Events Leading to the Manhattan Project
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1 the Equation of a Light Leptonic Magnetic Monopole and Its
The equation of a Light Leptonic Magnetic Monopole and its Experimental Aspects Georges Lochak Fondation Louis de Broglie 23, rue Marsoulan F-75012 Paris [email protected] Abstract. The present theory is closely related to Dirac’s equation of the electron, but not to his magnetic monopole theory, except for his relation between electric and magnetic charge. The theory is based on the fact, that the massless Dirac equation admits a second electromagnetic coupling, deduced from a pseudo-scalar gauge invariance. The equation thus obtained has the symmetry laws of a massless leptonic, magnetic monopole, able to interact weakly. We give a more precise form of the Dirac relation between electric and magnetic charges and a quantum form of the Poincaré first integral. In the Weyl representation our equation splits into P-conjugated monopole and antimonopole equations with the correct electromagnetic coupling and opposite chiralities, predicted by P. Curie. Charge conjugated monopoles are symmetric in space and not in time (contrary to the electric particles) : an important fact for the vacuum polarization. Our monopole is a magnetically excited neutrino, which leads to experimental consequences. These monopoles are assumed to be produced by electromagnetic pulses or arcs, leading to nuclear transmutations and, for beta radioactive elements, a shortening of the life time and the emission of monopoles instead of neutrinos in a magnetic field. A corresponding discussion is given in section 15. 1. Introduction. The hypothesis of separated magnetic poles is very old. In the 2nd volume of his famous Treatise of Electricity and Magnetism [1], devoted to Magnetism, Maxwell considered the existence of free magnetic charges as an evidence, just as the evidence of electric charges. -
Chapter 4. CLASSIFICATION UNDER the ATOMIC ENERGY
Chapter 4 CLASSIFICATION UNDER THE ATOMIC ENERGY ACT INTRODUCTION The Atomic Energy Act of 1946 was the first and, other than its successor, the Atomic Energy Act of 1954, to date the only U.S. statute to establish a program to restrict the dissemination of information. This Act transferred control of all aspects of atomic (nuclear) energy from the Army, which had managed the government’s World War II Manhattan Project to produce atomic bombs, to a five-member civilian Atomic Energy Commission (AEC). These new types of bombs, of awesome power, had been developed under stringent secrecy and security conditions. Congress, in enacting the 1946 Atomic Energy Act, continued the Manhattan Project’s comprehensive, rigid controls on U.S. information about atomic bombs and other aspects of atomic energy. That Atomic Energy Act designated the atomic energy information to be protected as “Restricted Data” and defined that data. Two types of atomic energy information were defined by the Atomic Energy Act of 1954, Restricted Data (RD) and a type that was subsequently termed Formerly Restricted Data (FRD). Before discussing further the Atomic Energy Act of 1946 and its unique requirements for controlling atomic energy information, some of the special information-control activities that accompanied the research, development, and production efforts that led to the first atomic bomb will be mentioned. Realization that an atomic bomb was possible had a profound impact on the scientists who first became aware of that possibility. The implications of such a weapon were so tremendous that the U.S. scientists conducting the initial, basic research related to nuclear fission voluntarily restricted the publication of their scientific work in this area. -
Unerring in Her Scientific Enquiry and Not Afraid of Hard Work, Marie Curie Set a Shining Example for Generations of Scientists
Historical profile Elements of inspiration Unerring in her scientific enquiry and not afraid of hard work, Marie Curie set a shining example for generations of scientists. Bill Griffiths explores the life of a chemical heroine SCIENCE SOURCE / SCIENCE PHOTO LIBRARY LIBRARY PHOTO SCIENCE / SOURCE SCIENCE 42 | Chemistry World | January 2011 www.chemistryworld.org On 10 December 1911, Marie Curie only elements then known to or ammonia, having a water- In short was awarded the Nobel prize exhibit radioactivity. Her samples insoluble carbonate akin to BaCO3 in chemistry for ‘services to the were placed on a condenser plate It is 100 years since and a chloride slightly less soluble advancement of chemistry by the charged to 100 Volts and attached Marie Curie became the than BaCl2 which acted as a carrier discovery of the elements radium to one of Pierre’s electrometers, and first person ever to win for it. This they named radium, and polonium’. She was the first thereby she measured quantitatively two Nobel prizes publishing their results on Boxing female recipient of any Nobel prize their radioactivity. She found the Marie and her husband day 1898;2 French spectroscopist and the first person ever to be minerals pitchblende (UO2) and Pierre pioneered the Eugène-Anatole Demarçay found awarded two (she, Pierre Curie and chalcolite (Cu(UO2)2(PO4)2.12H2O) study of radiactivity a new atomic spectral line from Henri Becquerel had shared the to be more radioactive than pure and discovered two new the element, helping to confirm 1903 physics prize for their work on uranium, so reasoned that they must elements, radium and its status. -
