Prompt γ-rays from Neutron Inelastic
|
|
- Aubrie Norma Lawson
- 5 years ago
- Views:
Transcription
1 Prompt γ-rays from Neutron Inelastic Scattering at FaNGaS: Benchmark Spectrum Analysis T.H. Randriamalala, M. Rossbach Institute of Energy and Climate Research, Nuclear Waste Management and Reactor Safety, Forschungszentrum Jülich GmbH, Germany August 23-28, 2015 MTAA 14 Delft, The Netherlands
2 Outline Introduction & Motivation Experimental Setup Sample Properties Benchmark Studies Conclusion & Outlook T.H. Randriamalala August 28, 2015 MTAA 14 2
3 Introduction & Motivation Prompt γ-rays Neutron Activation Analysis (m n, E ther. ) (m n, E > E T ) (m n, E ) Requirement for the use of fast neutrons interrogation: Knowledge of the absolute intensities or/and the partial cross section of (prompt) γ-rays Knowledge of the total (n, n γ) cross section T.H. Randriamalala August 28, 2015 MTAA 14 3
4 Introduction & Motivation FaNGaS The Fast Neutron Gamma Spectrometry aims to investigate (n, n γ) reaction using the ssion neutrons at FRM II, Garching. Scope of presentation: Confrontation of the measured intensity and count rate of γ-rays with the existing data or with the calculation results from theoretical model. T.H. Randriamalala August 28, 2015 MTAA 14 4
5 The Facility D 2 7 = 548 cm D 7 6 = 67 cm 1 Reactor core 4 Inner collimator 7 Irradiation position 2 Convertor plates (93% 235 U) 5 Outer collimator 8 Decay measurement 3 SR10 beam line 6 Shielded 50% HPGe position detector T.H. Randriamalala August 28, 2015 MTAA 14 5
6 FaNGaS Instrument Outer 2 Sample holder 3 γ 4 Detector shielding 5 collimator collimator (PE 5 n B4 C Pb ) Iron frame support W H L 126 cm 126 cm 266 cm Weight 4 tonnes Movable instrument T.H. Randriamalala August 28, 2015 MTAA 14 6
7 Beam Characteristic Neutron Beam Spectrum (Very pure) foil activation technique: Sample irrad. time 10 h Decay meas. time 1-2 h 12 threshold and 5 (n, γ) reactions Spectrum unfolding using STAYSL PNNL 1 code: Parametrized prior ux 2 : φ(e) = α t E exp( E/kT ) + α i E (1+c) exp( d/ E) + α f exp( E/a) sinh( be) 1 F.G. Perey, ORNL-TM-6062(1997). 2 H. Breitkreuz et al. NIM A 593 (2008) 466. T.H. Randriamalala August 28, 2015 MTAA 14 7
8 Beam Characteristic Neutron Beam Spectrum 10 8 E φ [MeV cm 2 s 1 ] E 2.1 MeV φde 10 8 cm 2 s 1 α f /α t > E [kev] Fast neutron beam energy spectrum at FaNGaS T.H. Randriamalala August 28, 2015 MTAA 14 8
9 FaNGaS Spectrometer n-type HPGe:GMX50-83, ORTEC Data acquisition: DSPEC-50, ORTEC + GammaVision-32 Spectrum evaluation: HYPERMET-PC Efficiency Ba Cl(n,γ) Co Cs Eu Cl 3 10 Energy [kev] 4 10 Detector eciency for prompt γ-rays (67 cm away from the detector) T.H. Randriamalala August 28, 2015 MTAA 14 9
10 Background H-D.E. N Ge 72 Ar, Ge In Ge C Al Pb 27 Pb 65 Cu 70 Ge Cu 63 Counts Pb 72 Ge 56,56Mn Ge Ge Pb 74 Ge Counts Pb Annih. B Ge 71m 75 m Ge Ge { H-S.E. X Energy [kev] Energy [kev] S.E. 55 -D.P. -S.E. -D.P.-S.E. 55 Counts D.E. 13 C -D.E. 14 N 12 C C C-S.E Counts N Pb 104 -D.P.-D.E S.E. -S.E. 2 H Energy [kev] Total count rate beam on: 4000 cps Strong lines: H(110 cps), B(36 cps), (5 cps) Fast neutron rate at the detector 10 s 1 (from Ge(n, n0 γ) Ge) 74 T.H. Randriamalala 3500 Energy [kev] August 28, 2015 MTAA 14 10
11 Sample Properties Foil Θ [mm] m [g] purity [%] Be Al Ti Co Ni Cu Zr Nb Rh Pd Cd In W Pt Pb U T.H. Randriamalala August 28, 2015 MTAA 14 11
12 Sample Properties Foil Θ [mm] m [g] purity [%] Be Al Ti Co Ni Cu Zr Nb Rh Pd Cd In W Pt Pb U T.H. Randriamalala August 28, 2015 MTAA 14 11
13 Benchmark Spectrum Found γ-rays are matched with γ-rays transition based on ENSDF a 83 γ-rays found: 54 (7), 56 (72), (4) Counts a Energy [kev] Prompt γ-rays from iron sample irradiation T.H. Randriamalala August 28, 2015 MTAA 14 12
14 Benchmark Analysis Found γ-rays Isotope Demidov 3 FaNGaS Missed by FaNGaS Co Ni Cu A.M Demidov et al., ATLAS of Gamma-Ray Spectra from Inelastic Scattering of Reactor Fast Neutrons Moscow (1978). T.H. Randriamalala August 28, 2015 MTAA 14 13
