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Computing ATOMIC NUCLEI
UNIVERSAL NUCLEAR ENERGY DENSITY FUNCTIONAL Computing ATOMIC NUCLEI Petascale computing helps disentangle the nuclear puzzle. The goal of the Universal Nuclear Energy Density Functional (UNEDF) collaboration is to provide a comprehensive description of all nuclei and their reactions based on the most accurate knowledge of the nuclear interaction, the most reliable theoretical approaches, and the massive use of computer power. Science of Nuclei the Hamiltonian matrix. Coupled cluster (CC) Nuclei comprise 99.9% of all baryonic matter in techniques, which were formulated by nuclear sci- the Universe and are the fuel that burns in stars. entists in the 1950s, are essential techniques in The rather complex nature of the nuclear forces chemistry today and have recently been resurgent among protons and neutrons generates a broad in nuclear structure. Quantum Monte Carlo tech- range and diversity in the nuclear phenomena that niques dominate studies of phase transitions in can be observed. As shown during the last decade, spin systems and nuclei. These methods are used developing a comprehensive description of all to understand both the nuclear and electronic nuclei and their reactions requires theoretical and equations of state in condensed systems, and they experimental investigations of rare isotopes with are used to investigate the excitation spectra in unusual neutron-to-proton ratios. These nuclei nuclei, atoms, and molecules. are labeled exotic, or rare, because they are not When applied to systems with many active par- typically found on Earth. They are difficult to pro- ticles, ab initio and configuration interaction duce experimentally because they usually have methods present computational challenges as the extremely short lifetimes. -
Nuclear Data
CNIC-00810 CNDC-0013 INDC(CPR)-031/L NUCLEAR DATA No. 10 (1993) China Nuclear Information Center Chinese Nuclear Data Center Atomic Energy Press CNIC-00810 CNDC-0013 INDC(CPR)-031/L COMMUNICATION OF NUCLEAR DATA PROGRESS No. 10 (1993) Chinese Nuclear Data Center China Nuclear Information Centre Atomic Energy Press Beijing, December 1993 EDITORIAL BOARD Editor-in-Chief Liu Tingjin Zhuang Youxiang Member Cai Chonghai Cai Dunjiu Chen Zhenpeng Huang Houkun Liu Tingjin Ma Gonggui Shen Qingbiao Tang Guoyou Tang Hongqing Wang Yansen Wang Yaoqing Zhang Jingshang Zhang Xianqing Zhuang Youxiang Editorial Department Li Manli Sun Naihong Li Shuzhen EDITORIAL NOTE This is the tenth issue of Communication of Nuclear Data Progress (CNDP), in which the achievements in nuclear data field since the last year in China are carried. It includes the measurements of 54Fe(d,a), 56Fe(d,2n), 58Ni(d,a), (d,an), (d,x)57Ni, 182~ 184W(d,2n), 186W(d,p), (d,2n) and S8Ni(n,a) reactions; theoretical calculations on n+160 and ,97Au, 10B(n,n) and (n,n') reac tions, channel theory of fission with diffusive dynamics; the evaluations of in termediate energy nuclear data for 56Fe, 63Cu, 65Cu(p,n) monitor reactions, and of 180Hf, ,8lTa(n,2n) reactions, revision on recommended data of 235U and 238U for CENDL-2; fission barrier parameters sublibrary, a PC software of EXFOR compilation, some reports on atomic and molecular data and covariance research. We hope that our readers and colleagues will not spare their comments, in order to improve the publication. Please write to Drs. -
Nuclear Data Library for Incident Proton Energies to 150 Mev
