Chien-Shiung Wu: the First Lady of Physics∗
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Women in Physics, 2000 Highlights
By Rachel Ivie AIP Publication Number R-430 June, 2000 Katie Stowe Women in Physics, 2000 Highlights • An increasingly large number of girls have some exposure to physics by taking it in high school. By 1997, almost one-half of high school physics students were girls (Figure 1) . About 400,000 girls take high school physics each year. • Women’s participation in physics decreases with each step up the academic ladder. For example, more than two-fifths of high school physics students in 1993 were girls, but women earned less than one-fifth of bachelor’s degrees in physics five years later (Figures 1 and 3) . • Although women now earn more than one half of all bachelor’s degrees in the U.S., physics is not attracting women as quickly as other fields, including life sciences, chemistry, and engineering (Figures 4 and 5) . Compared to other fields, women are sorely underrepresented in physics at both the bachelor’s and PhD levels (Figures 4, 5, 6, 7, and Table 1) . • Twenty U.S. physics departments (excluding women’s colleges) had more than 40% female bachelor’s degree recipients during the five academic years 1994-98. This report lists these departments as well as women’s colleges that grant bachelor’s degrees in physics (Tables 2 and 3) . • The proportion of women teaching physics decreases as academic rank and level of the department increases (Table 4) . However, the percentage of women faculty members at each rank is at least as high as the percentage of women earning PhDs at various points in the past. -
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. -
Physics in Your Future Introduces Physics and Careers in Physics to Young People, Their Parents, Teachers and Advisors
TM American Physical Society • Committee on the Status of Women in Physics Chiara La Tessa of Brookhaven National Laboratory is inside the target room of the NASA Space Radiation Laboratory at Brookhaven. She is aligning a detector called EGG counter in the center of a beam – something that’s done before each experiment. Physics helps us understand the world around us, the world inside us, and the world beyond us. Physics is the most basic and fundamental science; it deals with how and why matter and energy act as they do. The laws of physics apply to force and motion, gravity, electricity, magnetism, sound, light and heat. They help us understand the physical world and develop products that people need. Mastering physics is fun and challenging. It involves working with others, as well as alone. You learn how to solve problems, observe things carefully, make measurements and keep accurate records. You can use these valuable skills for the rest of your life. They open doors to many good jobs. Physicists ask questions about the physical world and try to find exact answers. They are creative and persistent. Some do basic research. Their goal is to increase our knowledge of the universe. Others do applied research. They use basic knowledge to solve world problems such as food and energy supply, environmental protection, transportation, communication and defense. Physicists work in industry, educational institutions, government, and medical centers today. Most are active scientists and engineers. They do research and development, administration, and teaching. Others use their physics background in fields like publishing, sales, law, accounting and medicine. -
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. -
Appendix E Nobel Prizes in Nuclear Science
Nuclear Science—A Guide to the Nuclear Science Wall Chart ©2018 Contemporary Physics Education Project (CPEP) Appendix E Nobel Prizes in Nuclear Science Many Nobel Prizes have been awarded for nuclear research and instrumentation. The field has spun off: particle physics, nuclear astrophysics, nuclear power reactors, nuclear medicine, and nuclear weapons. Understanding how the nucleus works and applying that knowledge to technology has been one of the most significant accomplishments of twentieth century scientific research. Each prize was awarded for physics unless otherwise noted. Name(s) Discovery Year Henri Becquerel, Pierre Discovered spontaneous radioactivity 1903 Curie, and Marie Curie Ernest Rutherford Work on the disintegration of the elements and 1908 chemistry of radioactive elements (chem) Marie Curie Discovery of radium and polonium 1911 (chem) Frederick Soddy Work on chemistry of radioactive substances 1921 including the origin and nature of radioactive (chem) isotopes Francis Aston Discovery of isotopes in many non-radioactive 1922 elements, also enunciated the whole-number rule of (chem) atomic masses Charles Wilson Development of the cloud chamber for detecting 1927 charged particles Harold Urey Discovery of heavy hydrogen (deuterium) 1934 (chem) Frederic Joliot and Synthesis of several new radioactive elements 1935 Irene Joliot-Curie (chem) James Chadwick Discovery of the neutron 1935 Carl David Anderson Discovery of the positron 1936 Enrico Fermi New radioactive elements produced by neutron 1938 irradiation Ernest Lawrence -
UC San Diego UC San Diego Electronic Theses and Dissertations
UC San Diego UC San Diego Electronic Theses and Dissertations Title The new prophet : Harold C. Urey, scientist, atheist, and defender of religion Permalink https://escholarship.org/uc/item/3j80v92j Author Shindell, Matthew Benjamin Publication Date 2011 Peer reviewed|Thesis/dissertation eScholarship.org Powered by the California Digital Library University of California UNIVERSITY OF CALIFORNIA, SAN DIEGO The New Prophet: Harold C. Urey, Scientist, Atheist, and Defender of Religion A dissertation submitted in partial satisfaction of the requirements for the degree Doctor of Philosophy in History (Science Studies) by Matthew Benjamin Shindell Committee in charge: Professor Naomi Oreskes, Chair Professor Robert Edelman Professor Martha Lampland Professor Charles Thorpe Professor Robert Westman 2011 Copyright Matthew Benjamin Shindell, 2011 All rights reserved. The Dissertation of Matthew Benjamin Shindell is approved, and it is acceptable in quality and form for publication on microfilm and electronically: ___________________________________________________________________ ___________________________________________________________________ ___________________________________________________________________ ___________________________________________________________________ ___________________________________________________________________ Chair University of California, San Diego 2011 iii TABLE OF CONTENTS Signature Page……………………………………………………………………...... iii Table of Contents……………………………………………………………………. iv Acknowledgements…………………………………………………………………. -
