Concurrent Reduction and Distillation; an Improved Technique for the Recovery and Chemical Refinement of the Isotopes of Cadmium and Zinc*
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How Earth Got Its Moon Article
FEATURE How Earth Got its MOON Standard formation tale may need a rewrite By Thomas Sumner he moon’s origin story does not add up. Most “Multiple impacts just make more sense,” says planetary scientists think that the moon formed in the earli- scientist Raluca Rufu of the Weizmann Institute of Science in est days of the solar system, around 4.5 billion years Rehovot, Israel. “You don’t need this one special impactor to Tago, when a Mars-sized protoplanet called Theia form the moon.” whacked into the young Earth. The collision sent But Theia shouldn’t be left on the cutting room floor just debris from both worlds hurling into orbit, where the rubble yet. Earth and Theia were built largely from the same kind of eventually mingled and combined to form the moon. material, new research suggests, and so had similar composi- If that happened, scientists expect that Theia’s contribution tions. There is no sign of “other” material on the moon, this would give the moon a different composition from Earth’s. perspective holds, because nothing about Theia was different. Yet studies of lunar rocks show that Earth and its moon are “I’m absolutely on the fence between these two opposing compositionally identical. That fact throws a wrench into the ideas,” says UCLA cosmochemist Edward Young. Determining planet-on-planet impact narrative. which story is correct is going to take more research. But the Researchers have been exploring other scenarios. Maybe answer will offer profound insights into the evolution of the the Theia impact never happened (there’s no direct evidence early solar system, Young says. -
Optimization Studies of the CERN-ISOLDE Neutron Converter and Fission Target System
Optimization Studies of the CERN-ISOLDE neutron converter and fission target system Raul Luís1, José G. Marques, Thierry Stora, Pedro Vaz, Luca Zanini 1ITN – Estrada Nacional 10, 2686-953, Sacavém, Portugal 2CERN – CH-1211, Genève 23, Switzerland 3PSI – 5232 Villigen, Switzerland E-mail: [email protected] Abstract. The ISOLDE facility at CERN has been one of the leading isotope separator on-line (ISOL) facilities worldwide since it became operative in 1967. More than 1000 isotopes are available at ISOLDE, produced after the bombardment of various primary targets with a pulsed proton beam of energy 1.4 GeV and an average intensity of 2 μA. A tungsten solid neutron converter has been used for ten years to produce neutron-rich fission fragments in UCx targets. In this work, the Monte Carlo code FLUKA and the cross section codes TALYS and ABRABLA were used to study the current layout of the neutron converter and fission target system of the ISOLDE facility. An optimized target system layout is proposed, which maximizes the production of neutron-rich isotopes and reduces the contamination by undesired proton-rich isobars. The studies here reported can already be applied to ISOLDE and will be of special relevance for the future facilities HIE-ISOLDE and EURISOL. 1. Introduction One of the most efficient ways to study nuclei far from stability is the Isotope Separation On-Line (ISOL) method, in which a beam of high-energy hadrons hits a thick target, producing a great variety of radioactive products through different processes like fission, spallation and fragmentation [1]. The resulting nuclides can be studied after they are extracted from the target, ionized and mass separated. -
