Chapter 16 Nuclear Chemistry
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Laser Spectroscopy of Neutron Rich Bismuth Isotopes
CERN LIBRARIES, GENEVA new lllllllllllIllllllllllllllllllllllllllllllll SC00000267 CD [L] Q D K,Q/pm lO CERN/ISC 94-7 P60 scP GEM} »- emit 1=·1>.o1=·osAL TO THE rsotos COMMITTEE 9 Le-? Laser Spectroscopy of Neutron Rich Bismuth Isotopes CERN1 — Mainz? — Manchester3 — Stony Brook4 Collaboration J. Behr4, J. Billowes3, P. Campbell3, T.G. Cooperg, U. Georg2, I.S. Grant3, G. Gwinner4, G. Huber], M. Keimz, J. Kilgallon3, A. Kleinz, R. Neugart2, M. Neurothz, G.D. Sprouse‘*, P.D. Wheelera, F. Xu‘* and the ISOLDE Collaboration] Spokesman: J. Billowes Contactman: G. Huber Summary The aim of the proposed experiment is to measure the optical isotope shifts and hyperfine structures of bismuth isotopes in the region 21°'2“Bi which lie above the N=126 shell closure. The change in nuclear mean square charge radii and static moments can be deduced. These will be the first isotones of lead to be measured immediately above the shell closure. This will provide new information on the systematics of the kink in the charge radii change with neutron number seen in the Pb isotopic chain, and will represent the first measurement of the odd proton hg/2 moment in the region above the closed 2°8Pb core. Laser resonance fluorescence will be used on the isotopic bismuth samples as they are released into a gas cell trap. This is a method that has been applied very successfully at SUNY, Stony Brook to the neutron deficient bismuth isotopes and it makes efficient use of the small samples available. The bismuth samples of 212Bi and 213Bi will be prepared by catching intense beams of 22°Fr and 2"Fr on thin lead foils. -
WO 2014/138594 Al 12 September 2014 (12.09.2014) P O P C T
(12) INTERNATIONAL APPLICATION PUBLISHED UNDER THE PATENT COOPERATION TREATY (PCT) (19) World Intellectual Property Organization International Bureau (10) International Publication Number (43) International Publication Date WO 2014/138594 Al 12 September 2014 (12.09.2014) P O P C T (51) International Patent Classification: ue, Unit 1, Somerville, Massachusetts 02143 (US). PA- C12P 7/52 (2006.01) POULIS, Andrew; 186 Turnpike Street, Canton, Mas sachusetts 02021 (US). KORYABKINA, Natalya A.; (21) International Application Number: 6214 Avalon Drive, Wilmington, Massachusetts 01887 PCT/US20 14/02 1796 (US). (22) International Filing Date: (74) Agents: MORRELL, Dennis G. et al; 271 Salem Street, 7 March 2014 (07.03.2014) Unit L, Woburn, Massachusetts 01801 (US). (25) Filing Language: English (81) Designated States (unless otherwise indicated, for every (26) Publication Language: English kind of national protection available): AE, AG, AL, AM, AO, AT, AU, AZ, BA, BB, BG, BH, BN, BR, BW, BY, (30) Priority Data: BZ, CA, CH, CL, CN, CO, CR, CU, CZ, DE, DK, DM, 61/774,684 8 March 2013 (08.03.2013) US DO, DZ, EC, EE, EG, ES, FI, GB, GD, GE, GH, GM, GT, 61/774,773 8 March 2013 (08.03.2013) US HN, HR, HU, ID, IL, IN, IR, IS, JP, KE, KG, KN, KP, KR, 61/774,73 1 8 March 2013 (08.03.2013) us KZ, LA, LC, LK, LR, LS, LT, LU, LY, MA, MD, ME, 61/774,735 8 March 2013 (08.03.2013) us MG, MK, MN, MW, MX, MY, MZ, NA, NG, NI, NO, NZ, 61/774,740 8 March 2013 (08.03.2013) us OM, PA, PE, PG, PH, PL, PT, QA, RO, RS, RU, RW, SA, 61/774,744 8 March 2013 (08.03.2013) us SC, SD, SE, SG, SK, SL, SM, ST, SV, SY, TH, TJ, TM, 61/774,746 8 March 2013 (08.03.2013) us TN, TR, TT, TZ, UA, UG, US, UZ, VC, VN, ZA, ZM, 61/774,750 8 March 2013 (08.03.2013) us ZW. -
Circular of the Bureau of Standards No. 562: Bibliography of Research on Deuterium and Tritium Compounds 1945 and 1952
