Chien-Shiung Wu 1912—1997
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
New Insights to Old Problems
New Insights to Old Problems∗ T. D. Lee Pupin Physics Laboratory, Columbia University, New York, NY, USA and China Center of Advanced Science and Technology (CCAST), Beijing, China Abstract From the history of the θ-τ puzzle and the discovery of parity non-conservation in 1956, we review the current status of discrete symmetry violations in the weak interaction. Possible origin of these symmetry violations are discussed. PACS: 11.30.Er, 12.15.Ff, 14.60.Pq Key words: history of discovery of parity violation, mixing angles, origin of symmetry violation, scalar field and properties of vacuum arXiv:hep-ph/0605017v1 1 May 2006 ∗Based on an invited talk given at the 2006 APS Meeting as the first presentation in the Session on 50 Years Since the Discovery of Parity Nonconservation in the Weak Interaction I, April 22, 2006 (Appendix A) 1 1. Symmetry Violations: The Discovery Almost exactly 50 years ago, I had an important conversation with my dear friend and colleague C. S. Wu. This conversation was critical for setting in mo- tion the events that led to the experimental discovery of parity nonconservation in β-decay by Wu, et al.[1]. In the words of C. S. Wu[2]: ”· · · One day in the early Spring of 1956, Professor T. D. Lee came up to my little office on the thirteenth floor of Pupin Physical Laboratories. He explained to me, first, the τ-θ puzzle. If the answer to the τ-θ puzzle is violation of parity–he went on–then the violation should also be observed in the space distribution of the beta-decay of polarized nuclei: one must measure the pseudo-scalar quantity <σ · p > where p is the electron momentum and σ the spin of the nucleus. -
The Standard Model Part II: Charged Current Weak Interactions I
Prepared for submission to JHEP The Standard Model Part II: Charged Current weak interactions I Keith Hamiltona aDepartment of Physics and Astronomy, University College London, London, WC1E 6BT, UK E-mail: [email protected] Abstract: Rough notes on ... Introduction • Relation between G and g • F W Leptonic CC processes, ⌫e− scattering • Estimated time: 3 hours ⇠ Contents 1 Charged current weak interactions 1 1.1 Introduction 1 1.2 Leptonic charge current process 9 1 Charged current weak interactions 1.1 Introduction Back in the early 1930’s we physicists were puzzled by nuclear decay. • – In particular, the nucleus was observed to decay into a nucleus with the same mass number (A A) and one atomic number higher (Z Z + 1), and an emitted electron. ! ! – In such a two-body decay the energy of the electron in the decay rest frame is constrained by energy-momentum conservation alone to have a unique value. – However, it was observed to have a continuous range of values. In 1930 Pauli first introduced the neutrino as a way to explain the observed continuous energy • spectrum of the electron emitted in nuclear beta decay – Pauli was proposing that the decay was not two-body but three-body and that one of the three decay products was simply able to evade detection. To satisfy the history police • – We point out that when Pauli first proposed this mechanism the neutron had not yet been discovered and so Pauli had in fact named the third mystery particle a ‘neutron’. – The neutron was discovered two years later by Chadwick (for which he was awarded the Nobel Prize shortly afterwards in 1935). -
XIII Probing the Weak Interaction
XIII Probing the weak interaction 1) Phenomenology of weak decays 2) Parity violation and neutrino helicity (Wu experiment and Goldhaber experiment) 3) V- A theory 4) Structure of neutral currents Parity → eigenvalues of parity are +1 (even parity), -1 (odd parity) Parity is conserved in strong and electromagnetic interactions Parity and momentum operator do not commute! Therefore intrinsic partiy is (strictly speaken) defined only for particles AT REST If a system of two particles has a relative angular momentum L, total parity is given by: (*) where are the intrinsic parity of particles Parity is a multiplicative quantum number Parity of spin + ½ fermions (quarks, leptons) per definition P = +1 Parity of spin - ½ anti-fermions (anti-quarks, anti-leptons) P = -1 Parity of W, Z, photon, gluons (and their antiparticles) P =-1 (result of gauge theory) (strictly speaken parity of photon and gluons are not defined, use definition of field) For all other composed and excited particles e.g. kaon, proton, pion, use rule (*) and/or parity conserving IA to determine intrinsic parity Reminder: Parity operator: Intrinsic parity of spin ½ fermions AT REST: +1; of antiparticles: -1 Wu-Experiment Idea: Measurement of the angular distribution of the emitted electron in the decay of polarized 60Co nulcei Angular momentum is an axial vector P J=5 J=4 If P is conserved, the angular distribution must be symmetric (to the dashed line) Identical rates for and . Experiment: Invert 60Co polarization and compare the rates under the same angle . photons are preferably emitted in direction of spin of Ni → test polarization of 60Co (elm. -