15 Benchmark Analysis I/I Dem Co Ni Cu E [kev] Relative γ-ray intensities compared to those of Demidov T.H. Randriamalala August 28, 2015 MTAA 14 13
16 Rate Comparison Measured count rate: R meas = R N = C Nεκt meas C : the counts in the peak ε: the eciency t meas : the measurement time κ: a correction factor (sample self-shielding) Calculated count rate: R calc = R N = σ p (E)φ(E)dE σ p : the γ-ray production cross section calculated from TALYS 3 φ: the determined ux 3 T.H. Randriamalala August 28, 2015 MTAA 14 14
17 Rate Comparison meas. 56 calc. 54 meas calc. R [ atom 1.s 1 ] R/R c E [kev] T.H. Randriamalala August 28, 2015 MTAA 14 15
18 Rate Comparison Co meas. 59 Co calc R [ atom 1.s 1 ] R/R c E [kev] T.H. Randriamalala August 28, 2015 MTAA 14 15
19 Rate Comparison Ni meas. 58 Ni calc R [ atom 1.s 1 ] R/R c E [kev] T.H. Randriamalala August 28, 2015 MTAA 14 15
20 Rate Comparison Cu meas. 63 Cu calc R [ atom 1.s 1 ] R/R c E [kev] T.H. Randriamalala August 28, 2015 MTAA 14 15
21 Conclusion Neutron inelastic (prompt) γ-rays were measured using 10 8 n cm 2 s 1 with Ē = 2.1 MeV at FaNGaS. FaNGaS can resolve a larger part of the γ-rays (cp. Demidov 1978) Measured intensity and count rate of γ-rays agreed with existing data. Outlook γ & n background reduction Total and partial cross sections determination Build an (n, n γ) catalog of elements T.H. Randriamalala August 28, 2015 MTAA 14 16
22 FaNGaS Collaboration: FZ-Jülich GmbH: M. Rossbach, T. Randriamalala, E.Mauerhofer MLZ, Garching: Zs. Révay, P. Kudejova, S. Söllradl, F. Wagner, C. Genreith FaNGaS is supported by BMBF. Project Nr: 02S9052A T.H. Randriamalala August 28, 2015 MTAA 14 17
23 Thanks for your attention!
24 Foils Mass [g] Reaction E thr [MeV ] R [/atom s] Al Al(n, p) 27 Mg (5.40 ± 0.14) Al(n, α) 24 Na (1.22 ± 0.04) Ti Ti(n, p) 46 Sc (1.87 ± 0.35) Ti(n, p) 47 Sc (2.19 ± 0.05) Ti(n, p) 48 Sc (5.45 ± 0.21) (n, p) 56 Mn (1.99 ± 0.07) Co Co(n, α) 56 Mn (4.00 ± 0.15) Ni Ni(n, p) 58 Co (9.67 ± 0.21) Ni(n, p) 61 Co 49 (2.45 ± 0.14) Cu Cu(n, p) 65 Ni (6.14 ± 0.37) Rh Rh(n, n ) 103m Rh (4.05 ± 0.36) In In(n, n ) 115m In (2.42 ± 0.04) (n, γ) 59 (3.22 ± 0.29) Co Co(n, γ) 60m Co (9.78 ± 0.22) In In(n, γ) 116m In (5.03 ± 0.08) W W(n, γ) 187 W (3.86 ± 0.10) Au Au(n, γ) 198 Au (9.59 ± 0.09) 10 17
Partial Neutron Capture Cross Section Determination of 237 Np, 242
Partial Neutron Capture Cross Section Determination of 237 Np, 242 Pu and 241 Am using Cold Neutron Beams Christoph Genreith 1, Matthias Rossbach 1 1 Institute of Energy and Climate Research, IEK-6, Forschungszentrum
More informationApplication of prompt gamma activation analysis with neutron beams for the detection and analysis of nuclear materials in containers
Application of prompt gamma activation analysis with neutron beams for the detection and analysis of nuclear materials in containers Zsolt Révay Institute of Isotopes, Budapest, Hungary Dept. of Nuclear
More informationCross-section Measurements of Relativistic Deuteron Reactions on Copper by Activation Method
Nuclear Physics Institute, Academy of Sciences of the Czech Republic Department of Nuclear Reactors, Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague Cross-section
More informationIntegral cross section measurements using TRIGA reactor and Am/Be neutron source
Page 117 Integral cross section measurements using TRIGA reactor and Am/Be neutron source M.S. Uddin 1*, S.M. Hossain 1, M.R. Zaman 2, S. Sudár 3 and S.M. Qaim 4 1 Institute of Nuclear Science and Technology
More informationHigh precision neutron inelastic cross section measurements
High precision neutron inelastic cross section measurements A. Olacel, C. Borcea, M. Boromiza, A. Negret IFIN-HH, DFN Outline The experimental setup GELINA GAINS Data analysis algorithm. Monte Carlo simulations
More informationCOMPARATIVE STUDY OF PIGE, PIXE AND NAA ANALYTICAL TECHNIQUES FOR THE DETERMINATION OF MINOR ELEMENTS IN STEELS