LA-UR-00-1067 Approved for public release; distribution is unlimited. 7Li(p,n) Nuclear Data Library for Incident Proton Title: Energies to 150 MeV Author(s): S. G. Mashnik, M. B. Chadwick, P. G. Young, R. E. MacFarlane, and L. S. Waters Submitted to: http://lib-www.lanl.gov/la-pubs/00393814.pdf Los Alamos National Laboratory, an affirmative action/equal opportunity employer, is operated by the University of California for the U.S. Department of Energy under contract W-7405-ENG-36. By acceptance of this article, the publisher recognizes that the U.S. Government retains a nonexclusive, royalty- free license to publish or reproduce the published form of this contribution, or to allow others to do so, for U.S. Government purposes. Los Alamos National Laboratory requests that the publisher identify this article as work performed under the auspices of the U.S. Department of Energy. Los Alamos National Laboratory strongly supports academic freedom and a researcher's right to publish; as an institution, however, the Laboratory does not endorse the viewpoint of a publication or guarantee its technical correctness. FORM 836 (10/96) Li(p,n) Nuclear Data Library for Incident Proton Energies to 150 MeV S. G. Mashnik, M. B. Chadwick, P. G. Young, R. E. MacFarlane, and L. S. Waters Los Alamos National Laboratory, Los Alamos, NM 87545 Abstract Researchers at Los Alamos National Laboratory are considering the possibility of using the Low Energy Demonstration Accelerator (LEDA), constructed at LANSCE for the Ac- celerator Production of Tritium program (APT), as a neutron source. Evaluated nuclear data are needed for the p+ ¡ Li reaction, to predict neutron production from thin and thick lithium targets. -
Nuclear Energy Agency Nuclear Data Committee
NUCLEAR ENERGY AGENCY NUCLEAR DATA COMMITTEE SUMMARY RECORD OF THE lWEEFPY-FIRST MEETING (Technical Sessions) CBNM, Gee1 (Belgium) 24th-28th September 1979 Compiled by C. COCEVA (Scientific Secretary) OECD NUCLEAR ENERGY AGENCY 38 Bd. Suchet, 75016 Paris TABLE OF CONTENTS TECHNICAL SESSIONS Participants in meeting 1. Isotopes 2. National Progress Reports 3. Meetings 4. Technical Discussions 5. Topical Meeting on "Progress in Neutron Data of Structural Materials for Fast ~eactors" 6. Neutron and Related Nuclear Data Compilations and Evaluations Appendices 1 Meetings of the IAEA/NDS planned for 1980, 1981 and 1982 2 Progranme of the Topical Meeting on "Progress in Neutron Data of Structural Materials for Fast Reactors " 3 Summary of the general discussion on the works presented at the Topical Meeting TECmTICAL SESSIONS Perticipants in the 21st Meeting were as follows : For Canada : Dr. W.G. Cross Atomic Energy of Canada Ltd. Chalk River For Japan : Dr. K. Tsukada Japan Atomic Energy Research Institute Tokai-blur a For the United States of America : Dr. R.E. Chrien (Chairman) Brookhaven National Laboratory Dr. S.L. Wl~etstone U.S. Department of Energy Dr. 8.T. Motz Los Alamos Scientific Laboratory Dr. F.G. Perey Oak Ridge National Laboratory For the countries of the European Communities and the European Commission acting together : Dr. R. Iiockhoff (Local Secretary) Central Bureau for Nuclear Pleasurements Geel, Belgium Dr. C. Coceva (Scientific Secretary) Comitato Nazionale per 1'Energia Nucleare Bologna, Italy Dr. S. Cierjacks Kernforschungszentrum Karlsruhe Federal Republic of Germany Dr. C. Fort Conunissariat i 1'Energie Atomique Cadaroche, France Dr. A. Michaudon (Vice-chairman) Commissariat 2 1'Energie Atomique Bruysrcs-1.e-ChZtel Dr. -
