Materials Science. Hand axes like this one found in the United Arab Emirates indicate humans left Africa 125,000 years ago.
|
|
- Harold Hicks
- 5 years ago
- Views:
Transcription
1
2 Summary Materials Science Ion Beam Analysis 3 MV Tandetron TM Accelerator Rutherford Backscattering Spectrometry (RBS) Elastic Recoil Detection (ERD) Nuclear Reaction Analysis (NRA) Ion implant/channeling Conclusion 2
3 Materials Science Hand axes like this one found in the United Arab Emirates indicate humans left Africa 125,000 years ago. Science/AAAS Dacian Koson 2000 years ago. Anti-reflecting coatings MgF2 3
4 Applications of thin films 4
5 5
6 6
7 Material fabrication New technology Characterization (amongst them IBA) Emerging New material Tuning/adjusting deposition parameters 7
8 Let s go inside the lab! 8
9 3 MV IFIN-HH 9
10 Goniometer from IBA chamber 10
11 11
12 RBS Thin films: ZnO, InN, WCN CarbonNanoWalls, TiO 2 Solar cells WS 2 Glasses of Te Thicknesses: from 0.5 nm up to 2 microns 12
13 Elemental analysis technique where alpha particles are scattered off of targets and is used to determine elemental composition and thin-film thickness. 13
14 RBS measurements Tribological samples of WCN/TiB/TiN deposited on Si Produced in IFIN-HH (dr. A. &G. Mateescu) Applications: hard coatings, space applications Information needed : thickness and stoichiometry (atomic composition) 14
15 Analysis sample no. 32 WCN/TiB 2 /TiN SEM cross section RBS spectrum WCN/TiB/TiN x6 layers 15
16 Elastic Recoil Detection 16
17 ERD of a DLC sample containing 30% H Energy [kev] R2_DLCERD.rbs Simulated Counts Channel Experimental conditions: He 2+ ions, 2.5 MeV, Mylar foil in front of the RBS mobile detector (11 μm) Thickness of 6590 at/cm 2, (510 nm 17 ), 1.4 g/cm 3
18 H measurement in CNWs 30% H in DLC substrate Carbon Nanowalls 12%-5% H in CNW sample 18
19 Nuclear Reaction Analysis 19
20 NRA of TiH MeV MeV gamma rays
21 Ion implantation experiments Protons: 1e13-1e15 atoms/cm 2 Helium: 1e13-1e15 atoms/cm 2 Niobium: 6e14 2e15 atoms/cm 2 Silver: 2e15 atoms/cm 2 Gold:1e15 atoms/cm 2 Silicon: 1e16 atoms/cm 2 Iron: 1e16 atoms/cm 2 21
22 Ion channeling on a monocrystaline silicon sample The minimum yield 2.5%. This value shows that the sample is of very good crystallinity. 22
23 Effects of Au ion 1.5 MeV on polymeric nanocomposites 23
24 BEFORE AFTER Increase of hardness: 0.63 GPa before Au + implantation and 1.88 after. 24
25 C12+C13 reaction experiment Collaborators from China: prof. X. Tang group Investigating C-13+C-12 Reaction by the Activation Method. Sensitivity Tests D. Chesneanu, L. Trache, R. Margineanu, A. Pantelica, D. Ghita, M. Straticiuc, I. Burducea, A. M. 25 Blebea-Apostu, C. M. Gomoiu and X. Tang, AIP Conf. Proc, vol. 1645, 311 (2015)
26 Are we there yet? Fusion cross section of 12 C+ 13 C at sub-barrier energies N.T. Zhang, X.D. Tang, H. Chen, D. Chesneanu, M. Straticiuc, L. Trache, I. Burducea, K.A. Li, Y.J. Li, D.G. Ghita, R. Margineanu, A. Pantelica and C. Gomoiu Published online: 12 February DOI:
27 CONCLUSION IBA methods offer valuable information for materials fabricants in order to improve and adjust their deposition methods which could lead to new materials and technologies Apply for beamtime: PAC meeting 27
28 References 1.Compositional, morphological and mechanical investigations of monolayer type coatings obtained by standard and reactive magnetron sputtering from Ti, TiB2 and WC V. Jinga, A. O. Mateescu, D. Cristea, G. Mateescu, I. Burducea, C. Ionescu, L. S. Craciun, I. Ghiuta, C. Samoila, D. Ursutiu, D. Munteanu Applied Surface Science 358 (2015) doi: /j.apsusc , Morphological and compositional investigations of the tribological coatings with quaternary & pentanary composition, obtained from WC, TiB2 and Ti by DC standard & reactive magnetron sputtering A. O. Mateescu, G. Mateescu, L. S. Craciun, C. Ionescu, I. Burducea Journal of Optoelectronics and Advances Materials, Vol. 17, No , November December 2015, p I. Burducea et al. / Nuclear Instruments and Methods in Physics Research B 359 (2015)
