Where Astronomy Meets Particle Physics
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Nuclear Technology
Nuclear Technology Joseph A. Angelo, Jr. GREENWOOD PRESS NUCLEAR TECHNOLOGY Sourcebooks in Modern Technology Space Technology Joseph A. Angelo, Jr. Sourcebooks in Modern Technology Nuclear Technology Joseph A. Angelo, Jr. GREENWOOD PRESS Westport, Connecticut • London Library of Congress Cataloging-in-Publication Data Angelo, Joseph A. Nuclear technology / Joseph A. Angelo, Jr. p. cm.—(Sourcebooks in modern technology) Includes index. ISBN 1–57356–336–6 (alk. paper) 1. Nuclear engineering. I. Title. II. Series. TK9145.A55 2004 621.48—dc22 2004011238 British Library Cataloguing in Publication Data is available. Copyright © 2004 by Joseph A. Angelo, Jr. All rights reserved. No portion of this book may be reproduced, by any process or technique, without the express written consent of the publisher. Library of Congress Catalog Card Number: 2004011238 ISBN: 1–57356–336–6 First published in 2004 Greenwood Press, 88 Post Road West, Westport, CT 06881 An imprint of Greenwood Publishing Group, Inc. www.greenwood.com Printed in the United States of America The paper used in this book complies with the Permanent Paper Standard issued by the National Information Standards Organization (Z39.48–1984). 10987654321 To my wife, Joan—a wonderful companion and soul mate Contents Preface ix Chapter 1. History of Nuclear Technology and Science 1 Chapter 2. Chronology of Nuclear Technology 65 Chapter 3. Profiles of Nuclear Technology Pioneers, Visionaries, and Advocates 95 Chapter 4. How Nuclear Technology Works 155 Chapter 5. Impact 315 Chapter 6. Issues 375 Chapter 7. The Future of Nuclear Technology 443 Chapter 8. Glossary of Terms Used in Nuclear Technology 485 Chapter 9. Associations 539 Chapter 10. -
Cosmic Questions, Answers Pending
special section | cosmic questions, Answers pending Cosmic questions, answers pending throughout human history, great missions of mission reveal the exploration have been inspired by curiosity, : the desire to find out about unknown realms. secrets of the universe such missions have taken explorers across wide oceans and far below their surfaces, THE OBJECTIVE deep into jungles, high onto mountain peaks For millennia, people have turned to the heavens in search of clues to nature’s mysteries. truth seekers from ages past to the present day and over vast stretches of ice to the earth’s have found that the earth is not the center of the universe, that polar extremities. countless galaxies dot the abyss of space, that an unknown form of today’s greatest exploratory mission is no matter and dark forces are at work in shaping the cosmos. Yet despite longer earthbound. it’s the scientific quest to these heroic efforts, big cosmological questions remain unresolved: explain the cosmos, to answer the grandest What happened before the Big Bang? ............................... Page 22 questions about the universe as a whole. What is the universe made of? ......................................... Page 24 what is the identity, for example, of the Is there a theory of everything? ....................................... Page 26 Are space and time fundamental? .................................... Page 28 “dark” ingredients in the cosmic recipe, com- What is the fate of the universe? ..................................... Page 30 posing 95 percent of the -
Against Transhumanism the Delusion of Technological Transcendence
Edition 1.0 Against Transhumanism The delusion of technological transcendence Richard A.L. Jones Preface About the author Richard Jones has written extensively on both the technical aspects of nanotechnology and its social and ethical implications; his book “Soft Machines: nanotechnology and life” is published by OUP. He has a first degree and PhD in physics from the University of Cam- bridge; after postdoctoral work at Cornell University he has held positions as Lecturer in Physics at Cambridge University and Profes- sor of Physics at Sheffield. His work as an experimental physicist concentrates on the properties of biological and synthetic macro- molecules at interfaces; he