COMPARATIVE STUDY OF PIGE, PIXE AND NAA ANALYTICAL TECHNIQUES FOR THE DETERMINATION OF MINOR ELEMENTS IN STEELS ANTOANETA ENE 1, I. V. POPESCU 2, T. BÃDICÃ 3, C. BEªLIU 4 1 Department of Physics, Faculty
More informationHigh-energy calibration data for neutron activation analysis
Nuclear Analysis and Radiography Department High-energy calibration data for neutron activation analysis L. Szentmiklósi 1, Zs. Révay 2, B. Maróti 1, D. Párkányi 1, I. Harsányi 1 1 Nuclear Analysis and
More informationIon-beam techniques. Ion beam. Electrostatic Accelerators. Van de Graaff accelerator Pelletron Tandem Van de Graaff
Ion-beam techniques RBS Target nucleus Ion beam STIM RBS: Rutherford backscattering ERD: Elastic recoil detection PIXE: Particle induced x-ray emission PIGE: Particle induced gamma emission NRA: Nuclear
More informationMeasurement of neutron energy spectrum at the radial channel No. 4 of the Dalat reactor
DOI 10.1186/s40064-016-2585-7 CASE STUDY Open Access Measurement of neutron energy spectrum at the radial channel No. 4 of the Dalat reactor Pham Ngoc Son 1* and Vuong Huu Tan 2 *Correspondence: pnson.nri@gmail.com
More informationTHE STRUCTURE OF ATOMS. ATOMS Atoms consist of a number of fundamental particles, the most important ones are...
Atomic Structure THE STRUCTURE OF ATOMS ATOMS Atoms consist of a number of fundamental particles, the most important ones are... Mass / kg Charge / C Relative mass Relative Charge PROTON NEUTRON ELECTRON
More informationThe first model was based only on the CANBERRA information which we. drawing. Canberra refused any other information.
Experimental and Monte Carlo determination of Gamma Spectrometry Efficiency Pavel Dryak, Petr Kovář Czech Metrology Institute February 2009 Leading motive of our testing The producer send the drawing after
More informationThis work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under contract
This work was performed under the auspices of the U.S. Department of Energy by under contract DE-AC52-7NA27344. Lawrence Livermore National Security, LLC The ITER tokamak Tungsten (W) is attractive as
More informationPreparatory experiments for cold-neutron induced fission studies at IKI
Preparatory experiments for cold-neutron induced fission studies at IKI A. Oberstedt 1, S. Oberstedt 2, R. Billnert 1, J. Karlsson 1, X. Ledoux 3, J.-G. Marmouget 3 and F.-J. Hambsch 2 1 School of Science
More informationCross-section section measurements of neutron threshold reactions in various materials
Nuclear Physics Institute, Academy of Sciences of Czech Republic Department of Nuclear Reactors, Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague Cross-section
More informationElement Cube Project (x2)
Element Cube Project (x2) Background: As a class, we will construct a three dimensional periodic table by each student selecting two elements in which you will need to create an element cube. Helpful Links
More informationPhotofission of 238-U Nuclei
Photofission of 238-U Nuclei International Thorium Energy Conference - ThEC18, 29-31st of October 2018, Belgium İsmail Boztosun This research has been supported by TÜBİTAK with grant number 114F220 Motivations
More informationKIVI 9 Oct 2015 Fysische Beeldtechnieken 18 feb
1 2 3 Dutch Isotopes Valley Stable Isotopes 4 Patient-hospital: how to recognize the disorder? How to find a targeting molecule? How to make new radionuclides? How to combine? How to test stability? How
More information1 of 5 14/10/ :21
X-ray absorption s, characteristic X-ray lines... 4.2.1 Home About Table of Contents Advanced Search Copyright Feedback Privacy You are here: Chapter: 4 Atomic and nuclear physics Section: 4.2 Absorption
More informationDetermination of the activity of radionuclides
BUREAU NATIONAL DE MÉTROLOGIE COMMISSARIAT À L'ÉNERGIE ATOMIQUE LABORATOIRE NATIONAL HENRI BECQUEREL Note technique LNHB/04-33 Determination of the activity of radionuclides contained in volume samples
More informationCross-section Measurements of (n,xn) Threshold Reactions
