JOHN HASBROUCK VAN VLECK March 13, 1899-October 27, 1980
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April 17-19, 2018 the 2018 Franklin Institute Laureates the 2018 Franklin Institute AWARDS CONVOCATION APRIL 17–19, 2018
april 17-19, 2018 The 2018 Franklin Institute Laureates The 2018 Franklin Institute AWARDS CONVOCATION APRIL 17–19, 2018 Welcome to The Franklin Institute Awards, the a range of disciplines. The week culminates in a grand United States’ oldest comprehensive science and medaling ceremony, befitting the distinction of this technology awards program. Each year, the Institute historic awards program. celebrates extraordinary people who are shaping our In this convocation book, you will find a schedule of world through their groundbreaking achievements these events and biographies of our 2018 laureates. in science, engineering, and business. They stand as We invite you to read about each one and to attend modern-day exemplars of our namesake, Benjamin the events to learn even more. Unless noted otherwise, Franklin, whose impact as a statesman, scientist, all events are free, open to the public, and located in inventor, and humanitarian remains unmatched Philadelphia, Pennsylvania. in American history. Along with our laureates, we celebrate his legacy, which has fueled the Institute’s We hope this year’s remarkable class of laureates mission since its inception in 1824. sparks your curiosity as much as they have ours. We look forward to seeing you during The Franklin From sparking a gene editing revolution to saving Institute Awards Week. a technology giant, from making strides toward a unified theory to discovering the flow in everything, from finding clues to climate change deep in our forests to seeing the future in a terahertz wave, and from enabling us to unplug to connecting us with the III world, this year’s Franklin Institute laureates personify the trailblazing spirit so crucial to our future with its many challenges and opportunities. -
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…………………………………………………………………. -
Supplementary Figure 1: Interconnected Multiplex with Six Nodes in Two Layers (A and D) and Corresponding Aggregated Networks (B and E)
Supplementary Figure 1: Interconnected multiplex with six nodes in two layers (A and D) and corresponding aggregated networks (B and E). The nodes are ranked by their eigenvector centrality in each layer separately, in the aggregated and in the whole interconnected structure (C and F). Case A, B and C. Nodes 1 and 3 have a key role in the multilayer, being bridges between the two layers. In a collaboration network they would represent scientists working on two different research areas who allow information to flow from one subject to the other. While nodes 1 and 3 gain centrality from their connections to \hubs" on different layers, they also gain centrality from their own counterparts in other layers, making them important in the multilayer network. In the aggregated network their versatility disappears, because the information is washed out by projecting on a single layer, where nodes 2 and 6 are still \hubs" but it is not possible to capture the importance of nodes 1 and 3 in bridging different areas. Case D, E and F. This example shows how aggregating the full information on a single network introduces a spurious symmetry between nodes 2, 3, 4 and 6 that is not present in the multilayer, except for 2 and 4. The resulting score in the aggregate is not able to capture the difference between these nodes (corresponding to a degeneration in the eigenspace) while it is evident that, for instance, node 6 is more central than node 3 because of its direct connection to node 1 { the \hub" { in layer 1. -
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. -
Edward B. Van Vleck 1863‐1943