NBS CIRCULAR 562 Bibliography of Research on Deuterium and Tritium Compounds 1945 to 1952 UNITED STATES DEPARTMENT OF COMMERCE NATIONAL BUREAU OF STANDARDS PERIODICALS OF THE NATIONAL BUREAU OF STANDARDS (Published monthly) The National Bureau of Standards is engaged in fundamental and applied research in physics, chemistry, mathematics, and engineering. Projects are conducted in fifteen fields: electricity and electronics, optics and metrology, heat and power, atomic and radiation physics, chemistry, mechanics, organic and fibrous materials, metallurgy, mineral products, building technology, applied mathematics, data process¬ ing systems, cryogenic engineering, radio propagation, and radio standards. The Bureau has custody of the national standards of measurement and conducts research leading to the improvement of scientific and engineering standards and of techniques and methods of measurement. Testing methods and in¬ struments are developed; physical constants and properties of materials are determined; and technical processes are investigated. Journal of Research The Journal presents research papers by authorities in the specialized fields of physics, mathematics, chemistry, and engineering. Complete details of the work are presented, including laboratory data, experimental procedures, and theoretical and mathematical analyses. Annual subscription: domestic, $4.00; 25 cents additional for foreign mailing. Technical News Bulletin Summaries of current research at the National Bureau of Standards are published each month in the Technical News Bulletin. The articles are brief, with emphasis on the results of research, chosen on the basis of their scientific or technologic importance. Lists of all Bureau publications during the preceding month are given, including Research Papers, Handbooks, Applied Mathematics Series, Building Mate¬ rials and Structures Reports, Miscellaneous Publications, and Circulars. -
Investigational New Drug Applications for Positron Emission Tomography (PET) Drugs
Guidance Investigational New Drug Applications for Positron Emission Tomography (PET) Drugs GUIDANCE U.S. Department of Health and Human Services Food and Drug Administration Center for Drug Evaluation and Research (CDER) December 2012 Clinical/Medical Guidance Investigational New Drug Applications for Positron Emission Tomography (PET) Drugs Additional copies are available from: Office of Communications Division of Drug Information, WO51, Room 2201 Center for Drug Evaluation and Research Food and Drug Administration 10903 New Hampshire Ave. Silver Spring, MD 20993-0002 Phone: 301-796-3400; Fax: 301-847-8714 [email protected] http://www.fda.gov/Drugs/GuidanceComplianceRegulatoryInformation/Guidances/default.htm U.S. Department of Health and Human Services Food and Drug Administration Center for Drug Evaluation and Research (CDER) December 2012 Clinical/Medical Contains Nonbinding Recommendations TABLE OF CONTENTS I. INTRODUCTION..............................................................................................................................................1 II. BACKGROUND ................................................................................................................................................1 A. PET DRUGS .....................................................................................................................................................1 B. IND..................................................................................................................................................................2 -
Chapter 3 the Fundamentals of Nuclear Physics Outline Natural
Outline Chapter 3 The Fundamentals of Nuclear • Terms: activity, half life, average life • Nuclear disintegration schemes Physics • Parent-daughter relationships Radiation Dosimetry I • Activation of isotopes Text: H.E Johns and J.R. Cunningham, The physics of radiology, 4th ed. http://www.utoledo.edu/med/depts/radther Natural radioactivity Activity • Activity – number of disintegrations per unit time; • Particles inside a nucleus are in constant motion; directly proportional to the number of atoms can escape if acquire enough energy present • Most lighter atoms with Z<82 (lead) have at least N Average one stable isotope t / ta A N N0e lifetime • All atoms with Z > 82 are radioactive and t disintegrate until a stable isotope is formed ta= 1.44 th • Artificial radioactivity: nucleus can be made A N e0.693t / th A 2t / th unstable upon bombardment with neutrons, high 0 0 Half-life energy protons, etc. • Units: Bq = 1/s, Ci=3.7x 1010 Bq Activity Activity Emitted radiation 1 Example 1 Example 1A • A prostate implant has a half-life of 17 days. • A prostate implant has a half-life of 17 days. If the What percent of the dose is delivered in the first initial dose rate is 10cGy/h, what is the total dose day? N N delivered? t /th t 2 or e Dtotal D0tavg N0 N0 A. 0.5 A. 9 0.693t 0.693t B. 2 t /th 1/17 t 2 2 0.96 B. 29 D D e th dt D h e th C. 4 total 0 0 0.693 0.693t /th 0.6931/17 C. -