Nuclear Physics Institute, Academy of Sciences of Czech Republic Department of Nuclear Reactors, Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague Cross-section
More informationExperimental Activities in China
Experimental Activities in China (June 2008 YU Hongwei China Nuclear Data Center, China Institute of Atomic Energy The facilities were used for the nuclear data measurements and studies including the China
More information7) Applications of Nuclear Radiation in Science and Technique (1) Analytical applications (Radiometric titration)
7) Applications of Nuclear Radiation in Science and Technique (1) (Radiometric titration) The radioactive material is indicator Precipitation reactions Complex formation reactions Principle of a precipitation
More informationAtomic Physics. Chapter 6 X ray. Jinniu Hu 24/12/ /20/13
Atomic Physics Chapter 6 X ray 11/20/13 24/12/2018 Jinniu Hu 1!1 6.1 The discovery of X ray X-rays were discovered in 1895 by the German physicist Wilhelm Roentgen. He found that a beam of high-speed electrons
More informationDeuteron activation cross section measurements at the NPI cyclotron
Nuclear Physics Institute Řež EAF 2011 Deuteron activation cross section measurements at the NPI cyclotron E. Šimečková, P. Bém, M. Honusek, J. Mrázek, M. Štefánik, L. Závorka Nuclear Physics Institute
More informationREFERENCE SOURCES FOR THE CALIBRATION OF THE AUTOCORRELATION SINGLE-CRYSTAL SCINTILLATION TIME SPECTROMETER
REFERENCE SOURCES FOR THE CALIBRATION OF THE AUTOCORRELATION SINGLE-CRYSTAL SCINTILLATION TIME SPECTROMETER V.A. MOROZOV 1, N.V. MOROZOVA 1, T. BĂDICĂ 2, D. DELEANU 2,3, D. GHIŢĂ 2, S. PASCU 2,3 1 Joint
More informationUnit 1 Part 2 Atomic Structure and The Periodic Table Introduction to the Periodic Table UNIT 1 ATOMIC STRUCTURE AND THE PERIODIC TABLE
UNIT 1 ATOMIC STRUCTURE AND THE PERIODIC TABLE PART 2 INTRODUCTION TO THE PERIODIC TABLE Contents 1. The Structure of the Periodic Table 2. Trends in the Periodic Table Key words: group, period, block,
More informationThe Periodic Table. Periodic Properties. Can you explain this graph? Valence Electrons. Valence Electrons. Paramagnetism
Periodic Properties Atomic & Ionic Radius Energy Electron Affinity We want to understand the variations in these properties in terms of electron configurations. The Periodic Table Elements in a column
More informationTopic 3: Periodicity OBJECTIVES FOR TODAY: Fall in love with the Periodic Table, Interpret trends in atomic radii, ionic radii, ionization energies &
Topic 3: Periodicity OBJECTIVES FOR TODAY: Fall in love with the Periodic Table, Interpret trends in atomic radii, ionic radii, ionization energies & electronegativity The Periodic Table What is the periodic
More informationExperimental Determination of Cross Sections for (n,x) Nuclear Reactions
WDS'07 Proceedings of Contributed Papers, Part III, 188 192, 2007. ISBN 978-80-7378-025-8 MATFYZPRESS Experimental Determination of Cross Sections for (n,x) Nuclear Reactions N. Dzysiuk and I. Kadenko
More informationExperimental determination of (n,x( n,x) cross sections on germanium (Ge( Ge), terbium (Tb) and lutetium (Lu)
Dzysiuk Nataliya and Kadenko Igor Experimental determination of (n,x( n,x) cross sections on germanium (Ge( Ge), terbium (Tb) and lutetium (Lu) Workshop on Nuclear reaction Data for Advanced Reactor Technologies
More informationBackground by Neutron Activation in GERDA
Background by Neutron Activation in GERDA Georg Meierhofer people involved: Kepler Center for Astro and Particle Physics University Tübingen P. Grabmayr J. Jochum P. Kudejova L. Canella J. Jolie IKP, Universität
More informationORBITAL DIAGRAM - A graphical representation of the quantum number "map" of electrons around an atom.
160 ORBITAL DIAGRAM - A graphical representation of the quantum number "map" of electrons around an atom. 4p 3d 4s 3p 3s 2p 2s 1s Each blank represents an ORBITAL, and can hold two electrons. The 4s subshell
More informationPerformance of the True Coincidence Correction Method in GammaVision. Keyser, Ronald M., Haywood, Susan E., and Upp, Daniel L.
