Discovery of the Selenium Isotopes
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Atmospheric Source Terms for the Idaho Chemical Processing Plant, 1957 – 1959
FINAL ATMOSPHERIC SOURCE TERMS FOR THE IDAHO CHEMICAL PROCESSING PLANT, 1957–1959 Contract No. 200-2002-00367 Task Order No. 1, Subtask 1 A final report to the Centers for Disease Control and Prevention Atlanta, Georgia 30335 SC&A, Inc. 6858 Old Dominion Drive, Suite 301 McLean, Virginia 22101 SENES Oak Ridge, Inc. 102 Donner Drive Oak Ridge, Tennessee 37830 Authors: Robert P. Wichner, SENES Oak Ridge, Inc. John-Paul Renier, SENES Oak Ridge, Inc. A. Iulian Apostoaei, SENES Oak Ridge, Inc. July 2005 ICPP Source Terms July 2005 TABLE OF CONTENTS EXECUTIVE SUMMARY .......................................................................................................ES-1 1.0 SCOPE AND APPROACH ............................................................................................. 1-1 1.1 Scope .................................................................................................................. 1-1 1.2 Approach.............................................................................................................. 1-1 1.2.1 Operational RaLa Releases ...................................................................... 1-1 1.2.2 Idaho Chemical Processing Plant Criticality Approach........................... 1-2 2.0 THE RADIOACTIVE LANTHANUM (RaLa) PROCESS ............................................ 2-1 2.1 Background .......................................................................................................... 2-1 2.1.1 Requirement ............................................................................................ -
A 1 Case-PR/ }*Rciofft.;Is Report
.A 1 case-PR/ }*rciofft.;is Report (a) This eruption site on Mauna Loa Volcano was the main source of the voluminous lavas that flowed two- thirds of the distance to the town of Hilo (20 km). In the interior of the lava fountains, the white-orange color indicates maximum temperatures of about 1120°C; deeper orange in both the fountains and flows reflects decreasing temperatures (<1100°C) at edges and the surface. (b) High winds swept the exposed ridges, and the filter cannister was changed in the shelter of a p^hoehoc (lava) ridge to protect the sample from gas contamination. (c) Because of the high temperatures and acid gases, special clothing and equipment was necessary to protect the eyes. nose, lungs, and skin. Safety features included military flight suits of nonflammable fabric, fuil-face respirators that are equipped with dual acidic gas filters (purple attachments), hard hats, heavy, thick-soled boots, and protective gloves. We used portable radios to keep in touch with the Hawaii Volcano Observatory, where the area's seismic activity was monitored continuously. (d) Spatter activity in the Pu'u O Vent during the January 1984 eruption of Kilauea Volcano. Magma visible in the circular conduit oscillated in a piston-like fashion; spatter was ejected to heights of 1 to 10 m. During this activity, we sampled gases continuously for 5 hours at the west edge. Cover photo: This aerial view of Kilauea Volcano was taken in April 1984 during overflights to collect gas samples from the plume. The bluish portion of the gas plume contained a far higher density of fine-grained scoria (ash). -
Cross Section Data for the Production of the Positron Emitting Niobium Isotope 90Nb Via the 90Zr(P, N)-Reaction
Radiochim. Acta 90, 1–5 (2002) by Oldenbourg Wissenschaftsverlag, München Cross section data for the production of the positron emitting niobium isotope 90Nb via the 90Zr(p, n)-reaction By S. Busse1,2,F.Rösch1,∗ andS.M.Qaim2 1 Institut für Kernchemie, Johannes Gutenberg-Universität, D-55128 Mainz, Germany 2 Institut für Nuklearchemie, Forschungszentrum Jülich GmbH, D-52425 Jülich, Germany (Received April 19, 2001; accepted in revised form July 16, 2001) Positron emitter 90Nb / Nuclear reaction / (α, 3n)-reactions on natural yttrium. A medium-sized cy- Excitation function / Calculated integral yield / clotron would allow the production of 90Nb via the (p, n)-, Experimental thick target