was elected a Fellow of the Royal Society in 2006 and was awarded the Institute of Physics’s Tabor Medal for Nanoscience in 2009. His blog, on nanotechnology and science policy, can be found at Soft Machines. About this ebook This short work brings together some pieces that have previously appeared on my blog Soft Machines (chapters 2,4 and 5). Chapter 3 is adapted from an early draft of a piece that, in a much revised form, appeared in a special issue of the magazine IEEE Spectrum de- voted to the Singularity, under the title “Rupturing the Nanotech Rapture”. Version 1.0, 15 January 2016 The cover picture is The Ascension, by Benjamin West (1801). Source: Wikimedia Commons ii Transhumanism, technological change, and the Singularity 1 Rapid technological progress – progress that is obvious by setting off a runaway climate change event, that it will be no on the scale of an individual lifetime - is something we take longer compatible with civilization. -
The Matter – Antimatter Asymmetry of the Universe and Baryogenesis
The matter – antimatter asymmetry of the universe and baryogenesis Andrew Long Lecture for KICP Cosmology Class Feb 16, 2017 Baryogenesis Reviews in General • Kolb & Wolfram’s Baryon Number Genera.on in the Early Universe (1979) • Rio5o's Theories of Baryogenesis [hep-ph/9807454]} (emphasis on GUT-BG and EW-BG) • Rio5o & Trodden's Recent Progress in Baryogenesis [hep-ph/9901362] (touches on EWBG, GUTBG, and ADBG) • Dine & Kusenko The Origin of the Ma?er-An.ma?er Asymmetry [hep-ph/ 0303065] (emphasis on Affleck-Dine BG) • Cline's Baryogenesis [hep-ph/0609145] (emphasis on EW-BG; cartoons!) Leptogenesis Reviews • Buchmuller, Di Bari, & Plumacher’s Leptogenesis for PeDestrians, [hep-ph/ 0401240] • Buchmulcer, Peccei, & Yanagida's Leptogenesis as the Origin of Ma?er, [hep-ph/ 0502169] Electroweak Baryogenesis Reviews • Cohen, Kaplan, & Nelson's Progress in Electroweak Baryogenesis, [hep-ph/ 9302210] • Trodden's Electroweak Baryogenesis, [hep-ph/9803479] • Petropoulos's Baryogenesis at the Electroweak Phase Transi.on, [hep-ph/ 0304275] • Morrissey & Ramsey-Musolf Electroweak Baryogenesis, [hep-ph/1206.2942] • Konstandin's Quantum Transport anD Electroweak Baryogenesis, [hep-ph/ 1302.6713] Constituents of the Universe formaon of large scale structure (galaxy clusters) stars, planets, dust, people late ame accelerated expansion Image stolen from the Planck website What does “ordinary matter” refer to? Let’s break it down to elementary particles & compare number densities … electron equal, universe is neutral proton x10 billion 3⇣(3) 3 3 n =3 T 168 cm− neutron x7 ⌫ ⇥ 4⇡2 ⌫ ' matter neutrinos photon positron =0 2⇣(3) 3 3 n = T 413 cm− γ ⇡2 CMB ' anti-proton =0 3⇣(3) 3 3 anti-neutron =0 n =3 T 168 cm− ⌫¯ ⇥ 4⇡2 ⌫ ' anti-neutrinos antimatter What is antimatter? First predicted by Dirac (1928). -
Scalar Correlation Functions in De Sitter Space from the Stochastic Spectral Expansion
IMPERIAL/TP/2019/TM/03 Scalar correlation functions in de Sitter space from the stochastic spectral expansion Tommi Markkanena;b , Arttu Rajantiea , Stephen Stopyrac and Tommi Tenkanend aDepartment of Physics, Imperial College London, Blackett Laboratory, London, SW7 2AZ, United Kingdom bLaboratory of High Energy and Computational Physics, National Institute of Chemical Physics and Biophysics, R¨avala pst. 10, Tallinn, 10143, Estonia cDepartment of Physics and Astronomy, UCL, Gower Street, London WC1E 6BT, United Kingdom dDepartment of Physics and Astronomy, Johns Hopkins University, Baltimore, MD 21218, United States of America E-mail: [email protected], tommi.markkanen@kbfi.ee, [email protected], [email protected], [email protected] Abstract. We consider light scalar fields during inflation and show how the stochastic spec- tral expansion method can be used to calculate two-point correlation functions of an arbitrary local function of the field in de Sitter space. In particular, we use this approach for a massive scalar field with quartic self-interactions to calculate the fluctuation spectrum of the density contrast and compare it to other approximations. We find that neither Gaussian nor linear arXiv:1904.11917v2 [gr-qc] 1 Aug 2019 approximations accurately reproduce the power spectrum, and in fact always overestimate it. For example, for a scalar field with only a quartic term in the potential, V = λφ4=4, we find a blue spectrum with spectral index n 1 = 0:579pλ. − Contents 1 Introduction1 2 The stochastic approach2 2.1 -