Experiment QM2: NMR Measurement of Nuclear Magnetic Moments
Physics 440 Spring (3) 2018 Experiment QM2: NMR Measurement of Nuclear Magnetic Moments Theoretical Background: Elementary particles are characterized by a set of properties including mass m, electric charge q, and magnetic moment µ. These same properties are also used to characterize bound collections of elementary particles such as the proton and neutron (which are built from quarks) and atomic nuclei (which are built from protons and neutrons). A particle's magnetic moment can be written in terms of spin as µ = g (q/2m) S where g is the "g-factor" for the particle and S is the particle spin. [Note 2 that for a classical rotating ball of charge S = (2mR /5) ω and g = 1]. For a nucleus, it is conventional to express the magnetic moment as µ A = gA µN IA /! where IA is the "spin", gA is the nuclear g-factor of nucleus A, and the constant µN = e!/2mp (where mp= proton mass) is known as the nuclear magneton. In a magnetic field (oriented in the z-direction) a spin-I nucleus can take on 2I+1 orientations with Iz = mI! where –I ≤ mI ≤ I. Such a nucleus experiences an orientation- dependent interaction energy of VB = –µ A•B = –(gA µN mI)Bz. Note that for a nucleus with positive g- factor the low energy state is the one in which the spin is aligned parallel to the magnetic field. For a spin-1/2 nucleus there are two allowed spin orientations, denoted spin-up and spin-down, and the up down energy difference between these states is simply given by |ΔVB| = VB −VB = 2µABz. -
Lecture #4, Matter/Energy Interactions, Emissions Spectra, Quantum Numbers
Welcome to 3.091 Lecture 4 September 16, 2009 Matter/Energy Interactions: Atomic Spectra 3.091 Periodic Table Quiz 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 88 89 Name Grade /10 Image by MIT OpenCourseWare. Rutherford-Geiger-Marsden experiment Image by MIT OpenCourseWare. Bohr Postulates for the Hydrogen Atom 1. Rutherford atom is correct 2. Classical EM theory not applicable to orbiting e- 3. Newtonian mechanics applicable to orbiting e- 4. Eelectron = Ekinetic + Epotential 5. e- energy quantized through its angular momentum: L = mvr = nh/2π, n = 1, 2, 3,… 6. Planck-Einstein relation applies to e- transitions: ΔE = Ef - Ei = hν = hc/λ c = νλ _ _ 24 1 18 Bohr magneton µΒ = eh/2me 9.274 015 4(31) X 10 J T 0.34 _ _ 27 1 19 Nuclear magneton µΝ = eh/2mp 5.050 786 6(17) X 10 J T 0.34 _ 2 3 20 Fine structure constant α = µ0ce /2h 7.297 353 08(33) X 10 0.045 21 Inverse fine structure constant 1/α 137.035 989 5(61) 0.045 _ 2 1 22 Rydberg constant R¥ = mecα /2h 10 973 731.534(13) m 0.0012 23 Rydberg constant in eV R¥ hc/{e} 13.605 698 1(40) eV 0.30 _ 10 24 Bohr radius a0 = a/4πR¥ 0.529 177 249(24) X 10 m 0.045 _ _ 4 2 1 25 Quantum of circulation h/2me 3.636 948 07(33) X 10 m s 0.089 _ 11 1 26 Electron specific charge -e/me -1.758 819 62(53) X 10 C kg 0.30 _ 12 27 Electron Compton wavelength λC = h/mec 2.426 310 58(22) X 10 m 0.089 _ 2 15 28 Electron classical radius re = α a0 2.817 940 92(38) X 10 m 0.13 _ _ 26 1 29 Electron magnetic moment` µe 928.477 01(31) X 10 J T 0.34 _ _ 3 30 Electron mag. -
The JEFF-3.1.1 Nuclear Data Library
