This talk addresses the use of neutron probe as a tool for Cultural Heritage (CH) research. Thanks to non-destructive nature of the probe this is a
|
|
- Claud Gibson
- 5 years ago
- Views:
Transcription
1 This talk addresses the use of neutron probe as a tool for Cultural Heritage (CH) research. Thanks to non-destructive nature of the probe this is a rapidly growing area of research which complements other techniques. 1
2 Neutron tool provides important piece of information on the science of ancient materials, i.e. in preservation and restoration of artifacts of different composition. Several examples will be addresses: these exploit the penetrating abilities of neutrons to study and visualize the interior properties of objects in totally non destructive and non invasive mode of analysis. 2
3 For example in conservation, to preserve artifacts and objects, it is important to assess their condition in order to develop tailored procedures to prevent deterioration. In this context neutron diffraction help to establish and monitor the condition of an artifact. Concerning making techniques, it has to be stressed that the material characterisation via neutron diffraction of an artifact is important to have insight about the materials and technologies that craftsmen used in ancient times. 3
4 Properties of neutron probe. The application of neutron-based imaging and analysis techniques overcame the limited penetrating power common to other probes. Neutrons can penetrate thick layers of dense materials without substantial scattering or loss of energy. 5
5 Neutrons visualize the interior properties of objects in totally non destructive and non invasive mode of analysis.
6 Neutron Fan showing the development of neutron scattering over the past four decades -- inner ring to outer ring, reading anticlockwise: 1960s Antiferromagnetism - basic physics 7
7 8
8 9
9 10
10 11
11 At X-ray and neutron facilities are available a number of nondestructive analytical techniques that are used in the CH field. In recent years the application of nuclear-based techniques to CH research has also expanded following the installation of laboratories with small ion accelerators close to museums which has facilitated the study of CH objects. 12
12 The history of neutron facilities 13
13 Intense neutron beam can be generated either in a reactor, from a neutron emitting isotope, or from a target in a proton accelerator.
14 Neutron beams
15 16
16 At ISIS neutron beams are generated from a target in a proton accelerator. 17
17 A ion source gun produces proton in the synchrotron. These are then accelerated and sent on a target that produces neutron beam can through a process know as Spallation, literally breaking the nucleus of the target. 18
18 Instrument suite 19
19 The Budapest Nuclear Reactor
20 The FRMII Neutron Reactor
21 Neutron Fluxes 22
22 A comparison of X-ray and neutron cross sections 23
23 Examples of Neutron Based Techniques 24
24 Neutron in Archeometry
25 26
26 27
27 Typical diffraction spectra as normalised number of counts as a function of d-spacing: best fit of data are shown, with the peak position of the different components.
28 Effects on the diffraction patterns: diffraction peak position, peak width and intensities as a function of d-spacing. 29
29
30 Determination of the provenance of the raw materials via neutron diffraction provides information on the identification of the manufacturing processes and the reconstruction of the trade paths of bronze artefacts of various provenance and times 31
31 Texture analysis measures the grain orientation distributions of crystallites in a material. Preferred orientations are visualized in pole figures that display characteristic pole density maxima and minima. This analysis provides information on making technique and whether the material is genuine or fake. The distribution of pole density maxima in the pole figures depends characteristically on the deformation history (e.g. plastic deformation during working; tectonic deformation of geological specimens). 32
32 These texture analysis provideed information on making technique of the coins and to asses whether the material was genuine or fake.
33
34 (Neutron diffraction experiment on INES)