KULAGE-DISSERTATION-2013.Pdf
ENCRYPTED NANOPARTICLES FOR SECURITY, COUNTER-INDUSTRIAL ESPIONAGE, AND COUNTERFEITING A Dissertation by ZACHARY ANDREW KULAGE Submitted to the Office of Graduate and Professional Studies of Texas A&M University in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY Chair of Committee, William S. Charlton Committee Members, Sean M. McDeavitt John W. Poston, Sr. Charles M. Folden III Head of Department, Yassin A. Hassan December 2013 Major Subject: Nuclear Engineering Copyright 2013 Zachary Andrew Kulage ABSTRACT Acts of terrorism and the use of explosives raise concerns about what can be done to prevent such acts. From stopping such a threat to preventing the illicit counterfeiting and smuggling of sensitive and proprietary goods, identification tag- gant technology can be applied to identify and interdict materials of a dubious na- ture. This cost effective approach to tag and track materials will find application in both the government and private sectors, particularly in the prevention of corporate espionage. A taggant system was created based on the modification of the natural isotopic vector of cadmium and tellurium to create artificial, unique, and robust identification capabilities. A proof of concept trial was undertaken to ascertain the effectiveness, reliability, and integrity of a system. Stable isotopes were mixed in various combi- nations to alter the isotopic vector and then neutron activation analysis techniques were used to evaluate the quality of the taggants. Two different neutron activation analysis facilities of differing capabilities were employed to test the limitations of the method in detection of trace amounts of taggant material. Testing of the taggant system found that solid phase taggants were capable of producing around 14,000 unique taggants for under $250 each while liquid phase taggants were capable of producing around 2,000 unique taggants for under $50 each. -
Neutron Capture Cross Sections of Cadmium Isotopes
Neutron Capture Cross Sections of Cadmium Isotopes By Allison Gicking A thesis submitted to Oregon State University In partial fulfillment of the requirements for the degree of Bachelor of Science Presented June 8, 2011 Commencement June 17, 2012 Abstract The neutron capture cross sections of 106Cd, 108Cd, 110Cd, 112Cd, 114Cd and 116Cd were determined in the present project. Four different OSU TRIGA reactor facilities were used to produce redundancy in the results and to measure the thermal cross section and resonance integral separately. When the present values were compared with previously measured values, the differences were mostly due to the kind of detector used or whether or not the samples were natural cadmium. Some of the isotopes did not have any previously measured values, and in that case, new information about the cross sections of those cadmium isotopes has been provided. Table of Contents I. Introduction………………………………………………………………….…….…1 II. Theory………………………………………………………………………...…...…3 1. Neutron Capture…………………………………………………….….……3 2. Resonance Integral vs. Effective Thermal Cross Section…………...………5 3. Derivation of the Activity Equations…………………………………....…..8 III. Methods………………………………………………………….................…...…...12 1. Irradiation of the Samples………………………………………….….....…12 2. Sample Preparation and Parameters………………..………...………..……16 3. Efficiency Calibration of Detectors…………………………..………....…..18 4. Data Analysis…………………………………...…….………………...…..19 5. Absorption by 113Cd……………………………………...……...….………20 IV. Results………………………………………………….……………..……….…….22 -