The Transuranium Elements: from Neptunium and Plutonium to Element 112
UCRL-JC- 124728 The Transuranium Elements: From Neptunium and Plutonium to Element 112 Professor Darleane C. Hoffman Lawrence Livermore National Laboratory G. Seaborg Institute for Transactinium Science RECEIVED T. Isotope Sciences Division sEp23 ?9g6 This paper was prepared for submittal to the Conference Proceedings NATO Advanced Study Institute on "Actinides and the Environment" Chania, Crete, Greece July 7-19, 1996 July 26, 1996 DISCWMER This document was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor the University of California nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or the University of California. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or the University of California, and shall not be used for advertising or product endorsement purposes. DISCLAIMER Portions of this document may be illegible in electronic image products. Images are produced from the best avaiiable original document. c THE TRANSURANIUM ELEMENTS: FROM NEPTUNIUM AM) PLUTONIUM TO ELEMENT112 DarIeane C. Hoffman Nuclear Science Division & Chemistry Department, University of California, Berkeley, CA 94720 & G. T. Seaborg Institute for ' Transactinium Science, MS-L23 1, LLNL, Livermore, CA 94550. -
Rutherford's Nuclear World: the Story of the Discovery of the Nuc
Rutherford's Nuclear World: The Story of the Discovery of the Nuc... http://www.aip.org/history/exhibits/rutherford/sections/atop-physic... HOME SECTIONS CREDITS EXHIBIT HALL ABOUT US rutherford's explore the atom learn more more history of learn about aip's nuclear world with rutherford about this site physics exhibits history programs Atop the Physics Wave ShareShareShareShareShareMore 9 RUTHERFORD BACK IN CAMBRIDGE, 1919–1937 Sections ← Prev 1 2 3 4 5 Next → In 1962, John Cockcroft (1897–1967) reflected back on the “Miraculous Year” ( Annus mirabilis ) of 1932 in the Cavendish Laboratory: “One month it was the neutron, another month the transmutation of the light elements; in another the creation of radiation of matter in the form of pairs of positive and negative electrons was made visible to us by Professor Blackett's cloud chamber, with its tracks curled some to the left and some to the right by powerful magnetic fields.” Rutherford reigned over the Cavendish Lab from 1919 until his death in 1937. The Cavendish Lab in the 1920s and 30s is often cited as the beginning of modern “big science.” Dozens of researchers worked in teams on interrelated problems. Yet much of the work there used simple, inexpensive devices — the sort of thing Rutherford is famous for. And the lab had many competitors: in Paris, Berlin, and even in the U.S. Rutherford became Cavendish Professor and director of the Cavendish Laboratory in 1919, following the It is tempting to simplify a complicated story. Rutherford directed the Cavendish Lab footsteps of J.J. Thomson. Rutherford died in 1937, having led a first wave of discovery of the atom. -
Harry Truman, the Atomic Bomb and the Apocalyptic Narrative
Volume 5 | Issue 7 | Article ID 2479 | Jul 12, 2007 The Asia-Pacific Journal | Japan Focus The Decision to Risk the Future: Harry Truman, the Atomic Bomb and the Apocalyptic Narrative Peter J. Kuznick The Decision to Risk the Future: Harry stressed that the future of mankind would be Truman, the Atomic Bomb and theshaped by how such bombs were used and Apocalyptic Narrative subsequently controlled or shared.[3] Truman recalled Stimson “gravely” expressing his Peter J. Kuznick uncertainty about whether the U.S. should ever use the bomb, “because he was afraid it was so I powerful that it could end up destroying the whole world.” Truman admitted that, listening In his personal narrative Atomic Quest, Nobel to Stimson and Groves and reading Groves’s Prize-winning physicist Arthur Holly Compton, accompanying memo, he “felt the same who directed atomic research at the University fear.”[4] of Chicago’s Metallurgical Laboratory during the Second World War, tells of receiving an urgent visit from J. Robert Oppenheimer while vacationing in Michigan during the summer of 1942. Oppenheimer and the brain trust he assembled had just calculated the possibility that an atomic explosion could ignite all the hydrogen in the oceans or the nitrogen in the atmosphere. If such a possibility existed, Compton concluded, “these bombs must never be made.” As Compton said, “Better to accept the slavery of the Nazis than to run a chance of drawing the final curtain on mankind.”[1] Certainly, any reasonable human being could be expected to respond similarly. Three years later, with Hitler dead and the Nazis defeated, President Harry Truman faced Truman and Byrnes en route to Potsdam, July a comparably weighty decision. -