35 The texture and microstucture analysis shows indications of successive hardening-annealinghardening processes.
36 In the ancient period funerary dowry is considered a distinctive characteristic of aristocrats, who also detained military and ritual power. The artefacts objects of this study were found not only in male tombs, suggesting that also women played a primary role in such ritual activities. 40
37 The samples analysed, 14 fragments, were part of a collection that comes from the ancient tombs. 41
38 Typical diffraction spectra as normalised number of counts as a function of d-spacing: best fit of data are shown, with the peak position of the different components; residue is reported in violet. The corrosion products and patinas revealed by the study, like Azurite, Nantokite, etc. depend on chemicalphysical conservation conditions of the particular object (for instance presence of water or absence of air). 42
39 Sample composed of two distinct parts (not coming from the same casting) Covellite is present in objects buried in non oxygenated conditions 43
40 Patina is a smooth and continuous layer that preserves detail and shape. Whereas corrosion describes discontinuous deposits of other environmental materials that determine a chemical attack. Different events such as burial, exposure to the atmosphere, marine conditions, laboratory environment (protection covering or pigments), lead to different corrosion products and patinas. Sequence of optical microscopy to characterise samples 44
41 45
42
43
44
45 The PGAI/NT set up at FRM II. 49
46 The Neutron Resonance Capture Analysis (NRCA) is used to determine the elemental composition of materials and artefacts. In NRCA neutron with energies corresponding to energy levels of the nucleus to be formed after capture are captured preferentially. Interaction of neutrons with nuclei as a function of neutron energy shows sharp peaks, known as resonances, at energies specific for each isotope. Resonances are the fingerprints of elements. They can be visualized in the neutron capture spectrum as a function of neutron energy. 50
47 Each capture event is followed by a number of prompt gamma rays. The energy of a neutron is determined by measuring the time it needs to travel a known distance (L in m). With a pulsed neutron source the time-of-flight (T in μs) can be determined from the start pulse of the source and a stop pulse generated by detection of the prompt capture gamma rays. 51
48 Example of NRCA experiment on brass object at GELINA, Belgium. The energies reveal the isotopes present and the areas the amount of the isotopes.
49
50 The principle of neutron thomography is based on the attenuation, through both diffusion and absorption, of a directional neutron beam by the matter through which it passes. Since different materials vary in their ability to attenuate neutrons, then both composition and structure can be probed. Principle: when beam pass trough a sample, part of the radiation is attenuated by the material related with the absorption coefficient 54
51 Roman sword. The neutron radiograhy is complimentary to X-ray radiography. 55
52 Roman dagger. Whereas X-rays are scattered and absorbed by the electrons, and as such atoms with greater electron shells interact more strongly, neutrons on the other hand interact with the atomic nuclei. 56
53 Neutron tomography: The basic principle behind tomography is that the interior structure of a 3-dimensional (3D) sample can be calculated based on a set of 2-dimensional (2D) projections (also called radiographies) of this sample, taken under different angles. 57
54 Cold neutron Tomography 58
55 Neutron Tomography/Imaging has wide industrial and scientific significance and can provide detailed information concerning the inner structure and composition of objects. The principle of neutron imaging is based on the attenuation, through both diffusion and absorption, of a directional neutron beam by the matter through which it passes. Since different materials vary in their ability to attenuate neutrons, then both composition and structure can be probed. 59
56 An example of combined used of 3 neutron techniques 60
57 61
58 Example of neutron analysis from marble objects from Villa Adriana Tivo Composition resulted from the studies: calcite (CaCO 3 ), dolomite (CaMg(CO 3 ) 2 ), silica (quarzo, plagioclasio, mica), oxides (rutite, magnetite) 63
59 Components: Plagioclasio (Ca 0.85 Na 0.14 Al 1.86 Si 2.14 O 8 ) = % 83.0 in weight Orthoclasio (KSi 3 AlO 8 ) = % 15.5 in weight Quarzo (SiO 2 ) = % 1.5 in in weight 64
60 An Aryballos Greek vase from Etruscan tumb dated VII-VI century A.C. 66
61 The project ANCIENT CHARM exploits the idea of developing an analysis technique based on neutron absorption. This idea is quite innovative in the field of archaeology, with a number of scientific and technical challenges. The project has been established to tap into some of Europe's leading research on neutron-based imaging and to apply it to artefact analysis. Neutrons with energies similar to chemical bonds are used to produce quantitative measures and even 3D images of the elemental composition and physical structure of artefacts. The multidisciplinary ANCIENT CHARM team includes neutron beam facilities, detector manufacturers, software engi-neers, physicists and representatives fromthe fields of archeology and cultural heritage. The aim of ANCIENT CHARM is to develop innovative neutron-imaging techniques and the associated equipment, and help establish neutron imaging as a mainstream archaeological analytical technique. In particular, the aim is to develop a neutron resonant capture imaging combined with neutron resonance transmission (NRCI/NRT). Both gamma-emission and neutron transmission measurements will be used to determine the elemental composition of an object in 3D. One of the key developments in the project has been the construction of a new equipment for 3D analysis of small objects, to be used at the ISIS spallation neutron sources. The equipment is now available at the ISIS spallation source and is used for experiments on test objects and on selected archaeological samples. 67
62 Neutrons that are either scattered or absorbed in the sample are removed from the incident beam. Bulk element concentrations can be determined by neutron resonance transmission (NRT) by placing an entire object in a neutron beam without any sample preparation. Transmitted neutrons are registered in the NRT detector while the gamma-rays emitted after neutron capture are recorded by the NRCA detector array. 69
63 Example
64 73
65 Black boxes are manifactured by archeaologists and then given to researcher. The archeaologists are the only one to know the material inside and how they are arranged. Combined use or radiography, tomography and diffraction allow to reconstruct what is inside.