Tribute to Valentine Telegdi
Tribute to Valentine Telegdi who passed away on April 8th in Pasadena by K. Freudenreich, ETHZ/IPP/LHP Plenary CHIPP Meeting, PSI, October 2, 2006 Val Telegdi: years 1922 - 1943 Born on January 11th, 1922 in Budapest, spent only a few years in Hungary. According to his own words in his younger years he was a master of “involuntary tourism” , participating passively in German occupations in three countries: Austria, Belgium and Northern Italy. He attended grammar school in Vienna and then a technical school in Brussels. From 1940 - 1943 he worked in a patent attorney’s office in Milan. He used to say that - contrary to Albert Einstein in Berne - being on the other side of the fence he really had to work hard. When the Germans occupied Northern Italy Val, together with his mother, fled to Switzerland. October 2, 2006, Plenary CHIPP Meeting, PSI, K. Freudenreich, ETHZ 1/20 Val Telegdi: years 1943 - 1946 After a short internment in a refugee camp he joined his father in Lausanne where he studied chemical engineering at the EPUL with a grant from the F onds Europ´een de Secours aux Etudiants. At the EPUL he also attended lectures in theoretical physics given by E.C.G. Stuckelberg¨ von Breidenbach whom he estimated very highly. Ironic telegram by Gell-Mann to “congratulate” Feynman for his Nobel prize: “Now you can give back my notes”, signed Stuckelberg¨ Stuckelberg¨ helped Val to be accepted by P. Scherrer at ETHZ. October 2, 2006, Plenary CHIPP Meeting, PSI, K. Freudenreich, ETHZ 2/20 Val Telegdi: years 1946 - 1951 In 1946 the institute of physics was located at the Gloriastrasse. -
Reversal of the Parity Conservation Law in Nuclear Physics
Reversal of the Parity Conservation Law in Nuclear Physics In late 1956, experiments at the National Bureau of proton with an atomic nucleus. The K meson seemed to Standards demonstrated that the quantum mechanical arise in two distinct versions, one decaying into two law of conservation of parity does not hold in the beta mesons, the other decaying into three pions, with the decay of 60Co nuclei. This result, reported in the paper two versions being identical in all other characteristics. An experimental test of parity conservation in beta A mathematical analysis showed that the two-pion and decay [1], together with ensuing experiments on parity the three-pion systems have opposite parity; hence, conservation in -meson decay at Columbia University, according to the prevalent theory, these two versions of shattered a fundamental concept of nuclear physics that the K meson had to be different particles. had been universally accepted for the previous 30 years. Early in 1956, T. D. Lee of Columbia University It thus cleared the way for a reconsideration of physical and C. N. Yang of the Institute for Advanced Study, theories, especially those relating to symmetry, and led Princeton University, made a survey [4] of experimental to new, far-reaching discoveries regarding the nature information on the question of parity. They concluded of matter and the universe. In particular, removal of that the evidence then existing neither supported nor the restrictions imposed by parity conservation first refuted parity conservation in the “weak interactions” resolved a serious conflict in the theory of subatomic responsible for the emission of beta particles, K-meson particles, known at the time as the tau-theta puzzle, and decay, and such. -
The Weak Force: from Fermi to Feynman
South Carolina Honors College Senior Thesis The Weak Force: From Fermi to Feynman Author: Mentor: Alexander Lesov Dr. Milind Purohit arXiv:0911.0058v1 [physics.hist-ph] 31 Oct 2009 October 31, 2009 2 Contents Thesis Summary 5 1 A New Force 7 1.1 The Energy Spectrum Problem . 7 1.2 Pauli: The Conscience of Physics . 8 1.3 TheNeutrino ........................ 9 1.4 EarlyQuantumTheory. 12 1.5 Fermi’sTheory ....................... 18 2 Parity Violation 21 2.1 Laporte’sRule ....................... 23 2.2 LeeandYang ........................ 24 2.3 The θ-τ Puzzle ....................... 25 2.4 ASymmetryinDoubt . .. 26 2.5 TheWuExperiment . .. 29 2.6 ATheoreticalStructureShattered . 30 3 The Road to V-A Theory 33 3.1 FermiTheoryRevisited. 33 3.2 Universal Fermi Interactions . 34 3.3 Consequences of Parity Violation . 36 3.3.1 Two Component Theory of the Neutrino . 37 3.3.2 ANewLagrangian . 38 3.4 TheBirthofV-ATheory. 39 3.5 PuzzlesandOpportunities . 41 Bibliography 43 3 4 CONTENTS Thesis Summary I think physicists are the Peter Pans of the human race. They never grow up and they keep their curiosity. - I.I. Rabi f one was to spend a few minutes observing the physical phenom- enaI taking place all around them, one would come the conclusion that there are only two fundamental forces of nature, Gravitation and Elec- tromagnetism. Just one century ago, this was the opinion held by the worldwide community of physicists. After many decades spent digging deeper and deeper into the heart of matter, two brand new types of interactions were identified, impelling us to add the Strong and Weak nuclear forces to this list. -