yield / Radionuclidic impurities (d, 2n)- or the (3He, 2n)-process. In fact even a small-sized cyclotron (Ep ≤ 16 MeV) should lead to sufficient quanti- ties of the radioisotope via the (p, n)-reaction. A few stud- Summary. The radioisotope 90Nb decays with a positron ies have shown that the (d, 2n)-reaction requires a deuteron + branching of 53% and a relatively low β -energy of energy of about 16 MeV [5–7], the (3He, 2n)-process a 3He- = . = . Emean 0 66 MeV and Emax 1 5 MeV. Its half-life of 14 6h energy of ≥ 30 MeV and the (α, 3n)-reaction an α-particle makes it especially promising for quantitative investigation energy of ≥ 45 MeV [8]. Furthermore, the systematics of of biological processes with slow distribution kinetics using (3He, 2n)- and (p, n)-reactions suggest that the production positron emission tomography. To optimise its production, 90 the excitation functions of 90Zr(p, xn)-processes were studied yield of Nb should be higher in the latter process. -
Calculations of \(N,2N\) Reaction Cross Sections for 74,76,78,80,82Se up to 20
128 EPJ Web of Conferences , 01001 (2016) DOI: 10.1051/epjconf/201612801001 TESNAT 2016 Halide Şahan1,a, Muhittin Şahan1, Eyyup Tel1 1Osmaniye Korkut Ata University, Faculty of Arts and Science, Department of Physics, Osmaniye, Turkey In the present work, the excitation functions of (n,2n) reactions for five isotopes of selenium (74,76,78,80,82Se) are calculated using ALICE/ASH, EMPIRE-3.2.2, PCROSS, and TALYS 1.6 computer codes based on statistical model up to 20 MeV. The theoretical calculations provide information of the (n,2n) excitation functions with the increasing target neutron number of selenium element. The calculated cross-sections were compared with experimental data from EXFOR and also with the cross- sections estimated with semi empirical formula developed by Tet et al. (2008) [18]. Results show a reasonably good agreement between the calculations and the experimental data from literature. ! " by Tel et al. [13]. These formulas have been given as follows; The theoretical calculation models are necessary to ⎪⎧7.15[]1− 2.45e−31.620(N −Z ) / A for even A⎪⎫ provide the estimation of the particle–induced reaction σ = (1) ln n,2n ⎨ ⎬ cross sections due to the experimental difficulty [1,2]. In ⎩⎪ 7.65[]1−1.59e−23.06(N −Z ) / A for odd A⎭⎪ past years the cross section of selenium isotopes (74,76,78,80,82,84Se) around 14-15 MeV have been measured For (n,2n) reaction cross sections of 74Se(n,2n)73Se, by many researches such as Hille and Münzer [3]; 76Se(n,2n)75Se, 78Se(n,2n)77Se, 80Se(n,2n)79Se and Minetti and Pasquarelli [4]; Casanova and Sanchez [5]; 82Se(n,2n)81Se at 14-15 MeV, the calculated cross 74,76,78,80,82 Hoang et al. -
AN43285 – Accurate Determination of Arsenic and Selenium in Environmental Samples Using Triple Quadrupole ICP-MS
Certified for Thermo Scientific™ iCAP™ TQe ICP-MS APPLICATION NOTE 43285 Accurate determination of arsenic and selenium in environmental samples using triple quadrupole ICP-MS Authors: Marcus Manecki1, Simon Lofthouse2, Philipp Boening3 and Shona McSheehy Ducos1; 1Thermo Fisher Scientific, Bremen, Germany; 2Thermo Fisher Scientific, Hemel Hempstead, UK; 3Institute of Chemistry and Biology of the Marine Environment (ICBM), Carl von Ossietzky University of Oldenburg, Oldenburg, Germany Keywords: Arsenic, interference removal, Selenium for example is an essential element that is REE, rock, selenium, soil, sediment necessary for normal thyroid function and due to its antioxidant properties, is associated with several health Goal benefits. Diseases associated with selenium deficiency To demonstrate the accurate determination of arsenic such as Keshan disease and symptoms of hypothyroidism, and selenium in sediments and rocks that contain elevated are most commonly found in areas where levels of levels of rare earth elements using triple quadrupole selenium in soil are particularly low. Supplementation as a ICP-MS. remedy is common practice and is not isolated to humans. Understanding where soil selenium deficiencies occur for Introduction example supports the correct supplementation of cattle Due to the impact arsenic and selenium can have in the grazing in those areas to prevent white muscle disease environment at low levels, as a toxin or essential nutrient (a cattle specific selenium deficiency disease). respectively, it is important to be able to quantify them accurately. Arsenic on the other hand, in its inorganic forms Instrumentation (the most common forms found in ground water and soils) An iCAP TQ ICP-MS was used to analyse all samples. -