66 75
67 76
68
69 The Baptistery, San Giovanni in Florence 78
70 79
71 1. The advanced deterioration state of the mercury-amalgam gilded sculptures suggested specific strategies for urgent restoration, especially addressing suitable cleaning treatments. 2. The gilding is also covered by encrustations due to a mixture of corrosion products and deposits (gypsum, quarts, feldspars, carbon, etc.) as a result of the interaction with the outdoor environment. 3. As a consequence oxide and salt layers constitute the current bed of the gold layer, requiring special attention from a restoration point of view. 80
72 81
73 82
74 83
75 84
76 85
77 86
78 Results of the analysis did not show any chlorine in the areas treated with chemical agents. Chlorine was instead detected in area treated with laser ablation. Copper Chlorine is a dangerous compound for the gilding since it forms excrescences. 87
79 Radiography with cold neutron showed the presence of an hole or of a material with less neutron absorption material. 88
80 89
81 90
82 Laser-scan of the samples and definition of the measurement points for the Ghiberti Heads mounted on the ENGIN-X diffractometer at the ISIS neutron source. 91
83 92
84 93
85 94
86 The different shapes of the peaks observed in the measurements are due to working processes: this is the proof that Ghiberti made a rifusion of one of the head. 95
87 96
88 97
89 98
90 99
91 101
92 Results from a Neutron Resonance Imaging experiment 103
93 Results from a Neutron Resonance Imaging experiment 104
94 105
95 107
96 Progetto per l'applicazione dei Neutroni Alla Ricerca in Elettronica e Archeometria is financed by CNR within the Agreement concerning collaboration in scientific research at the spallation neutron source ISIS signed between CNR and the STFC (Science Technology Facility Council). The project team, an Italian-British collaboration, aims, by 2014, to deliver at ISIS two instruments : IMAT, a Neutron Imaging diffractometer and CHIPIR, an instrument for Chip Irradiation. 108
97
98 110
99 Criteria for Research Infrastructure within FP7 111
100 112
101 113
102 114
103 115
Neutron Imaging at Spallation Neutron Sources
Neutron Imaging at Spallation Neutron Sources E.H. LEHMANN, A. KAESTNER Paul Scherrer Institut, Deptm. Spallation Neutron Source, Switzerland OUTLINE 1. Introduction: Motivation for Neutron Imaging 2.
More informationAn introduction to Neutron Resonance Densitometry (Short Summary)
An introduction to Neutron Resonance Densitometry (Short Summary) H. Harada 1, M. Koizumi 1, H. Tsuchiya 1, F. Kitatani 1, M. Seya 1 B. Becker 2, J. Heyse 2, S. Kopecky 2, C. Paradela 2, P. Schillebeeckx
More informationThere are five main methods whereby an unstable isotope can gain stability by losing energy. These are:
10. RADIOACTIVITY LOGGING 10.1 Introduction Radioactivity is used in several different types of logging tool. There are those that measure the natural radiation generated by the formation, such as the
More informationNeutron-resonance capture as a tool to analyse the internal compositions of objects non-destructively
Neutron-resonance capture as a tool to analyse the internal compositions of objects non-destructively H. Postma, Delft University of Technology, Mekelweg 15, 2629 JB Delft, the Netherlands P. Schillebeeckx,
More informationChapter 3: Neutron Activation and Isotope Analysis
Chapter 3: Neutron Activation and Isotope Analysis 3.1. Neutron Activation Techniques 3.2. Neutron Activation of Paintings 3.3. From Qumran to Napoleon 3.4. Neutron Activation with Accelerators 3.5. Isotope
More informationActivation Analysis. Characteristic decay mechanisms, α, β, γ Activity A reveals the abundance N:
2.5. Isotope analysis and neutron activation techniques The previously discussed techniques of material analysis are mainly based on the characteristic atomic structure of the elements and the associated
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 informationNeutron facilities and generation. Rob McQueeney, Ames Laboratory and Iowa State University
Neutron facilities and generation Rob McQueeney, Ames Laboratory and Iowa State University September 12, 2018 19-Sep-18 Physics 502 2 Neutrons compared to other probes of matter Bulk probe Interacts with
More informationUsing neutron resonances for non-destructive material analysis: the ANCIENT CHARM project
Using neutron resonances for non-destructive material analysis: the ANCIENT CHARM project Enrico Perelli Cippo and the ANCIENT CHARM Collaboration Departement of physics Giuseppe Occhialini, University
More information2. Which of the following statements help(s) to explain why gas can fill the vessel containing it completely while liquid cannot?