RHIC Begins Smashing Nuclei
NEWS RHIC begins smashing nuclei Gold at STAR - side view of a collision of two 30 GeV/nucleon gold End view in the STAR detector of the same collision looking along beams in the STAR detector at the Relativistic Heavy Ion Collider at the direction of the colliding beams. Approximately 1000 tracks Brookhaven. were recorded in this event On Monday 12 June a new high-energy laboratory director for RHIC. It was a proud rings filled, the ions will be whipped to machine made its stage debut as operators in moment for Ozaki, who returned to 70 GeV/nucleon. With stable beams coasting the main control room of Brookhaven's Brookhaven from Japan to oversee the con around the rings, the nuclei collide head-on, Relativistic Heavy Ion Collider (RHIC) finally struction and commissioning of this eventually at the rate of tens of thousands of declared victory over their stubborn beams. challenging machine. collisions per second. Several weeks before, Derek Lowenstein, The high temperatures and densities Principal RHIC components were manufac chairman of the laboratory's collider-acceler achieved in the RHIC collisions should, for a tured by industry, in some cases through ator department, had described repeated fleeting moment, allow the quarks and gluons co-operative ventures that transferred tech attempts to get stable beams of gold ions to roam in a soup-like plasma - a state of nology developed at Brookhaven to private circulating in RHIC's two 3.8 km rings as "like matter that is believed to have last existed industry. learning to drive at the Indy 500!". -
MITOCW | L2.3 Symmetries: Parity
MITOCW | L2.3 Symmetries: Parity PROFESSOR: Hello. In this lecture, we talk about parity and parity violation. So we talk about a discrete symmetry. A little bit of history in particle physics-- Lee and Yang in the 1950s wondered if there's any experiment testing parity invariance. There are many tests which had to do with a strong interaction and the electromagnetic interaction. But as it turned out, parity invariance had never been tested in the weak interaction. And so Lee and Yang were motivated in this because it was a puzzle at the time, so-called tau-theta puzzle, which turned out to be kaon decays into various articles. And then that puzzle, they solved the case with the same lifetime, but different spin states. And so they couldn't quite understand this, and were trying to understand whether or not one can have an experiment to test this. The experiments they proposed is one where you look at the nuclei and observe beta decay. So there's an electron coming out of the beta decay. If you are able to align the spin of the nuclei and put it in front of a mirror, you see that the physics going to the mirror state is not [INAUDIBLE] parity. You see that in the mirror, the spin is the opposite direction, but the momentum of the electrons, the electrons still come out on the bottom. So there's clearly some change in the physics going on in the mirrored state. So Madame Wu actually took up this idea, and immediately tested this in the same year. -
An Improbable Venture
AN IMPROBABLE VENTURE A HISTORY OF THE UNIVERSITY OF CALIFORNIA, SAN DIEGO NANCY SCOTT ANDERSON THE UCSD PRESS LA JOLLA, CALIFORNIA © 1993 by The Regents of the University of California and Nancy Scott Anderson All rights reserved. Library of Congress Cataloging in Publication Data Anderson, Nancy Scott. An improbable venture: a history of the University of California, San Diego/ Nancy Scott Anderson 302 p. (not including index) Includes bibliographical references (p. 263-302) and index 1. University of California, San Diego—History. 2. Universities and colleges—California—San Diego. I. University of California, San Diego LD781.S2A65 1993 93-61345 Text typeset in 10/14 pt. Goudy by Prepress Services, University of California, San Diego. Printed and bound by Graphics and Reproduction Services, University of California, San Diego. Cover designed by the Publications Office of University Communications, University of California, San Diego. CONTENTS Foreword.................................................................................................................i Preface.........................................................................................................................v Introduction: The Model and Its Mechanism ............................................................... 1 Chapter One: Ocean Origins ...................................................................................... 15 Chapter Two: A Cathedral on a Bluff ......................................................................... 37 Chapter Three: -
Nuclear Physics (5Th Lecture)