Performance of the True Coincidence Correction Method in GammaVision Keyser, Ronald M., Haywood, Susan E., and Upp, Daniel L. ORTEC, PerkinElmer Instruments, Inc. 801 South Illinois Avenue, Oak Ridge,
More informationBertram Blank CEN Bordeaux-Gradignan. Germanium detector calibration experimental studies: decay mirror decay future work
Bertram Blank CEN Bordeaux-Gradignan Germanium detector calibration experimental studies: 0 + -0 + decay mirror decay future work 20 th Colloque de GANIL, Amboise, October 15th 20th, 2017 Nuclear beta
More informationThe Possibility to Use Energy plus Transmutation Setup for Neutron Production and Transport Benchmark Studies
The Possibility to Use Energy plus Transmutation Setup for Neutron Production and Transport Benchmark Studies V. WAGNER 1, A. KRÁSA 1, M. MAJERLE 1, F. KŘÍŽEK 1, O. SVOBODA 1, A. KUGLER 1, J. ADAM 1,2,
More informationThe European Activation File: EAF-2005 decay data library
UKAEA FUS 516 EURATOM/UKAEA Fusion The European Activation File: EAF-2005 decay data library R.A. Forrest January 2005 UKAEA EURATOM/UKAEA Fusion Association Culham Science Centre Abingdon Oxfordshire
More informationEXPERIMENTAL STUDY OF NEUTRON FIELDS PRODUCED IN PROTON REACTIONS WITH HEAVY TARGETS. Nuclear Physics Institute AS CR, Rez Czech Republic
EXPERIMENTAL STUDY OF NEUTRON FIELDS PRODUCED IN PROTON REACTIONS WITH HEAVY TARGETS A. Kugler, V. Wagner Nuclear Physics Institute AS CR, 25068 Rez Czech Republic I. Introduction One of important aspects
More informationInvestigation of radiative proton-capture reactions using high-resolution g-ray spectroscopy
Investigation of radiative proton-capture reactions using high-resolution g-ray spectroscopy P. Scholz, F. Heim, J. Mayer, M. Spieker, and A. Zilges Institute for Nuclear Physics, University of Cologne
More informationNeutron Activation of 74 Ge and 76 Ge
Neutron Activation of 74 Ge and 76 Ge people involved: P. Grabmayr J. Jochum Georg Meierhofer P. Kudejova L. Canella J. Jolie IKP, Universität zu Köln Eurograd, Hallstatt 27.09. 29.09.2009 Outline Motivation:
More informationSpin Cut-off Parameter of Nuclear Level Density and Effective Moment of Inertia
Commun. Theor. Phys. (Beijing, China) 43 (005) pp. 709 718 c International Academic Publishers Vol. 43, No. 4, April 15, 005 Spin Cut-off Parameter of Nuclear Level Density and Effective Moment of Inertia
More informationExperimental Activities in China
Experimental Activities in China Yu Hongwei China Nuclear Data Center China Institute of Atomic Energy WPEC Meeting, June 5-6, 2008 Facilities CIAE: China s first experimental heavy water reactor, the
More informationUsing the Periodic Table
MATH SKILLS TRANSPARENCY WORKSHEET Using the Periodic Table 6 Use with Chapter 6, Section 6.2 1. Identify the number of valence electrons in each of the following elements. a. Ne e. O b. K f. Cl c. B g.
More informationFast neutron inelastic scattering Roland Beyer, Forschungszentrum Dresden-Rossendorf
Fast neutron inelastic scattering Roland Beyer, Forschungszentrum Dresden-Rossendorf Institute of Radiation Physics Roland Beyer www.fzd.de Member of the Leibniz Association Data needs for transmutation
More informationStability Nuclear & Electronic (then ion formation/covalent bonding)
Stability Nuclear & Electronic (then ion formation/covalent bonding) Most elements are not stable in their atomic form. (Exceptions to that? ) They become stable by gaining or losing e! to form ions, or
More informationORBITAL DIAGRAM - A graphical representation of the quantum number "map" of electrons around an atom.
178 (MAGNETIC) SPIN QUANTUM NUMBER: "spin down" or "spin up" - An ORBITAL (region with fixed "n", "l" and "ml" values) can hold TWO electrons. ORBITAL DIAGRAM - A graphical representation of the quantum
More informationNucleus. Electron Cloud
Atomic Structure I. Picture of an Atom Nucleus Electron Cloud II. Subatomic particles Particle Symbol Charge Relative Mass (amu) protons p + +1 1.0073 neutrons n 0 1.0087 electrons e - -1 0.00054858 Compare
More informationDIPOLE-STRENGTH IN N=50 NUCLEI STUDIED IN PHOTON-SCATTERING EXPERIMENTS AT ELBE
DIPOLE-STRENGTH IN N=50 NUCLEI STUDIED IN PHOTON-SCATTERING EXPERIMENTS AT ELBE R.Schwengner 1, G.Rusev 1, N.Benouaret 1,2, R.Beyer 1, F.Dönau 1, M.Erhard 1, E.Grosse 1,3, A.R.Junghans 1, K.Kosev 1, J.Klug
More informationCATHODE MATERIAL CHANGE AFTER DEUTERIUM GLOW DISCHARGE EXPERIMENTS
Savvatimova, I., Y. Kucherov, and A.B. Karabut. Cathode Material Change after Deuterium Glow Discharge Experiments. in Fourth International Conference on Cold Fusion. 1993. Lahaina, Maui: Electric Power
More informationHow many grams of sodium metal is required to completely react with 2545 grams of chlorine gas?
EXAMPLE PROBLEM: How many grams of sodium metal is required to completely react with 2545 grams of chlorine gas? 1 - Convert 2545 grams of chlorine to moles chlorine using formula weight 2 - Convert moles
More informationElectromagnetic Dipole Strength distribution in 124,128,134 Xe below the neutron separation energy
Electromagnetic Dipole Strength distribution in 124,128,134 Xe below the neutron separation energy Ralph Massarczyk Helmholtz-Zentrum Dresden-Rossendorf 29.05.2013 R.Massarczyk (HZDR) dipole strength in
More informationRadiometric Dating (tap anywhere)
Radiometric Dating (tap anywhere) Protons Neutrons Electrons Elements on the periodic table are STABLE Elements can have radioactive versions of itself called ISOTOPES!! Page 1 in your ESRT has your list!