Remembering Van: Three Madison families and other tales “Van had many enthusiasms and loyalties, but none exceeded those he felt for the University of Wisconsin and its home, Madison.” 1 Charles Van Hise Born in 1857, Charles Van Hise was a distinguished geologist who had been elected to the National Academy of Sciences in 1902. In 1903, he was named President of the University of Wisconsin 2 In 1904, Van Hise recruited Charles Russell Bardeen, a member of the first class to graduate of the Johns Hopkins Medical School, to found a medical school at the University of Wisconsin John Bardeen is at the right hand end. His grandfather, Charles W Bardeen, is second from the left. 3 Charles Sumner Slichter 1864-1946 In 1906, Van Hise appointed Charles S. Slichter head of the math department. An applied mathematician with interests in flow of liquids through porous media, Slichter realized the department needed to strengthen the faculty in pure mathematics. 4 Edward B. Van Vleck 1863‐1943 Edward B Van Vleck, had earned a PhD in mathematics at Gottingen in1893, and was a member of the National Academy of Sciences. Slichter’s first action as department head was to recruit Van Vleck to bring strength in pure mathematics. 5 John Hasbrouck Van Vleck was born in 1899. His interest in trains began at a early age. Van attended his first Wisconsin football game at age 10.(Wisconsin vs Minnesota) It was the first game at which the band played the famous song “On Wisconsin”. As an undergraduate at Wisconsin, Van played flute In the band. -
Report and Opinion 2016;8(6) 1
Report and Opinion 2016;8(6) http://www.sciencepub.net/report Beyond Einstein and Newton: A Scientific Odyssey Through Creation, Higher Dimensions, And The Cosmos Manjunath R Independent Researcher #16/1, 8 Th Main Road, Shivanagar, Rajajinagar, Bangalore: 560010, Karnataka, India [email protected], [email protected] “There is nothing new to be discovered in physics now. All that remains is more and more precise measurement.” : Lord Kelvin Abstract: General public regards science as a beautiful truth. But it is absolutely-absolutely false. Science has fatal limitations. The whole the scientific community is ignorant about it. It is strange that scientists are not raising the issues. Science means truth, and scientists are proponents of the truth. But they are teaching incorrect ideas to children (upcoming scientists) in schools /colleges etc. One who will raise the issue will face unprecedented initial criticism. Anyone can read the book and find out the truth. It is open to everyone. [Manjunath R. Beyond Einstein and Newton: A Scientific Odyssey Through Creation, Higher Dimensions, And The Cosmos. Rep Opinion 2016;8(6):1-81]. ISSN 1553-9873 (print); ISSN 2375-7205 (online). http://www.sciencepub.net/report. 1. doi:10.7537/marsroj08061601. Keywords: Science; Cosmos; Equations; Dimensions; Creation; Big Bang. “But the creative principle resides in Subaltern notable – built on the work of the great mathematics. In a certain sense, therefore, I hold it astronomers Galileo Galilei, Nicolaus Copernicus true that pure thought can -
A Rigorous Derivation of the Larmor and Van Vleck Contributions Baptiste Savoie
On the atomic orbital magnetism: A rigorous derivation of the Larmor and Van Vleck contributions Baptiste Savoie To cite this version: Baptiste Savoie. On the atomic orbital magnetism: A rigorous derivation of the Larmor and Van Vleck contributions. 2013. hal-00785100v1 HAL Id: hal-00785100 https://hal.archives-ouvertes.fr/hal-00785100v1 Preprint submitted on 5 Feb 2013 (v1), last revised 24 Apr 2014 (v5) HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. On the atomic orbital magnetism: a rigorous derivation of the Larmor and Van Vleck contributions. February 5, 2013 ∗ Baptiste Savoie Abstract The aim of this paper is to rigorously investigate the orbital magnetism of core electrons in crystalline ordered solids and in the zero-temperature regime. To achieve that, we consider a non-interacting Fermi gas subjected to an external periodic potential within the framework of the tight-binding approximation (i.e. when the distance R between two consecutive ions is large). For a fixed number of particles in the Wigner-Seitz cell and in the zero-temperature limit, we write down an asymptotic expansion for the bulk zero-field orbital susceptibility and prove that the leading term is the superposition of the Larmor diamagnetic contribution (reducing to the Langevin formula in the classical limit) together with the so-called orbital Van Vleck contribution. -
Quantum Theory Developments* 1N Chemistry