Top 10 Discoveries by ESO Telescopes
Top 10 Discoveries by ESO Telescopes • European Southern Observatory – reaching new heights in astronomy • Exploring the Universe from the Atacama Desert, in Chile since 1964 • ESO is the most productive astronomical observatory in the world TOP 10 discoveries by ESO telescopes, 26 April 2011 La Silla Observatory: ESO’s first observatory • Two of the most productive 4-metre class telescopes in the world – ESO 3.6-metre telescope, since 1976 – The New Technology Telescope (NTT, 3.58 m), since 1989 • 300 refereed publications per year TOP 10 discoveries by ESO telescopes, 26 April 2011 ESO’s top 10 discoveries 1. Stars orbiting the Milky Way black hole 2. Accelerating Universe 3. First image of an exoplanet 4. Gamma-ray bursts — the connections with supernovae and merging neutron stars 5. Cosmic temperature independently measured 6. Oldest star known in the Milky Way 7. Flares from the supermassive black hole at the centre of the Milky Way 8. Direct measurements of the spectra of exoplanets and their atmospheres 9. Richest planetary system 10. Milky Way stellar motions More info in: http://www.eso.org/public/science/top10.html TOP 10 discoveries by ESO telescopes, 26 April 2011 1. Stars orbiting the Milky Way black hole TOP 10 discoveries by ESO telescopes, 26 April 2011 1. Stars orbiting the Milky Way black hole • The discovery: unprecedented 16-year long study tracks stars orbiting the Milky Way black hole • When: a 16-year long campaign started in 1992, with 50 nights of observations in total • Instruments / telescopes: – SHARP / NTT, La Silla Observatory – NACO / Yepun (UT4), VLT • More info in press releases eso0226 and eso0846: http://www.eso.org/public/news/eso0226/ http://www.eso.org/public/news/eso0846/ TOP 10 discoveries by ESO telescopes, 26 April 2011 1. -
Resumo Dos V´Ideos Propostos De F740
Resumo dos V´ıdeosPropostos de F740 - Grupo 2 Gabriel Martins (197328), Ian Barboza (174822), Anderson Pitoli (166188) Junho 2020 1 Atom: Clash of Titans - Ep. 1 Neste epis´odio,´ediscorrida a hist´oriada teoria at^omicano s´eculo20, desde seus prim´ordios at´esuas considera¸c~oesatuais. No final do s´eculo19, tal teoria n~aoera de interesse da comunidade cient´ıfica,visto que ate ent~aon~aoparecia ter utilidade pr´atica;foi com o surgimento de motores `avapor que as aten¸c~oes se voltaram a esse campo de estudo, buscando uma maior efici^enciados gases utilizados. A prova de exist^enciado ´atomoveio atrav´esde Einstein em 1907, visando explicar a vibra¸c~aodas part´ıculasde p´olenem ´agua,e a partir da´ı, come¸cou-sea especula¸c~aode como tais ´atomosseriam e como se comportariam. O primeiro modelo que aparece no document´ariofoi o de Rutherford, que afirmava que toda a carga positiva do ´atomo,e portanto toda sua massa, est´a concentrada em seu centro, numa regi~aochamada de n´ucleo,que era cerca de 100.000 vezes menor que a elestrosfera que o cobria. O modelo resultou dos experimentos com a radia¸c~ao,particularmente a radia¸c~aoalfa, e sua reflex˜ao em uma folha de ouro. Por´em,havia um fen^omenoque n~aopodia ser explicado pelo modelo de Rutherford, as linhas espectrais observadas ao energizar gases. Niels Bohr cria ent~aoseu modelo, junto com a ´areade estudo que ficou conhecida como mec^anicaqu^antica, ele utilizava a teoria de saltos qu^anticos, que dizia que as linhas espectrais aconteciam devido `alibera¸c~aode energia na forma de radia¸c~aoem saltos que os el´etronsrealizavam entre suas poss´ıveis ´orbitas. -
Outline of Lecture 2 Baryon Asymmetry of the Universe. What's