More informationM.Cagnazzo Atominstitut, Vienna University of Technology Stadionallee 2, 1020 Wien, Austria
Measurements of the In-Core Neutron Flux Distribution and Energy Spectrum at the Triga Mark II Reactor of the Vienna University of Technology/Atominstitut ABSTRACT M.Cagnazzo Atominstitut, Vienna University
More informationNeutronics experiments for validation of activation and neutron transport data for fusion application at the DT neutron generator of TU Dresden
Neutronics experiments for validation of activation and neutron transport data for fusion application at the DT neutron generator of TU Dresden A. Klix1, A. Domula2, U. Fischer1, D. Gehre2, J. Henniger2,
More informationCLASS TEST GRADE 11. PHYSICAL SCIENCES: CHEMISTRY Test 4: Matter and materials 1
CLASS TEST GRADE PHYSICAL SCIENCES: CHEMISTRY Test 4: Matter and materials MARKS: 45 TIME: hour INSTRUCTIONS AND INFORMATION. Answer ALL the questions. 2. You may use non-programmable calculators. 3. You
More informationThe possibility to use energy plus transmutation set-up for neutron production and transport benchmark studies
PRAMANA c Indian Academy of Sciences Vol. 68, No. 2 journal of February 2007 physics pp. 297 306 The possibility to use energy plus transmutation set-up for neutron production and transport benchmark studies
More informationHow many grams of sodium metal is required to completely react with 2545 grams of chlorine gas?
146 EXAMPLE PROBLEM: How many grams of sodium metal is required to completely react with 2545 grams of chlorine gas? 1 - Convert 2545 grams of chlorine gas to moles. Use formula weight. 2 - Convert moles
More informationNeutron transmission and capture measurements for 241 Am at GELINA
Neutron transmission and capture measurements for 241 Am at GELINA C. Lampoudis, S. Kopecky, A. Plompen, C. Sage P. Schillebeeckx, R. Wynants, O. Bouland, G. Noguere and F. Gunsing 3 rd International Workshop
More informationAtoms and the Periodic Table
Atoms and the Periodic Table Parts of the Atom Proton Found in the nucleus Number of protons defines the element Charge +1, mass 1 Parts of the Atom Neutron Found in the nucleus Stabilizes the nucleus
More informationThe Periodic Table of the Elements
The Periodic Table of the Elements All matter is composed of elements. All of the elements are composed of atoms. An atom is the smallest part of an element which still retains the properties of that element.
More informationVERIFICATION OF MONTE CARLO CALCULATIONS OF THE NEUTRON FLUX IN THE CAROUSEL CHANNELS OF THE TRIGA MARK II REACTOR, LJUBLJANA
International Conference Nuclear Energy for New Europe 2002 Kranjska Gora, Slovenia, September 9-12, 2002 www.drustvo-js.si/gora2002 VERIFATION OF MONTE CARLO CALCULATIONS OF THE NEUTRON FLUX IN THE CAROUSEL
More informationCollimated LaBr 3 detector response function in radioactivity analysis of nuclear waste drums
Nuclear Science and Techniques 4 (13) 63 Collimated LaBr 3 detector response function in radioactivity analysis of nuclear waste drums QIAN Nan 1 WANG Dezhong 1,* WANG Chuan ZHU Yuelong MAUERHOFER Eric
More informationPART 1 Introduction to Theory of Solids
Elsevier UK Job code: MIOC Ch01-I044647 9-3-2007 3:03p.m. Page:1 Trim:165 240MM TS: Integra, India PART 1 Introduction to Theory of Solids Elsevier UK Job code: MIOC Ch01-I044647 9-3-2007 3:03p.m. Page:2
More informationCHEM 10113, Quiz 5 October 26, 2011
CHEM 10113, Quiz 5 October 26, 2011 Name (please print) All equations must be balanced and show phases for full credit. Significant figures count, show charges as appropriate, and please box your answers!
More information5 questions, 3 points each, 15 points total possible. 26 Fe Cu Ni Co Pd Ag Ru 101.
Physical Chemistry II Lab CHEM 4644 spring 2017 final exam KEY 5 questions, 3 points each, 15 points total possible h = 6.626 10-34 J s c = 3.00 10 8 m/s 1 GHz = 10 9 s -1. B= h 8π 2 I ν= 1 2 π k μ 6 P
More informationThis paper should be understood as an extended version of a talk given at the
This paper should be understood as an extended version of a talk given at the Abstract: 1 st JINA workshop at Gull Lake, 2002. Recent experimental developments at LANL (Los Alamos, NM, USA) and CERN (Geneva,
More information-"l" also contributes ENERGY. Higher values for "l" mean the electron has higher energy.
170 - Giving the four parameters will uniquely identify an electron around an atom. No two electrons in the same atom can share all four. These parameters are called QUANTUM NUMBERS. PRINCIPAL QUANTUM
More information? Physics with many Positrons
Varenna Summer School July 2009? Physics with many Positrons Positron Sources & Positron Beams Christoph Hugenschmidt Technische Universität München What is many? Galaxy: 1.5 10 43 e + /s! = 1 lake + 1
More information- Atomic line spectra are UNIQUE to each element. They're like atomic "fingerprints".
- Atomic line spectra are UNIQUE to each element. They're like atomic "fingerprints". - Problem was that the current model of the atom completely failed to explain why atoms emitted these lines. An orbit
More informationA. Aleksanyan, S. Amirkhanyan, H. Gulkanyan*, T. Kotanjyan, L. Poghosyan, V. Pogosov
Armenian Journal of Physics, 2015, vol. 8, issue 3, pp. 102-111 SEARCHING FOR LONG-LIVING RARE PRODUCTS OF THE 252 Cf SPONTANEOUS FISSION A. Aleksanyan, S. Amirkhanyan, H. Gulkanyan*, T. Kotanjyan, L.