N. TRINAJSTIC: Quantum Theory in Chemistry, Kern. Ind. 50 (7-8) 421-425 (2001) 421 Quantum Theory 1n• Chemistry - Early Developments* N. Trinajstic KUI 22/2001 The Rugjer Boskovic Institute, Received November 17, 2000 POB 180, HR-10002 Zagreb, Croatia Accepted March 30, 2001 . The beginnings of quantum theory, and the main group of phycisists responsible for rts early development, are briefly mentioned. The birthday of quantum chemistry is con sidered to be June 30, 1927 when the Editor (Karl Scheel) of Zeitschrift for Physik recei ved the manuscript by Walter Heitler and Fritz London, who used the Schrodinger equa tion to study the electronic structure of a hydrogen molecule cation and a hydrogen mo lecule and introduced exhange forces between atoms as responsible for forming the che mical bond (there are also other views regarding the birthday of quantum chemistry). First quantum chemists, their contributions and first books on quantum chemistry are briefly mentioned. Early development of quantum chemistry is succinctly reviewed. Key words: Quantum chemistry • quantum theory • molecular orbital (MO) theory • va- lence bond (VB) theory Introduction completed, especially in relation to the theory of re lativity, the second great physics theory of the 20th Quantum theory was born at the very end of the century, introduced in 1905 (in its "special" form) 19th century. Max Planck (1858-1947) delivered by Albert Einstein (1879-1955). 3 However, in this his historical lecture on December 14, 1900 at the essay we are interested in the early development of meeting of the German Physical Society in Berlin. quantum chemistry, that is, the application of quan In this lecture Planck stated that paradoxes distur tum theory in chemistry. -
Magnetic Susceptibility Measurements of Transition Metal Containing Compounds
Magnetic susceptibility measurements of transition metal containing compounds Introduction: Measurements of magnetic properties have been used to characterize a wide range of systems from oxygen, metallic alloys, solid state materials, and coordination complexes containing metals. Most organic and main group element compounds have all the electrons paired and these are diamagnetic molecules with very small magnetic moments. All of the transition metals have at least one oxidation state with an incomplete d subshell. Magnetic measurements, particularly for the first row transition elements, give information about the number of unpaired electrons. The number of unpaired electrons provides information about the oxidation state and electron configuration. The determination of the magnetic properties of the second and third row transition elements is more complex. The magnetic moment is calculated from the magnetic susceptibility, since the magnetic moment is not measured directly. There are several ways to express the degree to which a material acquires a magnetic moment in a field. The magnetic susceptibility per unit volume is defined by: I H where I is the intensity of the magnetization induced in the sample by the external magnetic field, H. The extent of the magnetic induction (I) depends on the sample. The induction may be visualized as an alignment of dipoles and/or by the formation of charge polarization in the sample. H is the strength of the external magnetic field in units of oersteds (Oe). The κ is unitless. Generally, it is more convenient to use mass units, therefore the mass or gram susceptibility is defined as: g d where d is the density of the solid. -
Nobel Prizes in Physics Closely Connected with the Physics of Solids
Nobel Prizes in Physics Closely Connected with the Physics of Solids 1901 Wilhelm Conrad Röntgen, Munich, for the discovery of the remarkable rays subsequently named after him 1909 Guglielmo Marconi, London, and Ferdinand Braun, Strassburg, for their contributions to the development of wireless telegraphy 1913 Heike Kamerlingh Onnes, Leiden, for his investigations on the properties of matter at low temperatures which lead, inter alia, to the production of liquid helium 1914 Max von Laue, Frankfort/Main, for his discovery of the diffraction of X-rays by crystals 1915 William Henry Bragg, London, and William Lawrence Bragg, Manchester, for their analysis of crystal structure by means of X-rays 1918 Max Planck, Berlin, in recognition of the services he rendered to the advancement of Physics by his discovery of energy quanta 1920 Charles Edouard Guillaume, Sèvres, in recognition of the service he has rendered to precise measurements in Physics by his discovery of anoma- lies in nickel steel alloys 1921 Albert Einstein, Berlin, for