29 Thank you for your attention! 29
Práctica de laboratorio número 6: Non-Rutherford scattering near the MeV 12 C(p,p) 12 C resonance
Práctica de laboratorio número 6: Non-Rutherford scattering near the 1.734 MeV 12 C(p,p) 12 C resonance 1) Scope In this experiment, the yield of protons backscattered from a thin gold foil deposited over
More informationIN THE NAME OF ALLAH, THE MOST MERCIFUL AND COMPASSIONATE
IN THE NAME OF ALLAH, THE MOST MERCIFUL AND COMPASSIONATE Ion Beam Analysis of Diamond Thin Films Sobia Allah Rakha Experimental Physics Labs 04-03-2010 Outline Diamond Nanostructures Deposition of Diamond
More informationThe Configuration of the Atom: Rutherford s Model
CHAPTR 2 The Configuration of the Atom: Rutherford s Model Problem 2.2. (a) When α particles with kinetic energy of 5.00 MeV are scattered at 90 by gold nuclei, what is the impact parameter? (b) If the
More informationAPPLICATION OF THE NUCLEAR REACTION ANALYSIS FOR AGING INVESTIGATIONS
1 APPLICATION OF THE NUCLEAR REACTION ANALYSIS FOR AGING INVESTIGATIONS G.Gavrilov, A.Krivchitch, V.Lebedev PETERSBURG NUCLEAR PHYSICS INSTITUTE E-mail: lebedev@pnpi.spb.ru kriv@rec03.pnpi.spb.ru We used
More informationSilver Thin Film Characterization
Silver Thin Film Characterization.1 Introduction Thin films of Ag layered structures, typically less than a micron in thickness, are tailored to achieve desired functional properties. Typical characterization
More informationAu-Ti THIN FILMS DEPOSITED ON GaAs
Au-Ti THIN FILMS DEPOSITED ON GaAs R. V. GHITA *, D. PANTELICA**, M. F. LAZARESCU *, A. S. MANEA *, C. LOGOFATU *, C. NEGRILA *, V. CIUPINA *** * National Institute of Material Physics, P.O. Box MG7, Mãgurele,
More informationRutherford Backscattering Spectrometry
Rutherford Backscattering Spectrometry EMSE-515 Fall 2005 F. Ernst 1 Bohr s Model of an Atom existence of central core established by single collision, large-angle scattering of alpha particles ( 4 He
More informationaccelerating opportunities
accelerating opportunities 9 MV Pelletron FN Tandem Accelerator for basic and applied research The 9MV Tandem Accelerator has been built by the High Voltage Engineering Corporation (HVEC) in 1973 and it
More informationMS482 Materials Characterization ( 재료분석 ) Lecture Note 5: RBS
2016 Fall Semester MS482 Materials Characterization ( 재료분석 ) Lecture Note 5: RBS Byungha Shin Dept. of MSE, KAIST 1 Course Information Syllabus 1. Overview of various characterization techniques (1 lecture)
More informationMS482 Materials Characterization ( 재료분석 ) Lecture Note 5: RBS. Byungha Shin Dept. of MSE, KAIST
2015 Fall Semester MS482 Materials Characterization ( 재료분석 ) Lecture Note 5: RBS Byungha Shin Dept. of MSE, KAIST 1 Course Information Syllabus 1. Overview of various characterization techniques (1 lecture)
More informationRutherford Backscattering Spectrometry
Rutherford Backscattering Spectrometry Timothy P. Spila, Ph.D. Frederick Seitz Materials Research Laboratory University of Illinois at Urbana-Champaign 214University of Illinois Board of Trustees. All
More informationJoint ICTP-IAEA Workshop on Nuclear Data for Analytical Applications October 2013
2495-03 Joint ICTP-IAEA Workshop on Nuclear Data for Analytical Applications 21-25 October 2013 Ion Beam Analysis Techniques for non-destructive Profiling Studies M. Kokkoris Department of Physics National
More informationLecture 22 Ion Beam Techniques
Lecture 22 Ion Beam Techniques Schroder: Chapter 11.3 1/44 Announcements Homework 6/6: Will be online on later today. Due Wednesday June 6th at 10:00am. I will return it at the final exam (14 th June).