More informationThe Shape of the Full-Energy Gamma Ray Peak in Germanium Detectors for Different Energies and Incident Geometries
The Shape of the Full-Energy Gamma Ray Peak in Germanium Detectors for Different Energies and Incident Geometries Ronald M. Keyser ORTEC 801 South Illinois Avenue Oak Ridge, TN 37831 Abstract The accurate
More informationNeutron Activation of 76Ge
Neutron Activation of 76Ge Georg Meierhofer people involved: P. Grabmayr J. Jochum Kepler Center for Astro and Particle Physics University Tübingen P. Kudejova L. Canella J. Jolie IKP, Universität zu Köln
More informationCHEMICAL COMPOUNDS MOLECULAR COMPOUNDS
48 CHEMICAL COMPOUNDS - Dalton's theory does not mention this, but there is more than one way for atoms to come together to make chemical compounds! - There are TWO common kinds of chemical compound, classified
More informationPARAMETERISATION OF FISSION NEUTRON SPECTRA (TRIGA REACTOR) FOR NEUTRON ACTIVATION WITHOUT THE USED OF STANDARD
Parameterisation of Fission Neutron Spectra (TRIGA Reactor) 81 7 PARAMETERISATION OF FISSION NEUTRON SPECTRA (TRIGA REACTOR) FOR NEUTRON ACTIVATION WITHOUT THE USED OF STANDARD Liew Hwi Fen Noorddin Ibrahim
More informationExperimental Studies on the Self-Shielding Effect in Fissile Fuel Breeding Measurement in Thorium Oxide Pellets Irradiated with 14 MeV Neutrons
Plasma Science and Technology, Vol.5, No.2, Feb. 20 Experimental Studies on the Self-Shielding Effect in Fissile Fuel Breeding Measurement in Thorium Oxide Pellets Irradiated with 4 MeV Neutrons Mitul
More informationCourse theme. Three hours of lab Complete E1 (Parts 1, 2, 3, 4, and 5B) Prepare discussion presentation Prepare team report.
Experiment Session 2 Electrons and Solution Color Three hours of lab Complete E (Parts, 2, 3, 4, and 5B) Prepare discussion presentation Prepare team report. Course theme There are structure and property
More informationThree hours of lab Complete E1 (Parts 1, 2, 3, 4, and 5B) Prepare discussion presentation Prepare team report. Course theme
Experiment 1 Session 2 Electrons and Solution Color Three hours of lab Complete E1 (Parts 1, 2, 3, 4, and 5B) Prepare discussion presentation Prepare team report. Course theme There are structure and property
More informationTurkey s first photonuclear reactions performed at Akdeniz University: Matter, Anti-matter, Pure Energy and Alchemy
(Ülkemizin ilk fotonükleer reaksiyonu Akdeniz Üniversitesinde gerçekleştirildi: Madde, Anti-Madde, Saf Enerji ve Simya) Turkey s first photonuclear reactions performed at Akdeniz University: Matter, Anti-matter,
More informationEssential Chemistry for Biology
1 Chapter 2 Essential Chemistry for Biology Biology and Society: More Precious than Gold A drought is a period of abnormally dry weather that changes the environment and one of the most devastating disasters.
More informationIAEA-SM-367/10/04/P SCREENING AND RADIOMETRIC MEASUREMENT OF ENVIRONMENTAL SWIPE SAMPLES
IAEA-SM-367/10/04/P SCREENING AND RADIOMETRIC MEASUREMENT OF ENVIRONMENTAL SWIPE SAMPLES V. MAIOROV, A. CIURAPINSKI, W. RAAB and V. JANSTA Safeguards Analytical Laboratory, International Atomic Energy
More informationThe Generalized Centroid Difference Method
15th International Symposium on Capture Gamma ray Spectroscopy and Related Topics (CGS15) 26.08.2014, Technische Universität Dresden The Generalized Centroid Difference Method for lifetime measurements
More informationBertram Blank CEN Bordeaux-Gradignan. Germanium detector calibration experimental studies: b decay mirror b decay future work
Bertram Blank CEN Bordeaux-Gradignan Germanium detector calibration experimental studies: 0 + - 0 + b decay mirror b decay future work Beta-Decay Weak Interaction Studies in the Era of the LHC International
More informationInvestigation of dipole strength at the ELBE accelerator in Dresden-Rossendorf
EPJ Web of Conferences 21, 04006 (2012) DOI: 10.1051/ epjconf/ 20122104006 C Owned by the authors, published by EDP Sciences, 2012 Investigation of dipole strength at the ELE accelerator in Dresden-Rossendorf
More informationPutting it together... - In the early 20th century, there was a debate on the structure of the atom. Thin gold foil
36 Putting it together... - In the early 20th century, there was a debate on the structure of the atom. RUTHERFORD EXPERIMENT Where do the particles go? Radioactive material A few bounce back A few particles
More informationGamma-neutron competition above the neutron separation energy in betadelayed
Gamma-neutron competition above the neutron separation energy in betadelayed neutron emitters Alejandro Algora IFIC (CSIC-Univ. Valencia), Spain DISCLAIMER: 1. We are only users of Level Densities and