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. -
April 2002 NEWS Volume 11, No
April 2002 NEWS Volume 11, No. 4 A Publication of The American Physical Society http://www.aps.org/apsnews Executive Board Expresses Concern Over Funding Imbalance In Bush Administration’s FY2003 Budget Request When President Bush unveiled outside of the scientific community tire research budget of the National for physical science remains es- his FY 2003 budget request for have expressed concern at the im- Science Foundation, in keeping sentially flat, the APS Executive The Executive Board of the R&D in February, no one was sur- balance of research funding with the president’s campaign bud- Board approved a resolution re- American Physical Society ap- prised at the emphasis on priorities in favor of the biological get to double the NIH budget by garding the FY2003 budget plauds the proposed increased antiterrorist, and on homeland sciences. 2003. request at its meeting on Febru- for the NIH and for life sciences and economic security in the wake For example, the National Insti- Noting that while funding for ary 23, 2002. The full text of the generally in the FY2003 Bud- of the September 11th attacks. How- tutes of Health would receive a $3.9 biological and medical research Executive Board statement is con- get Request submitted by President Bush on February 4, ever, many both within and billion increase, larger than the en- continues to increase, funding tained in the box at the right. 2002. However, the Board ex- presses great concern about Task Force to Weigh Pros the requested budgetary lev- Outlook on FY 2003 Budget Bills els for research in the physi- cal sciences. -
The Man Behind an Identity in Quantum Electrodynamics by F
The man behind an identity in quantum electrodynamics by F. J. Duarte Introduction The 6th of May, 2010, marks the 10th anniversary of the passing of John Clive Ward a quiet genius of physics whose ideas and contributions helped shape the post-war quantum era. Since John was an Australian citizen it is only appropriate to remember him in the pages of this journal. First, as a manner of introduction, I will outline John’s most salient contributions. Then, I will attempt a description of the physicists, teacher, and friend that I was privileged to know. Physics theoreticians thus producing a series of brilliant papers on: In an approximated chronological order the contributions of the Ising Model (Kac and Ward, 1952), quantum solid-state John Ward began with a paper published (with Maurice L. physics (Ward and Wilks, 1952), quantum statistics (Montroll H. Pryce) in Nature as part of his doctoral research at Oxford and Ward, 1958), and Fermion theory (Luttinger and Ward, (Pryce and Ward, 1947). This was a solution to a problem, 1960). His last paper was on the Dirac equation and higher that according to John was posed by Dirac, and that J. A. symmetries (Ward, 1978). Wheeler had tried to solve (Ward, 2004). The suggestion to tackle this problem was made by Pryce (a former student of In a piece written in an Oxford publication it was once stated R. H. Fowler and John’s supervisor). This had to do with that Ward “has contributed deeply to an astonishingly broad the decay of γ particles and the emission of two correlated range of theoretical physics: statistical mechanics, plasma photons in opposite directions. -
Some Aspects of the Theory of Heavy Ion Collisions
Some Aspects of the Theory of Heavy Ion Collisions Franc¸ois Gelis Institut de Physique Th´eorique CEA/Saclay, Universit´eParis-Saclay 91191, Gif sur Yvette, France June 16, 2021 Abstract We review the theoretical aspects relevant in the description of high energy heavy ion collisions, with an emphasis on the learnings about the underlying QCD phenomena that have emerged from these collisions. 1 Introduction to heavy ion collisions Elementary forces in Nature The interactions among the elementary constituents of matter are divided into four fundamental forces: gravitation, electromagnetism, weak nuclear forces and strong nuclear forces. All these interactions except gravity have a well tested a microscopic quantum description in terms of local gauge theories, in which the elementary matter fields are spin-1=2 fermions, interacting via the exchange of spin-1 bosons. In this framework, a special role is played by the Higgs spin-0 boson (the only fundamental scalar particle in the Standard Model), whose non-zero vacuum expectation value gives to all the other fields a mass proportional to their coupling to the Higgs. The discovery of the Higgs boson at the Large Hadron Collider in 2012 has so far confirmed all the Standard Model expectations. In this picture, gravity has remained a bit of an outlier: even though the classical field theory of gravitation (general relativity) has been verified experimentally with a high degree of precision (the latest of these verifications being the observation of gravitational waves emitted during the merger of massive compact objects - black holes or arXiv:2102.07604v3 [hep-ph] 15 Jun 2021 neutron stars), the quest for a theory of quantum gravity has been inconclusive until now (and possible experimental probes are far out of reach for the foreseeable future).