Arxiv:1305.1738V1 [Nucl-Ex] 8 May 2013 Ae Pcrsoystpa SLECR.High-Energy ISOLDE-CERN
Spins, Electromagnetic Moments, and Isomers of 107-129Cd D. T. Yordanov,1,2, ∗ D. L. Balabanski,3 J. Biero´n,4 M. L. Bissell,5 K. Blaum,1 I. Budinˇcevi´c,5 S. Fritzsche,6 N. Fr¨ommgen,7 G. Georgiev,8 Ch. Geppert,6, 7 M. Hammen,7 M. Kowalska,2 K. Kreim,1 A. Krieger,7 R. Neugart,7 W. N¨ortersh¨auser,6, 7 J. Papuga,5 and S. Schmidt6 1Max-Planck-Institut f¨ur Kernphysik, Saupfercheckweg 1, D-69117 Heidelberg, Germany 2CERN European Organization for Nuclear Research, Physics Department, CH-1211 Geneva 23, Switzerland 3INRNE, Bulgarian Academy of Science, BG-1784 Sofia, Bulgaria 4Instytut Fizyki imienia Mariana Smoluchowskiego, Uniwersytet Jagiello´nski, Reymonta 4, 30-059 Krak´ow, Poland 5Instituut voor Kern- en Stralingsfysica, KU Leuven, Celestijnenlaan 200D, B-3001 Leuven, Belgium 6GSI Helmholtzzentrum f¨ur Schwerionenforschung GmbH, D-64291 Darmstadt, Germany 7Institut f¨ur Kernchemie, Johannes Gutenberg-Universit¨at Mainz, D-55128 Mainz, Germany 8CSNSM-IN2P3-CNRS, Universit´ede Paris Sud, F-91405 Orsay, France (Dated: October 7, 2018) The neutron-rich isotopes of cadmium up to the N = 82 shell closure have been investigated by high-resolution laser spectroscopy. Deep-UV excitation at 214.5 nm and radioactive-beam bunching provided the required experimental sensitivity. Long-lived isomers are observed in 127Cd and 129Cd for the first time. One essential feature of the spherical shell model is unambiguously confirmed by − a linear increase of the 11/2 quadrupole moments. Remarkably, this mechanism is found to act well beyond the h11/2 shell. PACS numbers: 21.10.Ky, 21.60.Cs, 32.10.Fn, 31.15.aj When first proposed the nuclear shell model was protons impinging on a tungsten rod produced low- to largely justified on the basis of magnetic-dipole proper- medium-energy neutrons inducing fission in a uranium ties of nuclei [1]. -
I, Bichard Lewis Woodward, Was Horn in Kansas City
AUTOBIOGRAPHT I, Bichard Lewis Woodward, was horn in Kansas City, Missouri, December 11, 1913 - My elementary and secondary school education was in the public schools of Kansas City and St . Louis, Missouri. In June, 1935. I received the degree Bachelor of Science in Civil Engineering from Washington University. I received the degree Master of Science from Harvard University in June, 1948. Since 1937 I have been an officer of tie United States Public Health Service . Under the auspices of this organisation, I have studied in the Department of Physics at the Ohio State University since June, 1949- - 42 - ACKNOWLEDGMENTS I wish to acknowledge the assistance of my adviser Prof M. L. Pool, of my coworker Mr. S . C. Fultz, of our chemist Mr. James McGlotten, and of Mr. Claude McWhlrt and other members of the staff of the Physics Department shops. - hi - BLBLIOGEAPHT 1. J. H. Buck, Fhys. Rev., 59, 1025 (1938) 2. A. Mukerji. P. Preiswerk, Felv . Phys. Acta, 23, 516 (1950) 3* G • T. Seahorg, I. Perlman, Rev. Mod. Phys., 20, 585 (1998) 9-. G. E. Valley, R. 1. McCreary, Phys. Rev., 5 6, 863 (1939) 5 . S. Sag&ne, S . Kojina, G. Miyamoto, Fhys. Math. Soc . Japan, Proc., 21, 728 (1939) 6 . E. C. Barker, Plutonium Proj . Report Mon. P-269, 8 (199-7) 7. S . E. Haynes, Phys. Rev., 79, 9-23 (1998) 8 . I*. M. Langer, R. D. Moffat, Ihys . Rev., 80, 6 51 (1950) 9. A. C. Helmholz, Phys. Rev., 60, 9-15 (1991) 10. J. M. Cork, L. N. Hadley, Jr., C. V. -
Atomic Weights of the Elements 2013 (IUPAC Technical Report)