More informationLast 4 Digits of USC ID:
Chemistry 05 B Practice Exam Dr. Jessica Parr First Letter of last Name PLEASE PRINT YOUR NAME IN BLOCK LETTERS Name: Last 4 Digits of USC ID: Lab TA s Name: Question Points Score Grader 8 2 4 3 9 4 0
More informationName: SCH3U Worksheet-Trends
PERIODIC TRENDS WORKSHEET 1. Choose which statement about the alkali metals lithium and cesium is correct. a) as the atomic number increases, the Electronegativity of the elements increases b) as the atomic
More informationNAME (please print) MIDTERM EXAM FIRST LAST JULY 13, 2011
CEMISTRY 140A NAME (please print) MIDTERM EXAM IRST LAST JULY 13, 2011 SIGNATURE Vollhardt & Schore 6 th Edition Cp. 1 through 5 ID NUMBER LAST NAME PERSN SEATED IN T YUR RIGT: LAST NAME PERSN SEATED T
More informationNeutron-induced reaction cross sections measured at. Triangle Universities Nuclear Laboratory. John Kelley
Neutron-induced reaction cross sections measured at Triangle Universities Nuclear Laboratory John Kelley North Carolina State University and Triangle Universities Nuclear Laboratory Supported in part by
More informationReporting Category 1: Matter and Energy
Name: Science Teacher: Reporting Category 1: Matter and Energy Atoms Fill in the missing information to summarize what you know about atomic structure. Name of Subatomic Particle Location within the Atom
More informationCHEMICAL COMPOUNDS MOLECULAR COMPOUNDS
48 CHEMICAL COMPOUNDS - Dalton's theory does not mention this, but there is more than one way for atoms to come together to make chemical compounds! - There are TWO common kinds of chemical compound, classified
More informationIntroduction to X-ray Photoelectron Spectroscopy (XPS) XPS which makes use of the photoelectric effect, was developed in the mid-1960
Introduction to X-ray Photoelectron Spectroscopy (XPS) X-ray Photoelectron Spectroscopy (XPS), also known as Electron Spectroscopy for Chemical Analysis (ESCA) is a widely used technique to investigate
More informationMass Yield Distribution in the Photon-induced Fission of 232 Th, 238 U, nat Pb, and 209 Bi
Mass Yield Distribution in the Photon-induced Fission of 232 Th, 238 U, nat Pb, and 209 Bi H. Naik 1, G.N. Kim 2*, V.T. Nimje 3, K.C. Mittal 3, M.W. Lee 2, K. Kim 2, A. Goswami 1, M.-H. Cho 4 1 Radiochemistry
More informationLaser Spectroscopy on Bunched Radioactive Ion Beams
Laser Spectroscopy on Bunched Radioactive Ion Beams Jon Billowes University of Manchester Balkan School on Nuclear Physics, Bodrum 2004 Lecture 1. 1.1 Nuclear moments 1.2 Hyperfine interaction in free
More informationCHEMICAL COMPOUNDS MOLECULAR COMPOUNDS
48 CHEMICAL COMPOUNDS - Dalton's theory does not mention this, but there is more than one way for atoms to come together to make chemical compounds! - There are TWO common kinds of chemical compound, classified
More informationAtomic weight: This is a decimal number, but for radioactive elements it is replaced with a number in parenthesis.
47 Blocks on the periodic table 11 Sodium 22.99 Atomic number: This is always a whole number. The periodic table is arranged by atomic number! Element symbol: A one or two letter abbreviation for the name
More information-"l" also contributes ENERGY. Higher values for "l" mean the electron has higher energy.
175 - Giving the four parameters will uniquely identify an electron around an atom. No two electrons in the same atom can share all four. These parameters are called QUANTUM NUMBERS. PRINCIPAL QUANTUM
More informationHANDOUT SET GENERAL CHEMISTRY II
HANDOUT SET GENERAL CHEMISTRY II Periodic Table of the Elements 1 2 3 4 5 6 7 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 IA VIIIA 1 2 H He 1.00794 IIA IIIA IVA VA VIA VIIA 4.00262 3 Li 6.941 11 Na 22.9898
More informationWM2014 Conference, March 2 6, 2014, Phoenix, Arizona, USA
Experimental Comparison between High Purity Germanium and Scintillator Detectors for Determining Burnup, Cooling Time and Decay Heat of Used Nuclear Fuel - 14488 Peter Jansson *, Sophie Grape *, Stephen
More informationExperiment to validate EAF activation data: Activation on CuCrZr in NPI d-be neutron field
Nuclear Physics Institute Řež Report NPI ASCR Řež EXP(EFDA)-03/00 Experiment to validate EAF activation data: Activation on CuCrZr in NPI d-be neutron field P. Bém, V. Burjan, M. Götz, M. Honusek, J. Hep
More informationGuide to the Extended Step-Pyramid Periodic Table
Guide to the Extended Step-Pyramid Periodic Table William B. Jensen Department of Chemistry University of Cincinnati Cincinnati, OH 452201-0172 The extended step-pyramid table recognizes that elements
More information