services to Theoretical Physics, and especially for his discovery of the law of the photoelectric effect 1923 Robert Andrews Millikan, Pasadena, California, for his work on the ele- mentary charge of electricity and on the photo-electric effect 1924 Manne Siegbahn, Uppsala, for his discoveries and researches in the field of X-ray spectroscopy 1926 Jean Baptiste Perrin, Paris, for his work on the discontinuous structure of matter, and especially for his discovery of sedimentation equilibrium 1928 Owen Willans Richardson, London, for his work on the thermionic phe- nomenon and especially for his discovery of the law named after him 1929 Louis Victor de Broglie, Paris, for his discovery of the wave nature of electrons 1930 Venkata Raman, Calcutta, for his work on the scattering of light and for the discovery of the effect named after him © Springer International Publishing Switzerland 2015 199 R.P. -
A History of Quantum Chemistry
1 Quantum Chemistry qua Physics: The Promises and Deadlocks of Using First Principles In the opening paragraph of his 1929 paper “ Quantum Mechanics of Many-Electron Systems, ” Paul Adrien Maurice Dirac announced that: The general theory of quantum mechanics is now almost complete, the imperfections that still remain being in connection with the exact fi tting in of the theory with relativity ideas. These give rise to diffi culties only when high-speed particles are involved, and are therefore of no importance in the consideration of atomic and molecular structure and ordinary chemical reac- tions, in which it is, indeed, usually suffi ciently accurate if one neglects relativity variation of mass with velocity and assumes only Coulomb forces between the various electrons and atomic nuclei. The underlying physical laws necessary for the mathematical theory of a large part of physics and the whole of chemistry are thus completely known, and the diffi culty is only that the exact applica- tion of these laws leads to equations much too complicated to be soluble. It therefore becomes desirable that approximate practical methods of applying quantum mechanics should be developed, which can lead to an explanation of the main features of complex atomic systems without too much computation. (Dirac 1929, 714, emphasis ours) For most members of the community of physicists, it appeared that the solution of chemical problems amounted to no more than quantum-mechanical calculations. Physicists came under the spell of Dirac ’ s reductionist program, and quantum chem- istry came to be usually regarded as a success story of quantum mechanics. -
On the Verge of Umdeutung in Minnesota: Van Vleck and the Correspondence Principle. Part One. ?
On the verge of Umdeutung in Minnesota: Van Vleck and the correspondence principle. Part One. ? Anthony Duncan a, Michel Janssen b,∗ aDepartment of Physics and Astronomy, University of Pittsburgh bProgram in the History of Science, Technology, and Medicine, University of Minnesota Abstract In October 1924, The Physical Review, a relatively minor journal at the time, pub- lished a remarkable two-part paper by John H. Van Vleck, working in virtual iso- lation at the University of Minnesota. Using Bohr’s correspondence principle and Einstein’s quantum theory of radiation along with advanced techniques from classi- cal mechanics, Van Vleck showed that quantum formulae for emission, absorption, and dispersion of radiation merge with their classical counterparts in the limit of high quantum numbers. For modern readers Van Vleck’s paper is much easier to follow than the famous paper by Kramers and Heisenberg on dispersion theory, which covers similar terrain and is widely credited to have led directly to Heisen- berg’s Umdeutung paper. This makes Van Vleck’s paper extremely valuable for the reconstruction of the genesis of matrix mechanics. It also makes it tempting to ask why Van Vleck did not take the next step and develop matrix mechanics himself. Key words: Dispersion theory, John H. Van Vleck, Correspondence Principle, Bohr-Kramers-Slater (BKS) theory, Virtual oscillators, Matrix mechanics ? This paper was written as part of a joint project in the history of quantum physics of the Max Planck Institut f¨ur Wissenschaftsgeschichte and the Fritz-Haber-Institut in Berlin. ∗ Corresponding author. Address: Tate Laboratory of Physics, 116 Church St.