A New Gamma Camera for Positron Emission Tomography
INIS-mf—11552 A new gamma camera for Positron Emission Tomography NL89C0813 P. SCHOTANUS A new gamma camera for Positron Emission Tomography A new gamma camera for Positron Emission Tomography PROEFSCHRIFT TER VERKRIJGING VAN DE GRAAD VAN DOCTOR AAN DE TECHNISCHE UNIVERSITEIT DELFT, OP GEZAG VAN DE RECTOR MAGNIFICUS, PROF.DRS. P.A. SCHENCK, IN HET OPENBAAR TE VERDEDIGEN TEN OVERSTAAN VAN EEN COMMISSIE, AANGEWEZEN DOOR HET COLLEGE VAN DECANEN, OP DINSDAG 20 SEPTEMBER 1988TE 16.00 UUR. DOOR PAUL SCHOTANUS '$ DOCTORANDUS IN DE NATUURKUNDE GEBOREN TE EINDHOVEN Dit proefschrift is goedgekeurd door de promotor Prof.dr. A.H. Wapstra s ••I Sommige boeken schijnen geschreven te zijn.niet opdat men er iets uit zou leren, maar opdat men weten zal, dat de schrijver iets geweten heeft. Goethe Contents page 1 Introduction 1 2 Nuclear diagnostics as a tool in medical science; principles and applications 2.1 The position of nuclear diagnostics in medical science 2 2.2 The detection of radiation in nuclear diagnostics: 5 standard techniques 2.3 Positron emission tomography 7 2.4 Positron emitting isotopes 9 2.5 Examples of radiodiagnostic studies with PET 11 2.6 Comparison of PET with other diagnostic techniques 12 3 Detectors for positron emission tomography 3.1 The absorption d 5H keV annihilation radiation in solids 15 3.2 Scintillators for the detection of annihilation radiation 21 3.3 The detection of scintillation light 23 3.4 Alternative ways to detect annihilation radiation 28 3-5 Determination of the point of annihilation: detector geometry, -
Electron Capture in Stars
Electron capture in stars K Langanke1;2, G Mart´ınez-Pinedo1;2;3 and R.G.T. Zegers4;5;6 1GSI Helmholtzzentrum f¨urSchwerionenforschung, D-64291 Darmstadt, Germany 2Institut f¨urKernphysik (Theoriezentrum), Department of Physics, Technische Universit¨atDarmstadt, D-64298 Darmstadt, Germany 3Helmholtz Forschungsakademie Hessen f¨urFAIR, GSI Helmholtzzentrum f¨ur Schwerionenforschung, D-64291 Darmstadt, Germany 4 National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA 5 Joint Institute for Nuclear Astrophysics: Center for the Evolution of the Elements, Michigan State University, East Lansing, Michigan 48824, USA 6 Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA E-mail: [email protected], [email protected], [email protected] Abstract. Electron captures on nuclei play an essential role for the dynamics of several astrophysical objects, including core-collapse and thermonuclear supernovae, the crust of accreting neutron stars in binary systems and the final core evolution of intermediate mass stars. In these astrophysical objects, the capture occurs at finite temperatures and at densities at which the electrons form a degenerate relativistic electron gas. The capture rates can be derived in perturbation theory where allowed nuclear transitions (Gamow-Teller transitions) dominate, except at the higher temperatures achieved in core-collapse supernovae where also forbidden transitions contribute significantly to the rates. There has been decisive progress in recent years in measuring Gamow-Teller (GT) strength distributions using novel experimental techniques based on charge-exchange reactions. These measurements provide not only data for the GT distributions of ground states for many relevant nuclei, but also serve as valuable constraints for nuclear models which are needed to derive the capture rates for the arXiv:2009.01750v1 [nucl-th] 3 Sep 2020 many nuclei, for which no data exist yet. -
2.3 Neutrino-Less Double Electron Capture - Potential Tool to Determine the Majorana Neutrino Mass by Z.Sujkowski, S Wycech