Atomic Physics & Quantum Effects
KEY CONCEPTS ATOMIC PHYSICS & QUANTUM EFFECTS 1. PHOTONS & THE PHOTOELECTRIC EFFECT Max Planck explained blackbody radiation with his quantum hypothesis, which states that the energy of a thermal oscillator, Eosc, is not continuous, but instead is a discrete quantity given by the equation: Eosc = nhf n = 1, 2, 3,... where f is the frequency and h is a constant now known as Planck’s constant. Albert Einstein extended the idea by adding that all emitted radiation is quantized. He suggested that light is composed of discrete quanta, rather than of waves. According to his theory, each particle of light, known as a photon, has an energy E given by: E = hf Einstein’s theory helped him explain a phenomenon known as the photoelectric effect, in which a photon of light strikes a photosensitive material and causes an electron to be ejected from the material. A photocell constructed from photosensitive material can produce an electrical current when light shines on it. The kinetic energy, K, of a photoelectron displaced by a photon of energy, hf, is given by: K = hf - φ where the work function, φ, is the minimum energy needed to free the electron from the photosensitive material. No photoemission occurs if the frequency of the incident light falls below a certain cutoff frequency – or threshold frequency – given by: φ f0 = h Einstein's theory explained several aspects of the photoelectric effect that could not be explained by classical theory: • The kinetic energy of photoelectrons is dependent on the light’s frequency. • No photoemission occurs for light below a certain threshold frequency. -
The Development of Military Nuclear Strategy And
The Development of Military Nuclear Strategy and Anglo-American Relations, 1939 – 1958 Submitted by: Geoffrey Charles Mallett Skinner to the University of Exeter as a thesis for the degree of Doctor of Philosophy in History, July 2018 This thesis is available for Library use on the understanding that it is copyright material and that no quotation from the thesis may be published without proper acknowledgement. I certify that all material in this thesis which is not my own work has been identified and that no material has previously been submitted and approved for the award of a degree by this or any other University. (Signature) ……………………………………………………………………………… 1 Abstract There was no special governmental partnership between Britain and America during the Second World War in atomic affairs. A recalibration is required that updates and amends the existing historiography in this respect. The wartime atomic relations of those countries were cooperative at the level of science and resources, but rarely that of the state. As soon as it became apparent that fission weaponry would be the main basis of future military power, America decided to gain exclusive control over the weapon. Britain could not replicate American resources and no assistance was offered to it by its conventional ally. America then created its own, closed, nuclear system and well before the 1946 Atomic Energy Act, the event which is typically seen by historians as the explanation of the fracturing of wartime atomic relations. Immediately after 1945 there was insufficient systemic force to create change in the consistent American policy of atomic monopoly. As fusion bombs introduced a new magnitude of risk, and as the nuclear world expanded and deepened, the systemic pressures grew. -
Trinity Scientific Firsts
TRINITY SCIENTIFIC FIRSTS THE TRINITY TEST was perhaps the greatest scientifi c experiment ever. Seventy-fi ve years ago, Los Alamos scientists and engineers from the U.S., Britain, and Canada changed the world. July 16, 1945 marks the entry into the Atomic Age. PLUTONIUM: THE BETHE-FEYNMAN FORMULA: Scientists confi rmed the newly discovered 239Pu has attractive nuclear Nobel Laureates Hans Bethe and Richard Feynman developed the physics fi ssion properties for an atomic weapon. They were able to discern which equation used to estimate the yield of a fi ssion weapon, building on earlier production path would be most effective based on nuclear chemistry, and work by Otto Frisch and Rudolf Peierls. The equation elegantly encapsulates separated plutonium from Hanford reactor fuel. essential physics involved in the nuclear explosion process. PRECISION HIGH-EXPLOSIVE IMPLOSION FOUNDATIONAL RADIOCHEMICAL TO CREATE A SUPER-CRITICAL ASSEMBLY: YIELD ANALYSIS: Project Y scientists developed simultaneously-exploding bridgewire detonators Wartime radiochemistry techniques developed and used at Trinity with a pioneering high-explosive lens system to create a symmetrically provide the foundation for subsequent analyses of nuclear detonations, convergent detonation wave to compress the core. both foreign and domestic. ADVANCED IMAGING TECHNIQUES: NEW FRONTIERS IN COMPUTING: Complementary diagnostics were developed to optimize the implosion Human computers and IBM punched-card machines together calculated design, including fl ash x-radiography, the RaLa method, -