Nuclear Physics Parity non-conservation in beta decay Parity was introduced first by E. Wigner in 1927, for describing (5th lecture) symmetry of atomic quantum states against r → -r transformation. Electromagnetic interaction conserves the parity Content Strong interaction conserves the parity It was assumed that the weak interaction also conserves the parity. • Parity violation in weak interaction, Wu experiment However, in 1956 T.D.Lee and C.N.Yang showed, that there was no experimental evidence for parity conservation in weak interaction. • History of the neutrino, leptons’ families. Leptonic charge They explained the so called „tau-theta puzzle” assuming that • Anti-neutrino detection (Reines-Cowan experiment) parity is not conserved → Nobel-prize in 1957! • Neutrino detection (Davis experiment) • Solar neutrino puzzle • Neutrino oscillation, and neutrino masses 1 2 If parity is not conserved in weak interaction, this should be seen Why does this mean parity violation? also in nuclear b-decay! • Direction of electrons: p (momentum): vector → -1 if mirrored Experimental proof: C.S.Wu et al. (1957) • Direction of angular momentum J r p : axial vector → +1 if mirrored Result: 60 Polarized Co source: 2μB n - small temperature (~3 mK), kT e if parity was conserved strong magnetic field n Mirroring the coordinate axis is μB kT not a good symmetry! 3 4 http://hyperphysics.phy-astr.gsu.edu/hbase/quantum/imgqua/wu.gif 1 Angular momenta Explanation of the parity violation The story of the neutrino in Wu experiment (complete violation) Early history: 0 1914: Chadwick discovered the continuous energy spectrum of 214 Pb (RaB) using a magnetic spectrometer ~ ~ Interpretation (Rutherford): monoenergetic electrons come ~ 0 out of the nucleus, but they loose energy in the matter Only right-handed antineutrinos (p↑↑s), and 1927: Ellis and Wooster experiment: total energy released by left handed neutrinos (p↑↓s) exist! 210Bi (RaE) b-decays, measured by a differential calorimeter, that could stop all electrons inside. -
Communications-Mathematics and Applied Mathematics/Download/8110
A Mathematician's Journey to the Edge of the Universe "The only true wisdom is in knowing you know nothing." ― Socrates Manjunath.R #16/1, 8th Main Road, Shivanagar, Rajajinagar, Bangalore560010, Karnataka, India *Corresponding Author Email: [email protected] *Website: http://www.myw3schools.com/ A Mathematician's Journey to the Edge of the Universe What’s the Ultimate Question? Since the dawn of the history of science from Copernicus (who took the details of Ptolemy, and found a way to look at the same construction from a slightly different perspective and discover that the Earth is not the center of the universe) and Galileo to the present, we (a hoard of talking monkeys who's consciousness is from a collection of connected neurons − hammering away on typewriters and by pure chance eventually ranging the values for the (fundamental) numbers that would allow the development of any form of intelligent life) have gazed at the stars and attempted to chart the heavens and still discovering the fundamental laws of nature often get asked: What is Dark Matter? ... What is Dark Energy? ... What Came Before the Big Bang? ... What's Inside a Black Hole? ... Will the universe continue expanding? Will it just stop or even begin to contract? Are We Alone? Beginning at Stonehenge and ending with the current crisis in String Theory, the story of this eternal question to uncover the mysteries of the universe describes a narrative that includes some of the greatest discoveries of all time and leading personalities, including Aristotle, Johannes Kepler, and Isaac Newton, and the rise to the modern era of Einstein, Eddington, and Hawking. -
Neutrino, Parity Violaton, VA: a Historical Survey
Neutrino, parity violaton, V-A: a historical survey Ludmil Hadjiivanov Institute for Nuclear Research and Nuclear Energy Bulgarian Academy of Sciences Tsarigradsko Chaussee 72, BG-1784 Sofia, Bulgaria e-mail: [email protected] Abstract This is a concise story of the rise of the four fermion theory of the universal weak interaction and its experimental confirmation, with a special emphasis on the problems related to parity violation. arXiv:1812.11629v1 [physics.hist-ph] 30 Dec 2018 Contents Foreword 2 1 The beta decay and the neutrino 3 2 The notion of parity and the θ τ puzzle 7 − 3 Parity violation 10 4 The two-component neutrino 13 5 The V-A hypothesis 16 6 The end of the beginning 22 Acknowledgments 22 References 23 Appendix. Gamma matrices and the free spin 1/2 field 30 1 Foreword This article emerged initially as a part of a bigger project (joint with Ivan Todorov, still under construction) on the foundations of the Standard Model of particle physics and the algebraic structures behind its symmetries, based in turn on a lecture course presented by Ivan Todorov at the Physics Depart- ment of the University of Sofia in the fall of 2015. The first controversies found in beta decay properties were successfully resolved in the early 30-ies by Pauli and Fermi. The bold prediction of Lee and Yang from 1956 that parity might not be conserved in weak interactions has been confirmed in the beginning of 1957 by the teams of Mme Wu and Lederman and nailed by the end of the same year by Goldhaber, Grodzins and Sunyar who showed in a fine experiment that the neutrino was indeed left-handed.