More informationP627/Chem 542 Surface/Interface Science Spring 2013 Rutherford Backscattering Lab: Answers to Questions
Intro Questions: 1) How is a tandem ion accelerator different from a so-called van der Graaf accelerator, and what are some of the advantages (and drawbacks) of the tandem design? A tandem ion accelerator
More informationAtomic Collisions and Backscattering Spectrometry
2 Atomic Collisions and Backscattering Spectrometry 2.1 Introduction The model of the atom is that of a cloud of electrons surrounding a positively charged central core the nucleus that contains Z protons
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 informationRITU and the GREAT Spectrometer
RITU and the GREAT Spectrometer Cath Scholey Department of Physics University of Jyväskylä 19 th March 2006 3rd TASCA Detector Group Meeting, GSI Darmstadt C. Scholey (JYFL, Finland) RITU and the GREAT
More informationAP 5301/8301 Instrumental Methods of Analysis and Laboratory Lecture 11 Ion Beam Analysis
1 AP 5301/8301 Instrumental Methods of Analysis and Laboratory Lecture 11 Ion Beam Analysis Prof YU Kin Man E-mail: kinmanyu@cityu.edu.hk Tel: 344-7813 Office: P64 Lecture 8: outline Introduction o Ion
More informationRBS analyses of the composition and structure of thin films synthesized using the pulsed laser deposition technique
RBS analyses of the composition and structure of thin films synthesized using the pulsed laser deposition technique V. Craciun 1, E. Axente 1, G. Socol 1, D. Craciun 1, G. Dorcioman 1, P. Garoi 1, N. Stefan
More informationECE Semiconductor Device and Material Characterization
ECE 4813 Semiconductor Device and Material Characterization Dr. Alan Doolittle School of Electrical and Computer Engineering Georgia Institute of Technology As with all of these lecture slides, I am indebted
More informationStudies on 3D Fusion Reactions in TiDx under Ion Beam Implantation
Takahashi, A. Studies on 3D Fusion Reactions in TiDx under Ion Beam Implantation. in Tenth International Conference on Cold Fusion. 2003. Cambridge, MA: LENR-CANR.org. This paper was presented at the 10th
More informationMS482 Materials Characterization ( 재료분석 ) Lecture Note 12: Summary. Byungha Shin Dept. of MSE, KAIST
2015 Fall Semester MS482 Materials Characterization ( 재료분석 ) Lecture Note 12: Summary Byungha Shin Dept. of MSE, KAIST 1 Course Information Syllabus 1. Overview of various characterization techniques (1
More informationSurface analysis techniques
Experimental methods in physics Surface analysis techniques 3. Ion probes Elemental and molecular analysis Jean-Marc Bonard Academic year 10-11 3. Elemental and molecular analysis 3.1.!Secondary ion mass
More informationPreliminary results of the indirect study of the 12 C( 12 C,α) 20 Ne reaction via the THM applied to the 16 O( 12 C,α 20 Ne )α reaction
Preliminary results of the indirect study of the 12 C( 12 C,α) 20 Ne reaction via the THM applied to the 16 O( 12 C,α 20 Ne )α reaction G.G. Rapisarda, 1,2,6 C. Spitaleri, 1,2 C. Bordeanu, 3 Z. Hons, 4
More informationNuclear Reaction Analysis (NRA)
Nuclear Reaction Analysis (NRA) M. Mayer Max-Planck-Institut für Plasmaphysik, EURATOM Association, Garching, Germany Lectures given at the Workshop on Nuclear Data for Science and Technology: Materials
More informationInstitute of Physics & Power Engineering Current Status of the Problem of Cross Section Data for Ion Beam Analysis
Institute of Physics & Power Engineering Current Status of the Problem of Cross Section Data for Ion Beam Analysis A.F. Gurbich IBA Methods Acronym PIXE PIGE RBS NRA NRP or r-nra ERDA or FRS Particle-Induced
More informationOBSERVATION OF SURFACE DISTRIBUTION OF PRODUCTS BY X-RAY FLUORESCENCE SPECTROMETRY DURING D 2 GAS PERMEATION THROUGH PD COMPLEXES
Iwamura, Y., et al. Observation Of Surface Distribution Of Products By X-Ray Fluorescence Spectrometry During D2 Gas Permeation Through Pd Complexes. in The 12th International Conference on Condensed Matter
More informationImaging Methods: Scanning Force Microscopy (SFM / AFM)
Imaging Methods: Scanning Force Microscopy (SFM / AFM) The atomic force microscope (AFM) probes the surface of a sample with a sharp tip, a couple of microns long and often less than 100 Å in diameter.