Pure Appl. Chem. 2016; 88(3): 265–291 IUPAC Technical Report Juris Meija*, Tyler B. Coplen, Michael Berglund, Willi A. Brand, Paul De Bièvre, Manfred Gröning, Norman E. Holden, Johanna Irrgeher, Robert D. Loss, Thomas Walczyk and Thomas Prohaska Atomic weights of the elements 2013 (IUPAC Technical Report) DOI 10.1515/pac-2015-0305 Received March 26, 2015; accepted December 8, 2015 Abstract: The biennial review of atomic-weight determinations and other cognate data has resulted in changes for the standard atomic weights of 19 elements. The standard atomic weights of four elements have been revised based on recent determinations of isotopic abundances in natural terrestrial materials: cadmium to 112.414(4) from 112.411(8), molybdenum to 95.95(1) from 95.96(2), selenium to 78.971(8) from 78.96(3), and thorium to 232.0377(4) from 232.038 06(2). The Commission on Isotopic Abundances and Atomic Weights (ciaaw.org) also revised the standard atomic weights of fifteen elements based on the 2012 Atomic Mass Evaluation: aluminium (aluminum) to 26.981 5385(7) from 26.981 5386(8), arsenic to 74.921 595(6) from 74.921 60(2), beryllium to 9.012 1831(5) from 9.012 182(3), caesium (cesium) to 132.905 451 96(6) from 132.905 4519(2), cobalt to 58.933 194(4) from 58.933 195(5), fluorine to 18.998 403 163(6) from 18.998 4032(5), gold to 196.966 569(5) from 196.966 569(4), holmium to 164.930 33(2) from 164.930 32(2), manganese to 54.938 044(3) from 54.938 045(5), niobium to 92.906 37(2) from 92.906 38(2), phosphorus to 30.973 761 998(5) from 30.973 762(2), praseodymium to 140.907 66(2) from 140.907 65(2), Article note: Sponsoring body: IUPAC Inorganic Chemistry Division Committee: see more details on page 289. -
Precision Mass Measurements for Studies of Nucleosynthesis Via the Rapid Neutron-Capture Process
Dissertation submitted to the Combined Faculties for the Natural Sciences and for Mathematics of the Ruperto-Carola University of Heidelberg, Germany for the degree of Doctor of Natural Sciences Put forward by Diplomant: Dinko Atanasov Born in: Yambol, Bulgaria Oral examination: 06. July 2016 Precision mass measurements for studies of nucleosynthesis via the rapid neutron-capture process Penning-trap mass measurements of neutron-rich cadmium and caesium isotopes Prof. Dr. Klaus Blaum Referees: PD Dr. Adriana P´alffy Zusammenfasung Obwohl die Theorie ¨uber die schnelle Neutronenanlagerung (r-Prozess) schon vor mehr als 55 Jahren entwickelt wurde, wird ¨uber den exakten Ort im Universum an dem dieser Prozess stattfindet noch rege debattiert. Theoretische Studien sagen voraus, dass der Verlauf des r-Prozesses gepr¨agtwird durch ¨außerstneutronenreiche Materie mit sehr asymmetrischen Proton-zu-Neutron Verh¨altnissen.Die aktuellen Kenntnisse ¨uber Eigenschaften dieser neutro- nenreichen Isotope, die dazu geeignet sind als Eingangsdaten f¨urStudien ¨uber den r-Prozess herangezogen zu werden, sind nur unzureichend oder gar nicht vorhanden. Die grundlegen- den Eigenschaften der Kerne, wie Bindungsenergie, Halbwertszeiten und Reaktionsquerschnitt spielen eine wichtige Rolle in den theoretischen Simulationen und k¨onnendiese beeinflussen oder sogar zu drastisch alternativen Ergebnissen f¨uhren. Um diese Theorien mit gemesse- nen Daten zu untermauern und die Produktion neutronenreicher Isotope zu verbessern, wurde an Forschungseinrichtungen wie ISOLDE am CERN, ein g¨anzlich bemerkenswerter Aufwand betrieben. Das Ziel dieser Dissertation ist es die experimentelle Arbeit zu beschreiben, welche n¨otigwar, um die Pr¨azisionsmassenmessungender neutronenreichen Isotope Cadmium (129−131Cd) und C¨asium(132;146−148Cs) zu erm¨oglichen. Die Messungen wurden an der Iso- topenfabrik ISOLDE am CERN mithilfe des aus vier Ionenfallen bestehenden Massenspek- trometers ISOLTRAP durchgef¨uhrt. -