Outline of Lecture 2 Baryon asymmetry of the Universe. What’s the problem? Electroweak baryogenesis. Electroweak baryon number violation Electroweak transition What can make electroweak mechanism work? Dark energy Baryon asymmetry of the Universe There is matter and no antimatter in the present Universe. Baryon-to-photon ratio, almost constant in time: nB 10 ηB = 6 10− ≡ nγ · Baryon-to-entropy, constant in time: n /s = 0.9 10 10 B · − What’s the problem? Early Universe (T > 1012 K = 100 MeV): creation and annihilation of quark-antiquark pairs ⇒ n ,n n q q¯ ≈ γ Hence nq nq¯ 9 − 10− nq + nq¯ ∼ How was this excess generated in the course of the cosmological evolution? Sakharov conditions To generate baryon asymmetry, three necessary conditions should be met at the same cosmological epoch: B-violation C-andCP-violation Thermal inequilibrium NB. Reservation: L-violation with B-conservation at T 100 GeV would do as well = Leptogenesis. & ⇒ Can baryon asymmetry be due to electroweak physics? Baryon number is violated in electroweak interactions. Non-perturbative effect Hint: triangle anomaly in baryonic current Bµ : 2 µ 1 gW µνλρ a a ∂ B = 3colors 3generations ε F F µ 3 · · · 32π2 µν λρ ! "Bq a Fµν: SU(2)W field strength; gW : SU(2)W coupling Likewise, each leptonic current (n = e, µ,τ) g2 ∂ Lµ = W ε µνλρFa Fa µ n 32π2 · µν λρ a 1 Large field fluctuations, Fµν ∝ gW− may have g2 Q d3xdt W ε µνλρFa Fa = 0 ≡ 32 2 · µν λρ ' # π Then B B = d3xdt ∂ Bµ =3Q fin− in µ # Likewise L L =Q n, fin− n, in B is violated, B L is not. -
What Did the Early Universe Look Like? Key Stage 5
1 What did the early Universe look like? Key Stage 5 Topics covered: Cosmic Microwave Background Radiation, Wien’s displacement law, Doppler Effect Watch the video “What makes the Universe colourful?” https://vimeo.com/213990458 Scientists theorise that the Universe began with the Big Bang around 13.8 billion years ago. Space has been expanding ever since and the initial Big Bang energy has spread out. As a result the temperature of the Universe has fallen and the wavelength of light has stretched out. The history of the Universe can be split into different epochs – see the handout ‘TIMELINE OF THE UNIVERSE’. If we treat the Universe as a black body* then we can work out the peak wavelength of light travelling through the Universe at different epochs by using Wien’s law: 2.898 × 10−3 휆 = 푚푎푥 푇 휆푚푎푥 – peak wavelength emitted by the black body (m - metres) 푇 – temperature of the black body (K – Kelvin) * A black body is an ideal case of an object or system which perfectly absorbs and emits radiation and light and does not reflect any of it. 2 1. Use the ‘TIMELINE OF THE UNIVERSE’ handout to help. For each of the following epochs: 350,000 years (t1 - near the end of the photon epoch) 380,000 years (t2 - at recombination) 13.8 billion years (t3 - present day) a) Complete the table below to work out the peak wavelength (휆푚푎푥) of light that would be travelling through the Universe at that time. epoch Temperature Peak wavelength t1 350,000 years t2 380,000 years t3 13.8 billion years b) Mark these three wavelengths (as vertical lines / arrows) on the diagram below as t1, t2 and t3. -
SUMMARY. Part I: the Fractal 5D Organic Universe. I. the Fractal Universe, Its 5D Metric
SUMMARY. Part I: The Fractal 5D Organic Universe. I. The fractal Universe, its 5D Metric. II. Leibniz vs. Newton: Vital, Topologic Space. Its 3±¡ Dimotions. III. Absolute relativity. S=T. The Galilean Paradox. IV. The 5 Postulates of Non-Euclidean, Non-Aristotelian, vital topology V. Cyclical time. Its 3 ages=states of matter. Worldcycles of existence. VI. The Stientific method. Planes of Formal Stiences :¡logic, existential Algebra Part II: Astrophysics. ∆+4,3 scales: Cosmology & Astrophysics: Scalar big-bangs. Galatoms. Hyper-universe. I. Falsifications of the cosmic big-bang. Æntropic man: Science is culture. II. The little bang. III. The ages of the galaxy . IV The ‘Galatom’: Scalar Unification of the 5 forces as Dimotions of the galaxy. V. The ‘Galacell’: A galactic organism. Its symmetries of scale and topologies in space. VI. Light Stars, its topologic, organic parts. VII. Black stars. Thermodynamics of black holes. ∆-4,3 scales: Quantum physics. Comments on the right model. I. Broglie’s theory. 