Name: Class: ( ) There are 30 questions. Time Allowed: 45 min 1. Kinetic theory explains the behaviour of a substance in terms of the behaviour of the molecules in it. Which of the following is/are the
More informationDelft in Europe. Neutron & Positrons Oyster & the World
Delft in Europe Neutron & Positrons Oyster & the World where are we? Oyster - HOR Neutrons and Positrons European Spallation Source where are we? Oyster - HOR Neutrons and Positrons European Spallation
More informationCHARGED PARTICLE INTERACTIONS
CHARGED PARTICLE INTERACTIONS Background Charged Particles Heavy charged particles Charged particles with Mass > m e α, proton, deuteron, heavy ion (e.g., C +, Fe + ), fission fragment, muon, etc. α is
More informationThe basic structure of an atom is a positively charged nucleus composed of both protons and neutrons surrounded by negatively charged electrons.
4.4 Atomic structure Ionising radiation is hazardous but can be very useful. Although radioactivity was discovered over a century ago, it took many nuclear physicists several decades to understand the
More informationA Proposal of Nuclear Materials Detection and Inspection Systems in Heavily Shielded Suspicious Objects by Non-destructive Manner.
Magic Maggiore Technical Reachback Workshop 15 min. (March 28-30, 2017, JRC Ispra, Italy) A Proposal of Nuclear Materials Detection and Inspection Systems in Heavily Shielded Suspicious Objects by Non-destructive
More informationCOMMISSIONING TESTS OF THE NEW NEUTRON RADIOGRAPHY FACILITY AT THE LVR-15 REACTOR ABSTRACT
COMMISSIONING TESTS OF THE NEW NEUTRON RADIOGRAPHY FACILITY AT THE LVR-15 REACTOR J. ŠOLTÉS, L. VIERERBL Neutron Physics Department, Research Centre Rez Ltd., Hlavní 130, 250 68 Husinec-Řež, Czech Republic
More information4.4.1 Atoms and isotopes The structure of an atom Mass number, atomic number and isotopes. Content
4.4 Atomic structure Ionising radiation is hazardous but can be very useful. Although radioactivity was discovered over a century ago, it took many nuclear physicists several decades to understand the
More informationAtomic & Nuclear Physics
Atomic & Nuclear Physics Life and Atoms Every time you breathe you are taking in atoms. Oxygen atoms to be exact. These atoms react with the blood and are carried to every cell in your body for various
More informationV. 3. Development of an Accelerator Beam Loss Monitor Using an Optical Fiber
CYRIC Annual Report 2001 V. 3. Development of an Accelerator Beam Loss Monitor Using an Optical Fiber Kawata N. Baba M. Kato M.*, Miura T.**, and Yamadera A.***, Cyclotron and Radioisotope Center, Tohoku
More informationFlux and neutron spectrum measurements in fast neutron irradiation experiments
Flux and neutron spectrum measurements in fast neutron irradiation experiments G.Gorini WORKSHOP A neutron irradiation facility for space applications Rome, 8th June 2015 OUTLINE ChipIr and SEE: New Istrument
More informationRadionuclide Imaging MII Positron Emission Tomography (PET)
Radionuclide Imaging MII 3073 Positron Emission Tomography (PET) Positron (β + ) emission Positron is an electron with positive charge. Positron-emitting radionuclides are most commonly produced in cyclotron
More informationModern physics ideas are strange! L 36 Modern Physics [2] The Photon Concept. How are x-rays produced? The uncertainty principle
L 36 Modern Physics [2] X-rays & gamma rays How lasers work Medical applications of lasers Applications of high power lasers Medical imaging techniques CAT scans MRI s Modern physics ideas are strange!