Determining Atomic Mass Practice with Answers
Determining Atomic Mass Practice with Answers Atomic Mass • Refers to the mass of an atom. • Number of protons and neutrons • Atoms are too small to mass so mass is determined by the relative mass of a standard atom. By international agreement (IUPAC), Carbon12 is the chosen standard atom because of its abundance here on Earth. Atomic Mass Unit defined is a mass exactly equal to 1/12th of one carbon12 atom. 1 carbon12 atom = 12 amu Determining Atomic Mass Practice with Answers Determine Atomic Mass Unit for Hydrogen Hydrogen 1 as 1 proton and 0 neutrons 1/12 = .0833 x 100 = 8.33% So hydrogen is 8.33% of one atom of Carbon12 Atomic Mass of Hydrogen = mass of 1 atom of Carbon 12 x 8.33% = 12 x .0833 =.9996 = 1.0 amu Through different methods of experimental testing, chemists have more accurately determined the mass of hydrogen to be 1.008, which is more like 8.40%. Determining Atomic Mass Practice with Answers Determining Average Atomic Mass: Because element's usually have more than one isotope, which means their masses are different an average must be determine to reflect the mass of all an atom's isotopes. Example: A sample of cesium is 75% Cs-133, 20% Cs-132, and 5% Cs-134. What is the average atomic mass? ANSWER: .75 x 133 = 99.75 .20 x 132 = 26.4 .05 x 134 = 6.7 Total = 132.85 amu average atomic mass unit Determining Atomic Mass Practice with Answers Isotopes and Average Atomic Mass Iodine: 80% 127 I 17% 126 I 3% 128 I ANSWER: .80 x 127 = 101.6 .17 x 126 = 21.42 .03 x 128 = 3.84 Total = 126.86 amu Determining Atomic Mass Practice with Answers Determining Atomic Mass Practice with Answers Determining Atomic Mass Practice with Answers Determining Atomic Mass Practice with Answers Determining Atomic Mass Practice with Answers Determining Atomic Mass Practice with Answers Determining Atomic Mass Practice with Answers Determining Atomic Mass Practice with Answers Determining Atomic Mass Practice with Answers Determining Atomic Mass Practice with Answers Bromine which exists as a dark, red gas is Br2. -
Hyperfine Structure in Selenium, Palladium and Gold.* by L
HYPERFINE STRUCTURE IN SELENIUM, PALLADIUM AND GOLD.* BY L. SIBAZ~A. (From the Dcpa,'tment of Physics, CeJ~tral College, Balzgarore.) Received September 10, 1935. Selenium (At. no. 34; At. wt. 79.2). l'oI~ purposes of classification of selenium spectra, the arc arid spark lines of seleniunl have been mostly excited in tubes of various types with con- (lensed or uncondensed electrical discharge through selenium vapour or between alumiuium poles tipped with metallic selenium. A selenium arc either in vacuum or iu an atmosphere of nitrogen has aIso been employed. Such sources however are not suited for hyperfine structure work, as the lines obtained are broad and diffuse. Moreover most of the prominent are lines of selenium lie either in the near infra-red or in the extreme ultra-violet, thus rendering their analysis by high resolving power apparatus specially difficult. Some intense spark lines of selenium 1% in the visible region; lmt under the conditions employed for their emission in discharge tubes, the broadening of the lines renders such sources unsuitable for hyperfine structure study. The apparatus used, the essential part of ~-hich is a water- cooled hollow cathode, is the same as that employed by 2Prof. Venkatesaehar and the author in their investigation on the isotopic constitution of platinum, x The selenium powcler took the place of the platinum foil in the tubular space of the cathode (P1. XV, Fig. 1). For experimental details the above paper -,,~+ he consulted. Of the seventeen lines of selenium here examined, only two are are lines and the remaining fifteen belong to the first spark spectrum of selenium. -