Data Bank ISBN 978-92-64-99074-6 The JEFF-3.1.1 Nuclear Data Library JEFF Report 22 Validation Results from JEF-2.2 to JEFF-3.1.1 A. Santamarina, D. Bernard, P. Blaise, M. Coste, A. Courcelle, T.D. Huynh, C. Jouanne, P. Leconte, O. Litaize, S. Mengelle, G. Noguère, J-M. Ruggiéri, O. Sérot, J. Tommasi, C. Vaglio, J-F. Vidal Edited by A. Santamarina, D. Bernard, Y. Rugama © OECD 2009 NEA No. 6807 NUCLEAR ENERGY AGENCY Organisation for Economic Co-operation and Development ORGANISATION FOR ECONOMIC CO-OPERATION AND DEVELOPMENT The OECD is a unique forum where the governments of 30 democracies work together to address the economic, social and environmental challenges of globalisation. The OECD is also at the forefront of efforts to understand and to help governments respond to new developments and concerns, such as corporate governance, the information economy and the challenges of an ageing population. The Organisation provides a setting where governments can compare policy experiences, seek answers to common problems, identify good practice and work to co-ordinate domestic and international policies. The OECD member countries are: Australia, Austria, Belgium, Canada, the Czech Republic, Denmark, Finland, France, Germany, Greece, Hungary, Iceland, Ireland, Italy, Japan, Korea, Luxembourg, Mexico, the Netherlands, New Zealand, Norway, Poland, Portugal, the Slovak Republic, Spain, Sweden, Switzerland, Turkey, the United Kingdom and the United States. The Commission of the European Communities takes part in the work of the OECD. OECD Publishing disseminates widely the results of the Organisation’s statistics gathering and research on economic, social and environmental issues, as well as the conventions, guidelines and standards agreed by its members. -
The G Factor of Proton
The g factor of proton Savely G. Karshenboim a,b and Vladimir G. Ivanov c,a aD. I. Mendeleev Institute for Metrology (VNIIM), St. Petersburg 198005, Russia bMax-Planck-Institut f¨ur Quantenoptik, 85748 Garching, Germany cPulkovo Observatory, 196140, St. Petersburg, Russia Abstract We consider higher order corrections to the g factor of a bound proton in hydrogen atom and their consequences for a magnetic moment of free and bound proton and deuteron as well as some other objects. Key words: Nuclear magnetic moments, Quantum electrodynamics, g factor, Two-body atoms PACS: 12.20.Ds, 14.20.Dh, 31.30.Jv, 32.10.Dk Investigation of electromagnetic properties of particles and nuclei provides important information on fundamental constants. In addition, one can also learn about interactions of bound particles within atoms and interactions of atomic (molecular) composites with the media where the atom (molecule) is located. Since the magnetic interaction is weak, it can be used as a probe to arXiv:hep-ph/0306015v1 2 Jun 2003 learn about atomic and molecular composites without destroying the atom or molecule. In particular, an important quantity to study is a magnetic moment for either a bare nucleus or a nucleus surrounded by electrons. The Hamiltonian for the interaction of a magnetic moment µ with a homoge- neous magnetic field B has a well known form Hmagn = −µ · B , (1) which corresponds to a spin precession frequency µ hν = B , (2) spin I Email address: [email protected] (Savely G. Karshenboim). Preprint submitted to Elsevier Science 1 February 2008 where I is the related spin equal to either 1/2 or 1 for particles and nuclei under consideration in this paper. -
Deuterium Magnetic Resonance: Theory and Application to Lipid Membranes