More informationToF-SIMS or XPS? Xinqi Chen Keck-II
ToF-SIMS or XPS? Xinqi Chen Keck-II 1 Time of Flight Secondary Ion Mass Spectrometry (ToF-SIMS) Not ToF MS (laser, solution) X-ray Photoelectron Spectroscopy (XPS) 2 3 Modes of SIMS 4 Secondary Ion Sputtering
More informationOut of vacuum characterisation of surfaces: a possible approach?
Out of vacuum characterisation of surfaces: a possible approach? Lorenzo Giuntini Dipartimento di Fisica dell Università and Sezione INFN Firenze, Italy XVIII Congresso Nazionale sulla Scienza e Tecnologia
More informationProgress on Transmutation Experiments induced by D 2 gas permeation
12th International Workshop on Anomalies in Hydrogen Loaded Metals Progress on Transmutation Experiments induced by D 2 gas permeation T.Itoh 1,2, J. Kasagi 1, Y.Iwamura 1, S.Tsuruga 3 1 Condensed Matter
More informationSoft X-ray multilayer mirrors by ion assisted sputter deposition
Soft X-ray multilayer mirrors by ion assisted sputter deposition Valentino Rigato INFN Laboratori Nazionali di Legnaro Bologna, September 21, 2010 Source: INFN-LNL-2009 V. RIGATO 1 SIF- Bologna September
More informationState the main interaction when an alpha particle is scattered by a gold nucleus
Q1.(a) Scattering experiments are used to investigate the nuclei of gold atoms. In one experiment, alpha particles, all of the same energy (monoenergetic), are incident on a foil made from a single isotope
More informationDepth profiles of helium and hydrogen in tungsten nano-tendril surface morphology using Elastic Recoil Detection
PSFC/JA-12-82 Depth profiles of helium and hydrogen in tungsten nano-tendril surface morphology using Elastic Recoil Detection K.B. Woller, D.G. Whyte, G.M. Wright, R.P. Doerner*, G. de Temmerman** * Center
More informationPhysics 100 PIXE F06
Introduction: Ion Target Interaction Elastic Atomic Collisions Very low energies, typically below a few kev Surface composition and structure Ion Scattering spectrometry (ISS) Inelastic Atomic Collisions
More informationStopping power for MeV 12 C ions in solids
Nuclear Instruments and Methods in Physics Research B 35 (998) 69±74 Stopping power for MeV C ions in solids Zheng Tao, Lu Xiting *, Zhai Yongjun, Xia Zonghuang, Shen Dingyu, Wang Xuemei, Zhao Qiang Department
More informationANALYSIS OF PLASMA FACING MATERIALS IN CONTROLLED FUSION DEVICES. Marek Rubel
ANALYSIS OF PLASMA FACING MATERIALS IN CONTROLLED FUSION DEVICES Marek Rubel Alfvén Laboratory, Royal Institute of Technology, Association EURATOM VR, Stockholm, Sweden Acknowledgements Paul Coad and Guy
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 informationSpectroscopy on Mars!
Spectroscopy on Mars! Pathfinder Spirit and Opportunity Real World Friday H2A The Mars Pathfinder: Geological Elemental Analysis On December 4th, 1996, the Mars Pathfinder was launched from earth to begin
More informationInteraction of ion beams with matter
Interaction of ion beams with matter Introduction Nuclear and electronic energy loss Radiation damage process Displacements by nuclear stopping Defects by electronic energy loss Defect-free irradiation
More informationionbeam.kigam.re.kr Beam Application Ion Group
ionbeam.kigam.re.kr Ion Application Group http://ionbeam.kigam.re.kr Project Schedule Major subjects 88 89 9 91 92 93 94 95 96 97 98 99 1 2 3 4 5 6 7 8 9 1 11 Ion Analysis Setup of 1.7MV Tandem VDG Accelerator
More informationDefense Technical Information Center Compilation Part Notice
UNCLASSIFIED Defense Technical Information Center Compilation Part Notice ADPO11561 TITLE: Analysis of a-si02/ a-si Multilayer Structures by Ion Beam Methods and Electron Spin Resonance DISTRIBUTION: Approved
More informationIAP NAN of Ukraine activity in. Possible areas of cooperation in. Roman Kholodov, PICS Meeting, Basivka, Ukraine,
1 IAP NAN of Ukraine activity in field of High Energy Physics. Possible areas of cooperation in frame of PICS and beyond. Institute of Applied Physics National Academy of Sciences of Ukraine 2 The Institute
More informationRBS - Rutherford Backscattering Spectrometry M. Mayer
RBS - Rutherford Backscattering Spectrometry M. Mayer Max-Planck-Institut für Plasmaphysik, EURATOM Association, 85748 Garching, Germany History Scattering geometry and kinematics Rutherford cross section
More information15) Applications of ion sources and examples
15) Applications of ion sources and examples Ion sources are applied in basic science and in industry. In basic science ion sources are used as injectors for heavy ion accelerators. One of the main applications
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 informationFabrication and characterization of porous opaque PMMA foils to be laser irradiated producing ion acceleration
Fabrication and characterization of porous opaque PMMA foils to be laser irradiated producing ion acceleration Mariapompea Cutroneo 1,2*) 1 Nuclear Physics Institute, AS CR, 25068 Rez, Czech Republic 2
More informationPostprint.