DEPARTMENT OF NUCLEAR SPECTROSCOPY AND TECHNIQUE 39 The above conservatively large systematic hypothesis. TIle quoted uncertainties will be soon uncertainty reflects the fact that we did not finish reduced as our analysis progresses. evaluating the corrections fully in the current analysis We are simultaneously recording a large set of at the time of this writing, a situation that will soon radiative decay events for the processes t e'v y change. This result is to be compared with 1he and pi-+eN v y. The former will be used to extract previous most accurate measurement of McFarlane the ratio FA/Fv of the axial and vector form factors, a et al. (Phys. Rev. D 1984): quantity of great and longstanding interest to low BR = (1.026 ± 0.039)'1 I 0 energy effective QCD theory. Both processes are as well as with the Standard Model (SM) furthermore very sensitive to non- (V-A) admixtures in prediction (Particle Data Group - PDG 2000): the electroweak lagLangian, and thus can reveal BR = (I 038 - 1.041 )*1 0-s (90%C.L.) information on physics beyond the SM. We are currently analyzing these data and expect results soon. (1.005 - 1.008)* 1W') - excl. rad. corr. Tale 1 We see that even working result strongly confirms Current P1IBETA event sxpelilnentstatistics, compared with the the validity of the radiative corrections. Another world data set. interesting comparison is with the prediction based on Decay PIBETA World data set the most accurate evaluation of the CKM matrix n >60k 1.77k element V d based on the CVC hypothesis and ihce >60 1.77_ _ _ results -
1. Public Health Statement
AMERICIUM 1 1. PUBLIC HEALTH STATEMENT This public health statement tells you about americium and the effects of exposure. The Environmental Protection Agency (EPA) identifies the most serious hazardous waste sites in the nation. These sites make up the National Priorities List (NPL) and are the sites targeted for long-term federal cleanup activities. Americium has been found in at least 8 of the 1,636 current or former NPL sites. However, the total number of NPL sites evaluated for americium is not known. As more sites are evaluated, the sites at which americium is found may increase. This information is important because exposure to americium may harm you and because these sites may be sources of exposure. When a substance is released from a large area, such as an industrial plant, or from a container, such as a drum or bottle, it enters the environment. This release does not always lead to exposure. You are normally exposed to a substance only when you come in contact with it. You may be exposed by breathing, eating, or drinking the substance, or by skin contact. However, since americium is radioactive, you can also be exposed to its radiation if you are near it. External or internal exposure to radiation may occur from natural or man-made sources. Naturally occurring sources of radiation are cosmic radiation from space or naturally occurring radioactive materials in our body or in soil, air, water, or building materials. Man-made sources of radiation are found in consumer products, industrial equipment, atom bomb fallout, and to a smaller extent, from hospital waste and nuclear reactors. -
(A) Two Stable Isotopes of Lithium and Have Respective Abundances of And
NCERT Solution for Class 12 Physics :Chapter 13 Nuclei Q.13.1 (a) Two stable isotopes of lithium and have respective abundances of and . These isotopes have masses and , respectively. Find the atomic mass of lithium. Answer: Mass of the two stable isotopes and their respective abundances are and and and . m=6.940934 u Q. 13.1(b) Boron has two stable isotopes, and . Their respective masses are and , and the atomic mass of boron is 10.811 u. Find the abundances of and . Answer: The atomic mass of boron is 10.811 u Mass of the two stable isotopes are and respectively Let the two isotopes have abundances x% and (100-x)% Aakash Institute Therefore the abundance of is 19.89% and that of is 80.11% Q. 13.2 The three stable isotopes of neon: and have respective abundances of , and . The atomic masses of the three isotopes are respectively. Obtain the average atomic mass of neon. Answer: The atomic masses of the three isotopes are 19.99 u(m 1 ), 20.99 u(m 2 ) and 21.99u(m 3 ) Their respective abundances are 90.51%(p 1 ), 0.27%(p 2 ) and 9.22%(p 3 ) The average atomic mass of neon is 20.1771 u. Q. 13.3 Obtain the binding energy( in MeV ) of a nitrogen nucleus , given m Answer: m n = 1.00866 u m p = 1.00727 u Atomic mass of Nitrogen m= 14.00307 u Mass defect m=7 m n +7 m p - m m=7Aakash 1.00866+7 1.00727 - 14.00307 Institute m=0.10844 Now 1u is equivalent to 931.5 MeV E b =0.10844 931.5 E b =101.01186 MeV Therefore binding energy of a Nitrogen nucleus is 101.01186 MeV. -