Beta Decay of Neutron-Rich Isotopes of Zinc and Gallium
University of Tennessee, Knoxville TRACE: Tennessee Research and Creative Exchange Doctoral Dissertations Graduate School 5-2015 Beta decay of neutron-rich isotopes of zinc and gallium Mohammad Faleh M. Al-Shudifat University of Tennessee - Knoxville, [email protected] Follow this and additional works at: https://trace.tennessee.edu/utk_graddiss Part of the Nuclear Commons Recommended Citation Al-Shudifat, Mohammad Faleh M., "Beta decay of neutron-rich isotopes of zinc and gallium. " PhD diss., University of Tennessee, 2015. https://trace.tennessee.edu/utk_graddiss/3288 This Dissertation is brought to you for free and open access by the Graduate School at TRACE: Tennessee Research and Creative Exchange. It has been accepted for inclusion in Doctoral Dissertations by an authorized administrator of TRACE: Tennessee Research and Creative Exchange. For more information, please contact [email protected]. To the Graduate Council: I am submitting herewith a dissertation written by Mohammad Faleh M. Al-Shudifat entitled "Beta decay of neutron-rich isotopes of zinc and gallium." I have examined the final electronic copy of this dissertation for form and content and recommend that it be accepted in partial fulfillment of the equirr ements for the degree of Doctor of Philosophy, with a major in Physics. Robert Grzywacz, Major Professor We have read this dissertation and recommend its acceptance: Soren Sorensen, Thomas Papenbrock, Jason P. Hayward Accepted for the Council: Carolyn R. Hodges Vice Provost and Dean of the Graduate School (Original signatures are on file with official studentecor r ds.) Beta decay of neutron-rich isotopes of zinc and gallium A Dissertation Presented for the Doctor of Philosophy Degree The University of Tennessee, Knoxville Mohammad Faleh M. -
Evolution of Nuclear Structure in Neutron-Rich Odd-Zn Isotopes and Isomers ∗ C
Physics Letters B 771 (2017) 385–391 Contents lists available at ScienceDirect Physics Letters B www.elsevier.com/locate/physletb Evolution of nuclear structure in neutron-rich odd-Zn isotopes and isomers ∗ C. Wraith a, X.F. Yang b, , L. Xie c, C. Babcock a, J. Bieron´ d, J. Billowes c, M.L. Bissell b,c, K. Blaum e, B. Cheal a, L. Filippin f, R.F. Garcia Ruiz b,c, W. Gins b, L.K. Grob g, G. Gaigalas h, M. Godefroid f, C. Gorges i, H. Heylen b, M. Honma j, P. Jönsson k, S. Kaufmann g, M. Kowalska l, J. Krämer i, S. Malbrunot-Ettenauer l, R. Neugart e,g, G. Neyens b, W. Nörtershäuser g,i, F. Nowacki m, T. Otsuka n, J. Papuga b, R. Sánchez o, Y. Tsunoda p, D.T. Yordanov q a Oliver Lodge Laboratory, Oxford Street, University of Liverpool, Liverpool, L69 7ZE, United Kingdom b KU Leuven, Instituut voor Kern- en Stralingsfysica, B-3001 Leuven, Belgium c School of Physics and Astronomy, The University of Manchester, Manchester, M13 9PL, United Kingdom d Instytut Fizyki imienia Mariana Smoluchowskiego, Uniwersytet Jagiello´nski, ul. prof. Stanisława Łojasiewicza 11, Kraków, Poland e Max-Plank-Institut für Kernphysik, D-69117 Heidelberg, Germany f Chimie Quantique et Photophysique, Université Libre de Bruxelles, B-1050 Brussels, Belgium g Institut für Kernchemie, Universität Mainz, D-55128 Mainz, Germany h Institute of Theoretical Physics and Astronomy, Vilnius University, Sauletekio˙ av. 3, LT-10222 Vilnius, Lithuania i Institut für Kernphysik, TU Darmstadt, D-64289 Darmstadt, Germany j Center for Mathematical Sciences, University of Aizu, Tsuruga, -