http://www.diva-portal.org Postprint This is the accepted version of a paper published in AIP Advances. This paper has been peer-reviewed but does not include the final publisher proof-corrections or journal
More informationAtomic and Nuclear Analytical Methods
H.R. Verma Atomic and Nuclear Analytical Methods XRF, Mössbauer, XPS, NAA and Ion-Beam Spectroscopic Techniques With 128 Figures and 24 Tables Springer Contents 1 X-ray Fluorescence (XRF) and Particle-Induced
More informationFadei Komarov Alexander Kamyshan
Fadei Komarov Alexander Kamyshan Institute of Applied Physics Problems, Belarusian State University, Minsk, Belarus KomarovF@bsu.by Tasks and Objects 2 Introduction and motivation Experimental setup designed
More informationLight element IBA by Elastic Recoil Detection and Nuclear Reaction Analysis R. Heller
Text optional: Institute Prof. Dr. Hans Mousterian www.fzd.de Mitglied der Leibniz-Gemeinschaft Light element IBA by Elastic Recoil Detection and Nuclear Reaction Analysis R. Heller IBA Techniques slide
More informationEE 527 MICROFABRICATION. Lecture 5 Tai-Chang Chen University of Washington
EE 527 MICROFABRICATION Lecture 5 Tai-Chang Chen University of Washington MICROSCOPY AND VISUALIZATION Electron microscope, transmission electron microscope Resolution: atomic imaging Use: lattice spacing.
More informationJoint ICTP/IAEA Workshop on Advanced Simulation and Modelling for Ion Beam Analysis February 2009
015-0 Joint ICTP/IAEA Workshop on Advanced Simulation and Modelling for Ion Beam Analysis 3-7 February 009 Introduction to Ion Beam Analysis: General Physics M. Mayer Max-Planck-Institut fuer Plasmaphysik
More informationElastic Recoil Detection Method using DT Neutrons for Hydrogen Isotope Analysis in Fusion Materials. Abstract
Elastic Recoil Detection Method using DT Neutrons for Hydrogen Isotope Analysis in Fusion Materials Naoyoshi Kubota, Kentaro Ochiai, Keitaro Kondo 2 and Takeo Nishitani. :Japan Atomic Energy Research Institute,
More informationSYSTEM FOR PIXE TRACE ELEMENT ANALYSIS AT MTF. M. Beňo, J. Dobrovodský, D. Vaňa, S. Minárik
SYSTEM FOR PIXE TRACE ELEMENT ANALYSIS AT MTF M. Beňo, J. Dobrovodský, D. Vaňa, S. Minárik Slovak University of Technology in Bratislava, Faculty of Materials Science and Technology in Trnava (MTF), Advanced
More informationThe MIT Nuclear Products Generator for development of ICF diagnostics at Omega / Omega EP and the NIF
Introduction The MIT Nuclear Products Generator for development of ICF diagnostics at Omega / Omega EP and the NIF SBDs d + or 3 He +(2+) D or 3 He target Present MIT Graduate Students and the MIT Nuclear
More informationCHARGED PARTICLE EMISSIONS AND SURFACE MORPHOLOGY OF THE Pd/PdO:Dx AND THE TiDx TARGETS UNDER AN ELECTRON BEAM EXCITATION
Material Characterization Session 10 O_2 CHARGED PARTICLE EMISSIONS AND SURFACE MORPHOLOGY OF THE Pd/PdO:Dx AND THE TiDx TARGETS UNDER AN ELECTRON BEAM EXCITATION Andrei Lipson 1, Ivan Chernov 2, Alexei
More informationMultilayer Interference Coating, Scattering, Diffraction, Reflectivity
Multilayer Interference Coating, Scattering, Diffraction, Reflectivity mλ = 2d sin θ (W/C, T. Nguyen) Normal incidence reflectivity 1..5 1 nm MgF 2 /Al Si C Pt, Au 1 ev 1 ev Wavelength 1 nm 1 nm.1 nm Multilayer
More informationHigh-Resolution Gamma-Ray and Neutron Detectors For Nuclear Spectroscopy
High-Resolution Gamma-Ray and Neutron Detectors For Nuclear Spectroscopy Thomas Niedermayr, I. D. Hau, S. Terracol, T. Miyazaki, S. E. Labov and S. Friedrich Former colleagues: M. F. Cunningham, J. N.
