NY 14627, USA qSyracuse University, NY 13210, USA rUniversity of Sheffield, Sheffield, South Yorkshire S10 2TN, UK sUniversity of Bern, 3012 Bern, Switzerland t Columbia University, New York, NY 10027, USA uUniversity of California Los Angeles, Los Angeles, CA 90095, USA vColorado State University, Fort Collins, CO 80523, USA – 1 – Operated by Fermi Research Alliance, LLC under Contract No. -
Iw F'tf- 1 -I ÛG 0 Zi
w^. m.-m?^iw f'tf- 1 -I ÛG 0 Zi Tt;: ANOMALOUS KAGNETiC i-'.OMEKT OF THE MUOM : A REVIEW DF THE THEORETICAL CONTRIBUTIONS j. CUV.ET*, S. NARISON**, H. PERROTTET* and E. de RAFAEL14 ABSTRACT : we review the possible contributions to the muon g-factor anomaly, o^ = — t^ -Z) which arc potentially significant for a comparison between theory .^nd experiment at present. This includes purely ÇF.D perturbation theory effects up to eighth-order ; hadronic effects at fourth end sixth-order ; and weak interaction effects. From these sources we'get a total theoretical contribution O-.JTheory) = (1 155 920.6 ± 12.9) x 10"9 , to be cc.'pared with the latest CERK expc-rinental result £l] , a- (Experiment) <= (1 !G5 895 ± 27) x 10"9 . J'JNE 1«6 76/P.333 K Zïr.*.rz de Pnysique Théorique, CNRS Marseille. *" Boursier de la CEE (Coir.r.unautè Economique Européenne) Postal Address : Centre de r'nysique Théorique - uiRS 31, C'.OT.ir, -'cseph Aiguicr P-Wfc- i - INTRODUCTION The latest published value of the anomalous magnetic cornent of the rcuon ir&ccured by the CCRN \-\uor. Storage Ring Collaboration [ll is The accuracy of this rce a s urcr.G nt represents an improvement by an order of magnitude with respect to tne previous result '. Since then, the Ci'\\ tfuon Storage Ring has been in operation for a certain time and o still further improvement in the accuracy is soon expected. At this level of precision there are contributions to <*• ^ , other than those gevernce uy the quantum electrodynamics of nuons ar.d electrons (Gr-D), like hadronic effects and possibly weak interaction effects, 21 which play an important role '. -
Neutron-Deuteron Scattering and Three-Body Interactions
Digital Comprehensive Summaries of Uppsala Dissertations from the Faculty of Science and Technology 163 Neutron-Deuteron Scattering and Three-Body Interactions PHILIPPE MERMOD ACTA UNIVERSITATIS UPSALIENSIS ISSN 1651-6214 UPPSALA ISBN 91-554-6514-5 2006 urn:nbn:se:uu:diva-6739 ! " #$ #%%& '( ) * * * + , - . / , " +, #%%&, 0 1 2 -13 4 , 50 1 -6 6 7, 8 , &', 9 $# , , 4230 : 1))$1&) $1), 1 ** * 1 :) "; , - 1 ** . * . < * 1 , -. 1 . "//= 2>808 * - 2 , - ** * * . * , - * * . "//= . , 4 1 . 6. 2>808 . ?, @ . * . 2>808 . ? . . . 1 6 , / * 1 . * ** . * ** . ** < * , - . @ 1 . 1 , - ** * 1 * ** '%A * , - . * 1 * ** , 1 * @ ? ! " # $" % & '('" " )*+',(- " B + " #%%& 4220 &) 1&# $ 4230 : 1))$1&) $1) ( ((( 1&C': 5 (DD ,6,D E F ( ((( 1&C':7 To Kristina List of Papers This thesis is based on the following papers, which are referred to in the text by their Roman numerals. I J. Klug, J. Blomgren, A. Ataç, B. Bergenwall, A. Hildebrand, C. Johansson, P. Mermod, L. Nilsson, S. Pomp, U. Tippawan, K. Elmgren, N. Olsson, O. Jonsson, A.V. Prokofiev, P.-U. Renberg, P. Nadel-Turonski, -
Critique of Special Relativity (Prp-1)
CRITIQUE OF SPECIAL RELATIVITY (PRP-1) INTRODUCTION In 1887 Michelson and Morley attempted to measure the ether drift caused by the motion of the earth (at 30 km/s) in its orbit around the sun. The null result surprised everybody and for 18 years physicists tried unsuccessfully to explain the enigma. Finally, in 1905, Einstein published his revolutionary Special Theory of Relativity (STR) which rejected the ether and was quite controversial. It survived because a better solution has never been found. This may now gradually be changing. The present “Critique of Special Relativity” (PRP-1) is the first in a series of papers about “Post-Relativity Physics” (PRP). It is organized in 3 parts: Part I discusses alternative solutions in PRP for experiments and observation explained by STR. Part II discusses false arguments in favor of Special Relativity. It shows how the Sagnac effect and the GPS system have a natural explanation in classical physics, thus eliminating the need for alternative explanations in Relativity. In addition it shows that the proposed alternatives cannot work due to a fundamental flaw in Special Relativity so that the Sagnac effect and the GPS system actually disprove Relativity. Part III discusses experiments and observations which clearly disprove Special Relativity. PART I - ALTERNATIVE SOLUTIONS IN PRP FOR EXPERIMENTS EXPLAINED IN STR 1. THE ASSUMPTION OF ATOMIC RESONANCE CONTRACTION (ARC) Atomic Resonance Contraction (ARC) is a surprisingly simple alternative to STR’s kinematics. If we assume that atoms and therefore all solid objects contract by a factor 1/γ 2 in the direction of motion through the ether and by a factor 1/γ perpendicular to that motion (where γ = 1/(1-β2)1/2 with β = vc/ ) most ether drift experiments can easily be explained in classical physics. -
Chapter 15 Β Decay