Quarterly Reviews of Biophysics 10, 3 (1977), pp. 353-418. Printed in Great Britain Deuterium magnetic resonance: theory and application to lipid membranes JOACHIM SEELIG Department of Biophysical Chemistry, Biocenter of the University of Basel, Klingelbergstrasse 70, C//-4056 Basel, Switzerland I. INTRODUCTION 345 II. THEORY OF DEUTERIUM MAGNETIC RESONANCE 358 A. Deuterium magnetic resonance in the absence of molecular motion 358 1. General theory 358 2. Rotation of the coordinate system 359 3. Principal coordinate system 360 4. Energy levels 362 5. Lineshapes of polycrystalline samples 364 B. Deuterium magnetic resonance of liquid crystals 369 1. Anisotropic motions in liquid crystals 369 2. Deuterium-order parameters in planar-oriented liquid crystals 373 3. Lineshapes for random and cylindrical distributions of liquid crystalline microdomains 377 4. Anisotropic rotation of CD2 and CD3 groups 383 5. Deuterium quadrupole relaxation in anisotropic media 386 III. APPLICATION OF DEUTERIUM MAGNETIC RESONANCE TO LIPID MEMBRANES 388 A. Lipid bilayers composed of soap molecules 388 B. Phospholipid bilayers 393 1. Hydrocarbon region 394 2. Structure and flexibility of the polar head groups 405 REFERENCES 411 23-2 Downloaded from https://www.cambridge.org/core. WWZ Bibliothek, on 14 Nov 2017 at 10:27:10, subject to the Cambridge Core terms of use, available at https://www.cambridge.org/core/terms. https://doi.org/10.1017/S0033583500002948 354 J- SEELIG I. INTRODUCTION Proton and carbon-13 nmr spectra of unsonicated lipid bilayers and biological membranes are generally dominated by strong proton-proton and proton-carbon dipolar interactions. As a result the spectra contain a large number of overlapping resonances and are rather difficult to analyse. -
1. Physical Constants 101
1. Physical constants 101 1. PHYSICAL CONSTANTS Table 1.1. Reviewed 2010 by P.J. Mohr (NIST). Mainly from the “CODATA Recommended Values of the Fundamental Physical Constants: 2006” by P.J. Mohr, B.N. Taylor, and D.B. Newell in Rev. Mod. Phys. 80 (2008) 633. The last group of constants (beginning with the Fermi coupling constant) comes from the Particle Data Group. The figures in parentheses after the values give the 1-standard-deviation uncertainties in the last digits; the corresponding fractional uncertainties in parts per 109 (ppb) are given in the last column. This set of constants (aside from the last group) is recommended for international use by CODATA (the Committee on Data for Science and Technology). The full 2006 CODATA set of constants may be found at http://physics.nist.gov/constants. See also P.J. Mohr and D.B. Newell, “Resource Letter FC-1: The Physics of Fundamental Constants,” Am. J. Phys, 78 (2010) 338. Quantity Symbol, equation Value Uncertainty (ppb) speed of light in vacuum c 299 792 458 m s−1 exact∗ Planck constant h 6.626 068 96(33)×10−34 Js 50 Planck constant, reduced ≡ h/2π 1.054 571 628(53)×10−34 Js 50 = 6.582 118 99(16)×10−22 MeV s 25 electron charge magnitude e 1.602 176 487(40)×10−19 C = 4.803 204 27(12)×10−10 esu 25, 25 conversion constant c 197.326 9631(49) MeV fm 25 conversion constant (c)2 0.389 379 304(19) GeV2 mbarn 50 2 −31 electron mass me 0.510 998 910(13) MeV/c = 9.109 382 15(45)×10 kg 25, 50 2 −27 proton mass mp 938.272 013(23) MeV/c = 1.672 621 637(83)×10 kg 25, 50 = 1.007 276 466 77(10) u = 1836.152 672 47(80) me 0.10, 0.43 2 deuteron mass md 1875.612 793(47) MeV/c 25 12 2 −27 unified atomic mass unit (u) (mass C atom)/12 = (1 g)/(NA mol) 931.494 028(23) MeV/c = 1.660 538 782(83)×10 kg 25, 50 2 −12 −1 permittivity of free space 0 =1/μ0c 8.854 187 817 .. -
Binding Blocks: Building the Universe One Nucleus at the Time