1 5TH DIMENSION METRIC AND THE NESTED UNIVERSE. When we google the 5th dimension one gets surprised by the quantity of speculative answers to a question, which is no longer pseudo- science, but has been for two decades a field of research in systems sciences rather than physics (: no, the answers of google, considering the fifth dimension the upper-self etc. seem to be very popular, but are to 5D science more like a medium in earlier XX c. talking about the 4th dimension as astrological awareness, for lack of understanding of Einstein’s metric functions of the 4th dimension). This is the key word that differentiates pseudo-science from a proper scientific description of a dimension of space-time, the existence of a metric function that describes a dimension and allows to travel through it. -
Cosmology and Dark Matter Lecture 3
1 Cosmology and Dark Matter V.A. Rubakov Lecture 3 2 Outline of Lecture 3 Baryon asymmetry of the Universe Generalities. Electroweak baryon number non-conservation What can make electroweak mechanism work? Leptogenesis and neutrino masses Before the hot epoch 3 Baryon asymmetry of the Universe There is matter and no antimatter in the present Universe. Baryon-to-photon ratio, almost constant in time: nB 10 ηB = 6 10− ≡ nγ · 10 Baryon-to-entropy, constant in time: nB/s = 0.9 10 · − What’s the problem? Early Universe (T > 1012 K = 100 MeV): creation and annihilation of quark-antiquark pairs nq,nq¯ nγ Hence ⇒ ≈ nq nq¯ 9 − 10− nq + nq¯ ∼ Very unlikely that this excess is initial condition. Certainly not, if inflation. How was this excess generated in the course of the cosmological evolution? Sakharov’67, Kuzmin’70 4 Sakharov conditions To generate baryon asymmetry from symmetric initial state, three necessary conditions should be met at the same cosmological epoch: B-violation C- and CP-violation Thermal inequilibrium NB. Reservation: L-violation with B-conservation at T 100 GeV would do as well = Leptogenesis. ≫ ⇒ Can baryon asymmetry be due to 5 electroweak physics? Baryon number is violated in electroweak interactions. “Sphalerons”. Non-perturbative effect Hint: triangle anomaly in baryonic current Bµ : 2 µ 1 gW µνλρ a a ∂µ B = 3 3 ε Fµν F 3 colors generations 32π2 λρ Bq · · · a Fµν : SU(2)W field strength; gW : SU(2)W coupling Likewise, each leptonic current (n = e, µ,τ) 2 µ gW µνλρ a a ∂µ L = ε Fµν Fλρ n 32π2 · B is violated, B L B Le Lµ Lτ is not. -
Hot Big Bang Model: Early Universe and History of Matter Initial „Soup“ with Elementary Particles and Radiation in Thermal Equilibrium
Hot Big Bang model: early Universe and history of matter Initial „soup“ with elementary particles and radiation in thermal equilibrium. Radiation dominated era (recall energy density grows faster than matter density going back in time (~ a-4 rather than a-3). Thermal equilbrium maintained by electroweak interactions between individual particle species and between them and radiation field --- interaction rate G=n<vs>, where n is the number density of a type of particles, s the cross section and v the relative velocity (s depends on v in general). Key concepts: (1) At any given time particles can be created if their rest mass energy is such that kBT >> mc2, where T is the temperature of radiation. As the Universe expands T ~ a-1 (radiation dominated) so only increasingly lighter particles can be created. Important example: pair production from g + g < - -> e- + e+ (requires T > 5.8 x 109 K), which Immediately thermalize with electrons via Compton scattering and produce electronic - neutrinos via e- + e+ < --> ne + n e , also in thermal equilibrium with radiation. (2) As the Universe expands G decreases because n and v decrease -! when G < H(t) particle species decouples from photon fluid and n „freezes-out“ to the value at first decoupling(subsequently diluted only by expansion of Universe if particle stable). Present-day elementary particles are „thermal relics“ that have decoupled from photon 2 fluid at different times, some when they were still relativistic („hot relics“, kBT >> mc , T 2 is temperature of radiation field), some when they were non-relativistic (kBT <<mc ,“cold relics“) In the early Universe the very high temperatures (T ~ 1010 K a t ~ 1 s) guarantee that all elementary particles are relativistic and in thermal equilibrium with radiation.