Chapter 15 β Decay Note to students and other readers: This Chapter is intended to supplement Chapter 9 of Krane’s excellent book, ”Introductory Nuclear Physics”. Kindly read the relevant sections in Krane’s book first. This reading is supplementary to that, and the subsection ordering will mirror that of Krane’s, at least until further notice. β-particle’s are either electrons1 or positrons that are emitted through a certain class of nuclear decay associated with the “weak interaction”. The discoverer of electrons was Henri Becquerel, who noticed that photographic plates, covered in black paper, stored near ra- dioactive sources, became fogged. The black paper (meant to keep the plates unexposed) was thick enough to stop α-particles, and Becquerel concluded that fogging was caused by a new form of radiation, one more penetrating than α-particles. The name “β”, followed naturally as the next letter in the Greek alphabet after α, α-particles having already been discovered and named by Rutherford. Since that discovery, we have learned that β-particles are about 100 times more penetrating 1 than α-particles, and are spin- 2 fermions. Associated with the electrons is a conserved quantity, expressed as the quantum number known as the lepton number. The lepton number of the negatron is, by convention +1. The lepton number of the positron, also the anti- particle of the negatron, is -1. Thus, in a negatron-positron annihilation event, the next lepton number is zero. Only leptons can carry lepton number. (More on this soon.) Recall, from Chapter 13 (Chapter 6 in Krane), our discussion of the various decay modes that are associated with β decay: 1Technically, the word “electron” can represent either a negatron (a fancy word for e−) or a positron (e+). -
Abstract ANGULAR CORRELATIONS in FREE NEUTRON DECAY Jiirgen
365 ANGULAR CORRELATIONS IN FREE NEUTRON DECAY Jiirgen Last Institut Laue-Langevin 156 X 38042 Grenoble Cedex France Abstract The study of particle angular correlations in freeneutron decay provides important information about �-decay coupling constants, the structure of the hadronic weak current and possible extensions to the Standard Model. New experiments are expected to substantially reduce the uncertainty in the parity violating �-asymmetry A. The value of Yuct, which is currently derived from �-transition life times, might soon become available directly from neutron data. J7t=O+ An experiment which looks for time reversal violation in internal pair creation following polarized neutron captureon is briefly discussed. 366 NEIUTRON DECAY AND FUNDAMENTAL PHYSICS The term 'fundamental interaction' suggests that the physical system under study is elementary and prototypical for a whole class of similar processes. In this sense the weak decay of the neutron is clearly fundamental. Although the neutron possesses a complex internal structure, its quark contents is udd, it is the simplest baryonic system which undergoes semileptonic 13- decay. A neutron decays into a proton, an electron and an anti-neutrino. During this process one of the down-quarks is changed into an up-quark, emitting a W-boson which itsself decays into a pair of leptons. Since free quarks have not been observed in an experiment, neutron 13-decay is a very important source of information about the structure of the hadronic weak current and the weak coupling constants gA and gy. Their numerical values serve as input to nuclear astrop hysics problems, Big Bang cosmology, neutrino reactions and many other nuclear physics processes!. -
Albert Einstein and the Fizeau 1851 Water Tube Experiment
Albert Einstein and the Fizeau 1851 Water Tube Experiment Galina Weinstein In 1895 Hendrik Antoon Lorentz derived the Fresnel dragging coefficient in his theory of immobile ether and electrons. This derivation did not explicitly involve electromagnetic theory at all. According to the 1922 Kyoto lecture notes, before 1905 Einstein tried to discuss Fizeau's experiment "as originally discussed by Lorentz" (in 1895). At this time he was still under the impression that the ordinary Newtonian law of addition of velocities was unproblematic. In 1907 Max Laue showed that the Fresnel dragging coefficient would follow from a straightforward application of the relativistic addition theorem of velocities. This derivation is mathematically equivalent to Lorentz's derivation of 1895. From 1907 onwards Einstein adopted Laue's derivation. When Robert Shankland asked Einstein how he had learned of the Michelson-Morley experiment, Einstein told him that he had become aware of it through the writings of Lorentz, but only after 1905 had it come to his attention. "Otherwise", he said, "I would have mentioned it in my paper". He continued to say that the experimental results which had influenced him most were stellar aberration and Fizeau's water tube experiment. "They were enough". Indeed the famous Michelson-Morley experiment is not mentioned in the 1905 relativity paper; but curiously Einstein did not mention Fizeau's experimental result either, and this is puzzling in light of the importance of the experiment in Einstein's pathway to his theory. In this paper I try to discuss this question. 1. Fizeau's Water Tube Experiment of 1851 In 1818 Augustin Fresnel explained that the motion of the earth does not have any influence on the laws of refraction because the ether is partially carried along by the earth and light waves inside the optical medium are partially dragged along with the ether.