Stable Isotope Separation in Calutrons
Printed ill tho llnitzd Statss ot 4mcm 4vailsble frurii Nations' Technical Information Service U S :3ep?rtmelli uf Commerce 5285 Port 4oyal Cosd Spririizflald Viryinis 22161 NTlS ptwiodes P~III~~Copy ,498, Microfiche P,C1 I his rcpoti \*!is prspxed as an account of >,dSi-k sponsored by a3 agsncy of the United Sraies Governr;,ent. Neither thc !J nited Skiics i<n.~cti $IK~: nor any agency th2reof. no? any of thzir employoes, (ciakc?.Aijy ivarranty, express or irripiled, or assunias any legal liability or responsibility for ihe accuracy. compleienass, or usefulness of any inforriraiton. ;p ius, product, or process disclosed, or represents that its usewould not infr privately o-v?d ilghts Rcferencc herein to ai-y specific commercial product, process, or service by trade nziile, Zi'adei*lark, manufacturer, or otherwise, does not necsssarily constitute or imply its enduisemcat, recorn,n faVOiii-,g by ille United States(;ovc;riiiie!ii 01- any Zgency thereof Th opinions of auiihols cxp:essed here:!: d~ ~iui neccssarily statc or refisc?!host of the United Sta?ezGovernmer:?or any ngcncy therccf. ____ ___________... ..... .____ ORNL/TM-10356 OPERATIONS DIVISION STABLE ISOTOPE SEPARATION IN CALUTRONS: FORTY YEARS OF PRODUCTION AND DISTRIBUTION W. A. Bell J. G. Tracy Date Published: November 1987 Prepared by the OAK RIDGE NATIONAL LABORATORY Oak Ridge, Tennessee 37831 operated by MARTIN MARIETTA ENERGY SYSTEMS, INC. for the U.S. DEPARTMENT OF ENERGY under Contract No. DE-AC05-840R21400 iti CONTENTS Page ACKNOWLEDGMENTS ................................................. iv I. INTRODUCTION .............................................. 1 11. PROGRAM EVOLUTION ......................................... 1 111. RESEARCH AND DEVELOPMENT .................................. 5 IV. CHEMISTRY ................................................. 8 V. -
4.48 Cadmium
IUPAC 4.48 cadmium Stable Relative Mole isotope atomic mass fraction 106 Cd 105.906 460 0.012 45 108 Cd 107.904 183 0.008 88 110 Cd 109.903 007 0.124 70 111 Cd 110.904 183 0.127 95 112 Cd 111.902 763 0.241 09 113 † Cd 112.904 408 0.122 27 114 Cd 113.903 365 0.287 54 116 † Cd 115.904 763 0.075 12 † Radioactive isotope having a relatively long half-life and a characteristic terrestrial isotopic composition that contributes significantly and reproducibly to the determination of the standard atomic weight of the element in normal materials . Half-lives of 113 Cd and 116 Cd are 8.04 × 10 15 years and 3 × 10 19 years, respectively. P.O. 13757, Research Triangle Park, NC (919) 485-8700 IUPAC 4.48.1 Cadmium isotopes in biology Metal accumulation is a threat to our world’s water systems and wildlife. As a way to measure the influence of heavy metals on wildlife with mass spectrometric techniques, some researchers use animal food enriched in specific cadmium isotopes . These experiments work by exposing the animals to a diet enriched in 106 Cd and/or other stable isotopes of metals (for example, 65 Cu and/or 62 Ni) for a period of time. Depending on the purpose of the experiment, the residence time of the food in the gut is determined and isotopic compositions of the gut and/or feces are measured via inductively coupled plasma mass spectrometry (ICP-MS). This information is used to measure bio-uptake (absorption and incorporation of a substance by living tissue) and accumulation rates of metals in an exposed animal [352, 353].