More informationPHY492: Nuclear & Particle Physics. Lecture 3 Homework 1 Nuclear Phenomenology
PHY49: Nuclear & Particle Physics Lecture 3 Homework 1 Nuclear Phenomenology Measuring cross sections in thin targets beam particles/s n beam m T = ρts mass of target n moles = m T A n nuclei = n moles
More informationJoint ICTP/IAEA Workshop on Advanced Simulation and Modelling for Ion Beam Analysis
2015-19 Joint ICTP/IAEA Workshop on Advanced Simulation and Modelling for Ion Beam Analysis 23-27 February 2009 Use of the IBA DataFurnace C. Jeynes University of Surrey Ion Beam Centre U.K. IBA techniques:
More informationV.Storizhko Institute of Applied Physics, National Academy of Sciences of Ukraine
IAP accelerator based facility for simulation and studies of radiation induced defects in materials V.Storizhko Institute of Applied Physics, National Academy of Sciences of Ukraine IAEA Technical Meeting
More informationBenchmark measurements of non-rutherford proton elastic scattering cross section for boron
Published in: Nuclear Instr. Meth. B (01) 0 Benchmark measurements of non-rutherford proton elastic scattering cross section for boron M. Chiari (a), M. Bianconi (b), I. Bogdanović Radović (c), M. Mayer
More informationAccelerator facilities - Ruđer Bošković Institute, Zagreb, Croatia
Accelerator facilities - Ruđer Bošković Institute, Zagreb, Croatia Milko Jaksic, Neven Soic Our capabilities (accelerator, sources, beamlines,...) Research activities (projects, users, int. collaborations,...)
More informationProgramme for Research-Development-Innovation for Space Technology and Advanced Research - STAR
Programme for Research-Development-Innovation for Space Technology and Advanced Research - STAR Dr. Ing. Gheorghe Mateescu Romanian Space Week, 12-16 May 2014, Bucharest, Romania Partner organizations
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 informationDynamic measurement of the helium concentration of evolving tungsten nanostructures using Elastic Recoil Detection during plasma exposure
PSFC/JA-14-38 Dynamic measurement of the helium concentration of evolving tungsten nanostructures using Elastic Recoil Detection during plasma exposure Woller, K.B., Whyte, D.G., Wright, G.M. January,
More informationM. Audronis 1 and F. Zimone 2 1. Nova Fabrica Ltd. 1. Angstrom Sciences Inc.
M. Audronis 1 and F. Zimone 2 1 Nova Fabrica Ltd. 1 Angstrom Sciences Inc. Email: info@novafabrica.biz 1 Founded in 2013 the company is based in Lithuania (northern EU). NF are involved in two business
More informationA Comparison between Channel Selections in Heavy Ion Reactions
Brazilian Journal of Physics, vol. 39, no. 1, March, 2009 55 A Comparison between Channel Selections in Heavy Ion Reactions S. Mohammadi Physics Department, Payame Noor University, Mashad 91735, IRAN (Received
More informationNuclear AstroPhysics at ELI-NP: preliminary experiments with ELISSA detector. Giovanni Luca Guardo
Nuclear AstroPhysics at ELI-NP: preliminary experiments with ELISSA detector Giovanni Luca Guardo ELI-NP facility For the first time, a very high spectral density (10 4 γ/s/ev), brilliant γ beam,
More informationMaterials Analysis Using Fast Ions
A. Denker, W. Bohne, J. Rauschenberg,J. Röhrich, E. Strub Ionenstrahllabor Hahn-Meitner-Institut Berlin Materials Analysis Using Fast Ions Introduction: Energy Loss PIXE Proton Induced X-ray Emission RBS
More informationSome more equations describing reactive magnetron sputtering.