More information1. The most important aspects of the quantum theory.
Lecture 5. Radiation and energy. Objectives: 1. The most important aspects of the quantum theory: atom, subatomic particles, atomic number, mass number, atomic mass, isotopes, simplified atomic diagrams,
More informationRad T 290 Worksheet 2
Class: Date: Rad T 290 Worksheet 2 1. Projectile electrons travel from a. anode to cathode. c. target to patient. b. cathode to anode. d. inner shell to outer shell. 2. At the target, the projectile electrons
More informationDesign of an Integrated Inspection System For Detection of Explosive and Illicit Materials
Design of an Integrated Inspection System For Detection of Explosive and Illicit Materials IAEA 2 nd CRP Meeting, Mumbai, 12 16 November 2007 R. M. Megahid Nuclear Research Centre, Atomic Energy Authority
More informationPHYSICS A2 UNIT 2 SECTION 1: RADIOACTIVITY & NUCLEAR ENERGY
PHYSICS A2 UNIT 2 SECTION 1: RADIOACTIVITY & NUCLEAR ENERGY THE ATOMIC NUCLEUS / NUCLEAR RADIUS & DENSITY / PROPERTIES OF NUCLEAR RADIATION / INTENSITY & BACKGROUND RADIATION / EXPONENTIAL LAW OF DECAY
More informationNuclear Cross-Section Measurements at the Manuel Lujan Jr. Neutron Scattering Center
1 Nuclear Cross-Section Measurements at the Manuel Lujan Jr. Neutron Scattering Center M. Mocko 1, G. Muhrer 1, F. Tovesson 1, J. Ullmann 1 1 LANSCE, Los Alamos National Laboratory, Los Alamos NM 87545,
More information5 Atomic Physics. 1 of the isotope remains. 1 minute, 4. Atomic Physics. 1. Radioactivity 2. The nuclear atom
5 Atomic Physics 1. Radioactivity 2. The nuclear atom 1. In a fission reactor, which particle causes a Uranium-235 nucleus to split? A. alpha-particle B. gamma ray C. neutron D. proton 2. A radioactive
More informationToday, I will present the first of two lectures on neutron interactions.
Today, I will present the first of two lectures on neutron interactions. I first need to acknowledge that these two lectures were based on lectures presented previously in Med Phys I by Dr Howell. 1 Before
More informationCRaTER Science Requirements
CRaTER Science Requirements Lunar Reconnaissance Orbiter CRaTER Preliminary Design Review Justin Kasper (CRaTER Proj. Sci.) Outline Energy deposition Classical ionizing radiation Nuclear fragmentation
More informationBasic physics Questions
Chapter1 Basic physics Questions S. Ilyas 1. Which of the following statements regarding protons are correct? a. They have a negative charge b. They are equal to the number of electrons in a non-ionized
More information10/8/15. Earth Materials Minerals and Rocks. I) Minerals. Minerals. (A) Definition: Topics: -- naturally occurring What are minerals?