Isotopes of M&M-Ium
Name _________________________________________________________________ Hour __________________ Isotopes of m&m-ium Elements commonly exist with differing numbers of neutrons. We call these elements isotopes and an example is Bromine-79 and Bromine-81. These isotopes are naturally occurring…but do not exist equally in nature. Br-79 is more common and occurs 55% of the time while Br-81 occurs 45% of the time. To calculate the average atomic mass (the weighted average of the masses of its isotopes) of bromine you need to take into account the relative abundance of each element. The average atomic mass = (% abundance of isotope 1)x(mass of isotope 1) + (% abundance of isotope 2)x(mass of isotope 2) (% should be expressed in decimals) Pre-Lab Questions: 1. Calculate the average atomic mass of Bromine using the % abundances above: 2. Carbon has 2 stable isotopes: C-12 with a natural abundance of 98.89% and C-14 at 1.11%. Calculate the average atomic mass of Carbon. m&mium, a recently discovered element from the chocolate mountains of Wonkaland, exits as two isotopes. m&mium has many different colors and your job is to find the average atomic mass of one color of m&mium. Safety Precautions: Never eat anything that has touched lab equipment! Use a baking cup so your group can eat the m&ms when you are done! Procedure: Show all work for all calculations. 1. Record the number of small m&m’s and large m&m’s you have (your color only) in the table. 2. Record the total number of m&m’s you have. -
Discovery of the Bromium Isotopes
Discovery of the Bromium Isotopes J. Kathawa, J. Claes, M. Thoennessen∗ National Superconducting Cyclotron Laboratory and Department of Physics and Astronomy, Michigan State University, East Lansing, MI 48824, USA Abstract Twenty-eight bromium isotopes have so far been observed; the discovery of these isotopes is discussed. For each isotope a brief summary of the first refereed publication, including the production and identification method, is presented. ∗Corresponding author. Email address: [email protected] (M. Thoennessen) Preprint submitted to Atomic Data and Nuclear Data Tables April 28, 2010 Contents 1. Introduction . 2 2. Discovery of 70−97Br ................................................................................... 3 2.1. 70Br............................................................................................. 3 2.2. 71Br............................................................................................. 3 2.3. 72Br............................................................................................. 5 2.4. 73Br............................................................................................. 5 2.5. 74Br............................................................................................. 5 2.6. 75Br............................................................................................. 5 2.7. 76Br............................................................................................. 6 2.8. 77Br............................................................................................ -
Detection of Elements at All Three R-Process Peaks in the Metal-Poor Star HD 160617
Published in the Astrophysical Journal A Preprint typeset using LTEX style emulateapj v. 5/2/11 DETECTION OF ELEMENTS AT ALL THREE R-PROCESS PEAKS IN THE METAL-POOR STAR HD 1606171 ,2 ,3 Ian U. Roederer4 and James E. Lawler5 Published in the Astrophysical Journal ABSTRACT We report the first detection of elements at all three r-process peaks in the metal-poor halo star HD 160617. These elements include arsenic and selenium, which have not been detected previously in halo stars, and the elements tellurium, osmium, iridium, and platinum, which have been detected previously. Absorption lines of these elements are found in archive observations made with the Space Telescope Imaging Spectrograph onboard the Hubble Space Telescope. We present up-to-date absolute atomic transition probabilities and complete line component patterns for these elements. Additional archival spectra of this star from several ground-based instruments allow us to derive abundances or