My Time with Sir Rudolf Peierls
ARTICLE-IN-A-BOX My Time with Sir Rudolf Peierls Professor Peierls took up the Wykeham Professorship at Oxford in October 1963. I started as his research assistant in the Department of Theoretical Physics at the beginning of November the same year. I had just ¯nished my PhD with Mel Preston, a former student of Peierls at Birmingham. Theoretical Physics, which Peierls headed, was a large department housed at 12-14 Parks Road. It had many faculty members, graduate students, post-doctoral fellows, and visiting foreign professors. The faculty included R H Dalitz, the Royal Society professor lured from Chicago, Roger Elliott, D ter Haar, David Brink, L Castillejo, amongst others. In addition to his administrative duties, Peierls lectured on nuclear theory, supervised students, and actively participated in seminars and colloquia. The latter took place at the Clarendon laboratory nearby, where the experimentalists worked. In addition, nuclear physics was also housed at 9 Keble Road. We all took afternoon tea at the Clarendon, thereby bringing some cohesion amongst the diverse groups. At this time, Divakaran and Rajasekaran were both at Oxford ¯nishing their doctoral work with Dalitz. K Chandrakar (plasma physics) and E S Rajagopal (low-temperature physics) were at the Clarendon. As will be clear from Professor Baskaran's article, Peierls was a versatile physicist, having made fundamental contributions in condensed matter physics, statistical mechanics, quantum ¯eld theory and nuclear physics. I think it is fair to say that in the mid-sixties his focus was mostly in nuclear theory, in addition to his work in the Pugwash movement on nuclear disarmament. -
I. I. Rabi Papers [Finding Aid]. Library of Congress. [PDF Rendered Tue Apr
I. I. Rabi Papers A Finding Aid to the Collection in the Library of Congress Manuscript Division, Library of Congress Washington, D.C. 1992 Revised 2010 March Contact information: http://hdl.loc.gov/loc.mss/mss.contact Additional search options available at: http://hdl.loc.gov/loc.mss/eadmss.ms998009 LC Online Catalog record: http://lccn.loc.gov/mm89076467 Prepared by Joseph Sullivan with the assistance of Kathleen A. Kelly and John R. Monagle Collection Summary Title: I. I. Rabi Papers Span Dates: 1899-1989 Bulk Dates: (bulk 1945-1968) ID No.: MSS76467 Creator: Rabi, I. I. (Isador Isaac), 1898- Extent: 41,500 items ; 105 cartons plus 1 oversize plus 4 classified ; 42 linear feet Language: Collection material in English Location: Manuscript Division, Library of Congress, Washington, D.C. Summary: Physicist and educator. The collection documents Rabi's research in physics, particularly in the fields of radar and nuclear energy, leading to the development of lasers, atomic clocks, and magnetic resonance imaging (MRI) and to his 1944 Nobel Prize in physics; his work as a consultant to the atomic bomb project at Los Alamos Scientific Laboratory and as an advisor on science policy to the United States government, the United Nations, and the North Atlantic Treaty Organization during and after World War II; and his studies, research, and professorships in physics chiefly at Columbia University and also at Massachusetts Institute of Technology. Selected Search Terms The following terms have been used to index the description of this collection in the Library's online catalog. They are grouped by name of person or organization, by subject or location, and by occupation and listed alphabetically therein. -
Chem 103, Section F0F Unit I
Lecture 4 - Observations that Led to the Chem 103, Section F0F Nuclear Model of the Atom Unit I - An Overview of Chemistry Dalton’s theory proposed that atoms were indivisible particles. Lecture 4 • By the late 19th century, this aspect of Dalton’s theory was being challenged. • Work with electricity lead to the discovery of the electron, • Some observations that led to the nuclear model as a particle that carried a negative charge. for the structure of the atom • The modern view of the atomic structure and the elements • Arranging the elements into a (periodic) table 2 Lecture 4 - Observations that Led to the Lecture 4 - Observations that Led to the Nuclear Model of the Atom Nuclear Model of the Atom The cathode ray In 1897, J.J. Thomson (1856-1940) studies how cathode rays • Cathode rays were shown to be electrons are affected by electric and magnetic fields • This allowed him to determine the mass/charge ration of an electron Cathode rays are released by metals at the cathode 3 4 Lecture 4 - Observations that Led to the Lecture 4 - Observations that Led to the Nuclear Model of the Atom Nuclear Model of the Atom In 1897, J.J. Thomson (1856-1940) studies how cathode rays In 1897, J.J. Thomson (1856-1940) studies how cathode rays are affected by electric and magnetic fields are affected by electric and magnetic fields • Thomson estimated that the mass of an electron was less • Thomson received the 1906 Nobel Prize in Physics for his that 1/1000 the mass of the lightest atom, hydrogen!! work.