Binding Blocks: building the Universe one nucleus at the time C. Aa. Diget, A. Pastore, K. Leech, T. Haylett , S. Lock, T. Sanders, M. Shelley, H. V. Willett, Department of Physics, University of York, Heslington, York, Y010 5DD, United Kingdom J. Keegans, E.A. Milne Centre for Astrophysics School of Mathematics and Physical Sciences, University of Hull, Hull, HU6 7RX, United Kingdom L. Sinclair, Castle Hill Hospital, Cottingham, HU16 5JQ, United Kingdom E. C. Simpson, Department of Nuclear Physics, Research School of Physics and Engineering, The Australian National University, Canberra ACT 2601, Australia and the Binding Blocks collaboration #JOEJOH #JOEJOH #JOEJOH #MPDLT #MPDLT #MPDLT #VJMEJOHUIF6OJWFSTF #VJMEJOHUIF6OJWFSTF #VJMEJOHUIF6OJWFSTF E-mail: [email protected] POFOVDMFVTBUBUJNF POFOVDMFVTBUBUJNF POFOVDMFVTBUBUJNF Abstract. We present a new teaching and outreach activity based around the construction of a three-dimensional chart of isotopes using LEGOr bricksz. The activity, Binding Blocks, demonstrates nuclear and astrophysical processes through a seven-meter chart of all nuclear isotopes, built from over 26,000 LEGOr bricks. It integrates A-level and GCSE curricula across areas of nuclear physics, astrophysics, arXiv:1610.02296v2 [physics.ed-ph] 18 Oct 2016 and chemistry, including: nuclear decays (through the colours in the chart); nuclear binding energy (through tower heights); production of chemical elements in the cosmos; fusion processes in stars and fusion energy on Earth; as well as links to medical physics, particularly diagnostics and radiotherapy. z LEGOr is a trademark of the LEGO Group of companies which does not sponsor, authorise or endorse the present work. Binding Blocks: building the Universe one nucleus at the time 2 1. -
Overview of Nuclear Data
Overview of Nuclear Data Michal Herman National Nuclear Data Center Brookhaven National Laboratory Nuclear Data Program Link between basic science and applications Nuclear Science Community ✦ experiments Eur. Phys.✦ J.theory A (2012) 48:113 Page 11 of 39 10Nuclear2 Data Application Cross section (barn) 10Community Community ✦ natural needs data: compilationLu(n,γ) @ DANCE 1 ENDF/B−VII.0 SAMMY7.0 broadened and fitted 10−1 1 10 102 ✦ ✦ evaluation Neutron energy (eV) complete Fig. 15. Cross-section for the 175Lu(n, γ) reaction measured with a natural Lutetium sample in the resolved resonance ✦ organized ✦range.archival 176Lu(n,γ) @ DANCE ✦ 104 ENDF/B−VII.0 SAMMY7 broadened and fitted traceable DANCE detector ✦ dissemination 103 ✦ readable LANSCE Cross section (barn) 102 Fig. 14. The DANCE detector (picture credits: LANSCE-NSM. Herman Berkeley, May 27-19, 2015 LA-UR-0802953). 10 1 processed into physical quantities, like the total γ cascade 10−1 1 10 102 energy, γ multiplicity, individual gamma ray energies, and Neutron energy (eV) neutron time of flight. After analysis of these data and sev- 176 eral corrections (calibration, dead time correction, back- Fig. 16. Cross-section for the Lu(n, γ)reactioninthere- solved resonance range. ground subtraction) the neutron radiative capture cross- section σ(n,γ)(En) is obtained. Results are presented here 176 2 Lu(n,γ) @ DANCE for three energy ranges: i) thermal energy, ii) resolved res- 10 onance region, and iii) above 1 keV in the unresolved res- ENDF/B−VII.0 onance region. K. Wisshak et al, 2006 H. Beer et al, 1984 i) For an incident neutron energy of 0.025 eV, the mea- BRC sured cross-sections for 175Lu(n, γ)and176Lu(n, γ), are in Cross section (barn) good agreement with published values [64] while improv- 10 ing their precisions.