upper limits of 45 elements in HD 160617, including 27 elements produced by neutron-capture reactions. The average abundances of the elements at the three r-process peaks are similar to the predicted solar system r-process residuals when scaled to the abundances in the rare earth element domain. This result for arsenic and selenium may be surprising in light of predictions that the production of the lightest r-process elements generally should be decoupled from the heavier r-process elements. Subject headings: atomic data — nuclear reactions, nucleosynthesis, abundances — stars: abundances — stars: individual (HD 160617) — stars: Population II 1. INTRODUCTION in greater abundance during n-capture reactions. The Understanding the origin of the elements is one of the s-process path closely follows the valley of β-stability, major challenges of modern astrophysics. -
Proceedings of the 1990 Billings Land Reclamation Symposium On
U.S. GEOLOGICAL SURVEY CI-RCULAR 1064 Proceedings of the 1990 Billings Land Reclamation Symposium on Selenium in Arid and Semiarid Environments, Western United States AVAILABILITY OF BOOKS AND MAP OF THE U.S. GEOLOGICAL SURVEY Instructions on ordering publications of the U.S. Geological Survey, along with prices of the Jast offerings, arc·Jive!l in the cur rent-year issues of the monthly catalog "New Publications of th U.S. Geological Survey." Prices of available U.l:~ Sur· . vey publications released prior to the current year are listed in e most recent annual "Price and Availability List" Puhlications that are listed in various U.S. Geological Survey catalogs (see b ck inside cover) but not listed in the most recent annual "Price and Availability List" are no longer available. Prices of reports released to the open files are ~iven in the li ting "U.S. Geological Survey Open-File Reports,'~ updated month ly, which is for sale in microfiche froiD the U.S. Geological S ey, Books and Open-File Reports Section, Federal Center, Box 25425, Denver, CO 80225. Reports released through the NTIS y be obtained by writing to the National Technical Information Service, U.S. Department of Commerce, Springfield, VA 22161 please include NTIS report numbez with inquiry. Order U.S. Geological Survey publications by mail or over the counter from the offices given below. BY MAIL OVER THE COUNTER Books Books Professional Papers, Bulletins, Water-Supply Papers, Techniqu of Water-Resources Investigations, Circulars, publications of general in Books of the -
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Anomalies in the Fermi Effect • ... be conbi~e~,.CL bjvsome as equally probable, or even more ~:Sa"b ~ s tfi:aR the fixst=aite"!'f'l'autive •. While we "ffhal.l ~ 4 ~ a.~.a,.fyf---c __.,. emphasize the pas si bili ty o 4his eeeond vie'fvj~we will · t.A----~ . (J ¢::6 d.t"ia: -; ~~.... ~. ,,-..A( ~ not discuss £? in ~ etail as the .:j:j rEf~ ax; ¥10 't:"-t dfGtJ..tL ~ ,..u~ [.!lt·v ...... ~YJ ~- ~. r/ ~ This unequal treatment is not due to a biased opinion in . ~,.,,,~ . ~ !-'. ' 'M·•/. favour of one of e ·· ' views, and seems -t;o-..b€ just'fied (/~A rt• f.-# £r.~- .-/ ~ e.e i.o I~,_,_ "-!- H . .t:/ ,d"~ t~t .vrlk t.~ 1 ~-.. a : . , . - · by t h e fact that the f1Fst VJ:ew- leads \ to a number of p otentially pas si ble ~l r ( • (-(;;-- -~~ "1:1 /experiments wnich may decide / 3:-rr~~~ , ·o-: a ~ n. ~ , I~ - "/Z,_ - /t , .y /I(, " ,. /.. ' . .... I /7<Vt.. (,_.1' ~~ whereas it se5!ms to be diffipul t to think of cn ~. t'- ,.. (, ...... 1 #t.r t~- ....-.~..., "'<../ t<t.,.-< ""'"' t t( /'l'n J ( "t·C experiments,. ~t'O a:mc t · decision o·n-~ a - - - "' ANOMALIB.S IN TilE FERMI EFFECT 1) Amaldi, D'Agostino and Segre have found that neutrons Which have been slowed down by paraffin wax induce in indium two radio active half-life periods (16 eea. and 54 min.). T.A. Cha~ers and 2) I have subsequently reported that indium can also be comparatively strongly activated with a third period of several hours if irradiated by neutrons from a radon alpha-particle beryllium source in the ab- sence of hydrogen-containing substances, and we raised the question whether its existence can be satisfactorily explained without a new assumption.