Positron Emission Tomography
Positron emission tomography A.M.J. Paans Department of Nuclear Medicine & Molecular Imaging, University Medical Center Groningen, The Netherlands Abstract Positron Emission Tomography (PET) is a method for measuring biochemical and physiological processes in vivo in a quantitative way by using radiopharmaceuticals labelled with positron emitting radionuclides such as 11C, 13N, 15O and 18F and by measuring the annihilation radiation using a coincidence technique. This includes also the measurement of the pharmacokinetics of labelled drugs and the measurement of the effects of drugs on metabolism. Also deviations of normal metabolism can be measured and insight into biological processes responsible for diseases can be obtained. At present the combined PET/CT scanner is the most frequently used scanner for whole-body scanning in the field of oncology. 1 Introduction The idea of in vivo measurement of biological and/or biochemical processes was already envisaged in the 1930s when the first artificially produced radionuclides of the biological important elements carbon, nitrogen and oxygen, which decay under emission of externally detectable radiation, were discovered with help of the then recently developed cyclotron. These radionuclides decay by pure positron emission and the annihilation of positron and electron results in two 511 keV γ-quanta under a relative angle of 180o which are measured in coincidence. This idea of Positron Emission Tomography (PET) could only be realized when the inorganic scintillation detectors for the detection of γ-radiation, the electronics for coincidence measurements, and the computer capacity for data acquisition and image reconstruction became available. For this reason the technical development of PET as a functional in vivo imaging discipline started approximately 30 years ago. -
Nuclear Equations
Nuclear Equations In nuclear equations, we balance nucleons (protons and neutrons). The atomic number (number of protons) and the mass number (number of nucleons) are conserved during the reaction. Nuclear Equations Alpha Decay Nuclear Equations Beta Decay Nuclear Equations Beta Decay Nuclear Equations Positron Emission: A positron is a particle equal in mass to an electron but with opposite charge. Nuclear Equations Electron Capture: A nucleus absorbs an electron from the inner shell. Nuclear Equations EXAMPLE 4.1 Balancing Nuclear Equations Write balanced nuclear equations for each of the following processes. In each case, indicate what new element is formed. a. Plutonium-239 emits an alpha particle when it decays. b. Protactinium-234 undergoes beta decay. c. Carbon-11 emits a positron when it decays. d. Carbon-11 undergoes electron capture. EXAMPLE 4.1 Balancing Nuclear Equations continued Exercise 4.1 Write balanced nuclear equations for each of the following processes. In each case, indicate what new element is formed. a. Radium-226 decays by alpha emission. b. Sodium-24 undergoes beta decay. c. Gold-188 decays by positron emission. d. Argon-37 undergoes electron capture. EXAMPLE 4.2 More Nuclear Equations 5 In the upper atmosphere, a nitrogen-14 nucleus absorbs a neutron. A carbon-14 nucleus and another particle are formed. What is the other particle? Half-Life Half-life of a radioactive sample is the time required for ½ of the material to undergo radioactive decay. Half-Life Half-Life Fraction Remaining = 1/2n Half-life T1/2 = 0.693/ k(decay constant) If you know how much you started with and how much you ended with, then you can determine the number of half-lives.