Some more equations describing reactive magnetron sputtering D. Depla, S. Mahieu, W. Leroy, K. Van Aeken, J. Haemers, R. De Gryse www.draft.ugent.be discharge voltage (V) 44 4 36 32 28..5 1. 1.5 S (Pumping
More informationApplication of Ion Beam Analysis Techniques to the Study of Cultural Heritage Objects
Application of Ion Beam Analysis Techniques to the Study of Cultural Heritage Objects Technological and Nuclear Institute - Unit of Physics and Accelerators 1 What is IBA? The IBA (Ion Beam Analysis) techniques
More informationA new detector for neutron beam monitoring
A new detector for neutron beam monitoring European Organization for Nuclear Research (CERN), Geneva, Switzerland in collaboration with Commissariat à l Energie Atomique (CEA), Saclay, France, Instituto
More informationNew irradiation zones at the CERN-PS
Nuclear Instruments and Methods in Physics Research A 426 (1999) 72 77 New irradiation zones at the CERN-PS M. Glaser, L. Durieu, F. Lemeilleur *, M. Tavlet, C. Leroy, P. Roy ROSE/RD48 Collaboration CERN,
More informationThe scanning microbeam PIXE analysis facility at NIRS
Nuclear Instruments and Methods in Physics Research B 210 (2003) 42 47 www.elsevier.com/locate/nimb The scanning microbeam PIXE analysis facility at NIRS Hitoshi Imaseki a, *, Masae Yukawa a, Frank Watt
More informationINTRODUCTION to ION BEAM TECHNIQUES. Marko Karlušić Ruđer Bošković Institute, Zagreb
INTRODUCTION to ION BEAM TECHNIQUES Marko Karlušić Ruđer Bošković Institute, Zagreb INTRODUCTION to ION BEAM ANALYSIS (IBA) Electrostatic accelerators Ion beam analysis with examples RBS ERDA PIXE Nuclear
More informationCharacterization of Secondary Emission Materials for Micro-Channel Plates. S. Jokela, I. Veryovkin, A. Zinovev
Characterization of Secondary Emission Materials for Micro-Channel Plates S. Jokela, I. Veryovkin, A. Zinovev Secondary Electron Yield Testing Technique We have incorporated XPS, UPS, Ar-ion sputtering,
More informationAccreting neutron stars provide a unique environment for nuclear reactions
, Tracy Steinbach, Jon Schmidt, Varinderjit Singh, Sylvie Hudan, Romualdo de Souza, Lagy Baby, Sean Kuvin, Ingo Wiedenhover Accreting neutron stars provide a unique environment for nuclear reactions High
More informationIntroduction to Radiological Sciences Neutron Detectors. Theory of operation. Types of detectors Source calibration Survey for Dose
Introduction to Radiological Sciences Neutron Detectors Neutron counting Theory of operation Slow neutrons Fast neutrons Types of detectors Source calibration Survey for Dose 2 Neutrons, what are they?
More informationin2p , version 1-28 Nov 2008
Author manuscript, published in "Japanese French Symposium - New paradigms in Nuclear Physics, Paris : France (28)" DOI : 1.1142/S21831391444 November 23, 28 21:1 WSPC/INSTRUCTION FILE oliveira International
More informationCharacterization of the 3 MeV Neutron Field for the Monoenergetic Fast Neutron Fluence Standard at the National Metrology Institute of Japan
Characterization of the 3 MeV Neutron Field for the Monoenergetic Fast Neutron Fluence Standard at the National Metrology Institute of Japan Hideki Harano * National Metrology Institute of Japan, National
More informationSupplementary Table 1. Parameters for estimating minimum thermal conductivity in MoS2
Supplementary Table 1. Parameters for estimating minimum thermal conductivity in MoS2 crystal. The three polarizations (TL1 TL2 and TA) are named following the isoenergydecomposition process described
More informationFeasibility Studies for the EXL Project at FAIR *
* a,b,, S. Bagchi c, S. Diebold d, C. Dimopoulou a, P. Egelhof a, V. Eremin e, S. Ilieva a, N. Kalantar-Nayestanaki c, O. Kiselev a,f, T. Kröll f, Y.A. Litvinov a,g, M. Mutterer a, M.A. Najafi c, N. Petridis
More informationLight ion recoil detector
Light ion recoil detector Overall design The detector for light (target-like) particles is a substantial part of the R3B setup. It allows registration of recoils in coincidence with the heavy fragments,
More informationThe MIT Accelerator for development of ICF diagnostics at OMEGA / OMEGA-EP and the NIF
Introduction The MIT Accelerator for development of ICF diagnostics at OMEGA / OMEGA-EP and the NIF SBDs d + or 3 He +(2+) D or 3 He target Present MIT Graduate Students and the MIT Accelerator OLUG 21
More informationHeavy Ion Recoil Spectroscopy of Surface Layers
UNIVERSITY OF HELSINKI REPORT SERIES IN PHYSICS HU-P-D99 Heavy Ion Recoil Spectroscopy of Surface Layers Timo Sajavaara Accelerator Laboratory Department of Physical Sciences Faculty of Science University
More information1 (a) Sketch the electric field surrounding the gold nucleus drawn below. (3)
1 (a) Sketch the electric field surrounding the gold nucleus drawn below. (b) The spreadsheet shown approximately models the behaviour of an alpha particle as it approaches a gold nucleus. The proton number
More informationSecondary ion mass spectrometry (SIMS)
Secondary ion mass spectrometry (SIMS) Lasse Vines 1 Secondary ion mass spectrometry O Zn 10000 O 2 Counts/sec 1000 100 Li Na K Cr ZnO 10 ZnO 2 1 0 20 40 60 80 100 Mass (AMU) 10 21 10 20 Si 07 Ge 0.3 Atomic
More informationRadiation (Particle) Detection and Measurement
Radiation (Particle) Detection and Measurement Radiation detection implies that the radiation interacts (e.g. leaves at least part of its energy) in the material. A specific material is chosen, because
More informationRadioactivity - Radionuclides - Radiation
Content of the lecture Introduction Particle/ion-atom atom interactions - basic processes on on energy loss - stopping power, range Implementation in in Nucleonica TM TM Examples Origin and use of particles
More informationElectron Rutherford Backscattering, a versatile tool for the study of thin films
Electron Rutherford Backscattering, a versatile tool for the study of thin films Maarten Vos Research School of Physics and Engineering Australian National University Canberra Australia Acknowledgements:
More informationCharacteristics of Filtered Neutron Beam Energy Spectra at Dalat Reactor
World Journal of Nuclear Science and Technology, 2014, 4, 96-102 Published Online April 2014 in SciRes. http://www.scirp.org/journal/wjnst http://dx.doi.org/10.4236/wjnst.2014.42015 Characteristics of
More informationCarbon Deposition and Deuterium Inventory in ASDEX Upgrade
1 IAEA-CN-116 / EX / 5-24 Carbon Deposition and Deuterium Inventory in ASDEX Upgrade M. Mayer 1, V. Rohde 1, J. Likonen 2, E. Vainonen-Ahlgren 2, J. Chen 1, X. Gong 1, K. Krieger 1, ASDEX Upgrade Team
More informationSearch for Nuclear Reaction Products in Gas Phase Experiments - Deuterium Permeation and Absorption -
Session 3 O_2 Nuclear Measurements (I) Search for Nuclear Reaction Products in Gas Phase Experiments - Deuterium Permeation and Absorption - A. Kitamura 1, Y. Sasaki 1, Y. Miyoshi 1, Y. Yamaguchi 1, A.
More informationAMS MEASUREMENTS OF DEUTERIUM CAPTURED IN TUNGSTEN LAYERS DEPOSITED BY MAGNETRON SPUTTERING
Romanian Reports in Physics, Vol. 65, No. 4, P. 1258 1264, 2013 AMS MEASUREMENTS OF DEUTERIUM CAPTURED IN TUNGSTEN LAYERS DEPOSITED BY MAGNETRON SPUTTERING A.R. PETRE 1,3, T. ACSENTE 2, M. ENACHESCU 1,
More informationCLUSTER SIZE DEPENDENCE OF SPUTTERING YIELD BY CLUSTER ION BEAM IRRADIATION
CLUSTER SIZE DEPENDENCE OF SPUTTERING YIELD BY CLUSTER ION BEAM IRRADIATION T. Seki 1,2), T. Murase 1), J. Matsuo 1) 1) Quantum Science and Engineering Center, Kyoto University 2) Collaborative Research
More informationQuality Assurance. Purity control. Polycrystalline Ingots
Quality Assurance Purity control Polycrystalline Ingots 1 Gamma Spectrometry Nuclide Identification Detection of Impurity Traces 1.1 Nuclides Notation: Atomic Mass Atomic Number Element Neutron Atomic
More informationAnnax-I. Investigation of multi-nucleon transfer reactions in
Annax-I Investigation of multi-nucleon transfer reactions in 40 Ca on 68,70 Zn at and near the Coulomb barrier. Abstract We will study the multi-nucleon transfer between two medium-heavy nuclei to find
More informationSecondary Ion Mass Spectrometry (SIMS) Thomas Sky
1 Secondary Ion Mass Spectrometry (SIMS) Thomas Sky Depth (µm) 2 Characterization of solar cells 0,0 1E16 1E17 1E18 1E19 1E20 0,2 0,4 0,6 0,8 1,0 1,2 P Concentration (cm -3 ) Characterization Optimization
More information