minerals Earth Materials Minerals and Rocks I) Minerals Minerals Topics: What are minerals? Basic Chemistry Amethysts in geode: minerals Characteristics of Minerals Types of Minerals -- orderly arrangement
More informationChemistry Instrumental Analysis Lecture 19 Chapter 12. Chem 4631
Chemistry 4631 Instrumental Analysis Lecture 19 Chapter 12 There are three major techniques used for elemental analysis: Optical spectrometry Mass spectrometry X-ray spectrometry X-ray Techniques include:
More informationResearch Physicist Field of Nuclear physics and Detector physics. Developing detector for radiation fields around particle accelerators using:
Christopher Cassell Research Physicist Field of Nuclear physics and Detector physics Developing detector for radiation fields around particle accelerators using: Experimental data Geant4 Monte Carlo Simulations
More informationRadioactive Decay 1 of 20 Boardworks Ltd 2016
Radioactive Decay 1 of 20 Boardworks Ltd 2016 Radioactive Decay 2 of 20 Boardworks Ltd 2016 What is radiation? 3 of 20 Boardworks Ltd 2016 The term radiation (also known as nuclear radiation) refers to
More informationApplications for PIXE and other Ion Beam Analysis (IBA)
Applications for PIXE and other Ion Beam Analysis (IBA) PIXE-PAN Summer Science Program University of Notre Dame June, 2007 Larry Lamm, Research Professor Many, many facilities worldwide Some IBA Techniques
More informationApplied Nuclear Physics at the NUS Physics Department
Applied Nuclear Physics at the NUS Physics Department Thomas Osipowicz, Department of Physics Faculty of Science, NUS A few words on the history of Nuclear Physics Early 20 st century: Various types (,,
More informationRadioactive Decay What is Radioactivity? http://explorecuriocity.org/explore/articleid/3033 http://explorecuriocity.org/explore/articleid/3035 http://explorecuriocity.org/explore/articleid/2160 Quick Review
More informationEXPERIMENT 11: NUCLEAR RADIATION
Introduction: radioactive nuclei. third is electromagnetic radiation. EXPERIMENT 11: NUCLEAR RADIATION In this lab, you will be investigating three types of emissions from Two types of these emissions
More informationPartial 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 informationMINERALS Smith and Pun Chapter 2 ATOMIC STRUCTURE
MINERALS Smith and Pun Chapter 2 1 ATOMIC STRUCTURE 2 1 ATOMIC STRUCTURE (2) (See Smith and Pun, pages 29-35) ELEMENT: Substance that cannot be broken down into other substances by ordinary chemical methods
More informationPolarQuest Detector Construction Days: CERN Cosmic rays and applications: when fundamental Science helps everyday life
PolarQuest Detector Construction Days: CERN 20180522-24 Cosmic rays and applications: when fundamental Science helps everyday life M. Garbini, I. Gnesi courtesy of F. Riggi Cosmic Rays First, what are
More information12th International Congress on the Deterioration and Conservation of Stone Columbia University, New York, 2012
NON-DESTRUCTIVE INVESTIGATIONS OF DIMENSION STONES BY NEAR INFRARED SPECTROSCOPY (NIR) Jörg Bowitz 1, Angela Ehling 2 1 Dr. Bowitz Consulting Berlin 2 Federal Institution for Geosciences and Natural Resources
More informationINTRODUCTION TO MEDICAL PHYSICS 1 Quiz #1 Solutions October 6, 2017
INTRODUCTION TO MEDICAL PHYSICS 1 Quiz #1 Solutions October 6, 2017 This is a closed book examination. Adequate information is provided you to solve all problems. Be sure to show all work, as partial credit
More informationNeutron Log. Introduction
Neutron Log Introduction This summary focuses on the basic interactions between the tool s signal and measured information, that help characterize the formation. It is not intended to be a comprehensive
More informationAnswerIT! Atoms and isotopes. Structure of an atom Mass number, atomic number and isotopes Development of the model of the atom.
AnswerIT! Atoms and isotopes Structure of an atom Mass number, atomic number and isotopes Development of the model of the atom. Atoms and isotopes - AnswerIT 1. The diameter of an atom is about 0.000 000
More informationNuclear cross-section measurements at the Manuel Lujan Jr. Neutron Scattering Center. Michal Mocko
Nuclear cross-section measurements at the Manuel Lujan Jr. Neutron Scattering Center Michal Mocko G. Muhrer, F. Tovesson, J. Ullmann International Topical Meeting on Nuclear Research Applications and Utilization
More informationW. Udo Schröder Departments of Chemistry & of Physics and Astronomy
W. Udo Schröder Departments of Chemistry & of Physics and Astronomy ANSEL Faculty Instructors ACS NuSci Acad Infrastructure 2 Prof. Frank Wolfs Prof. Udo Schrőder Research: Large Underground Xenon (LUX)
More informationExample 1: Neutron Activation Analysis of Medieval Silver Coins
Example 1: Neutron Activation Analysis of Medieval Silver Coins Turnosgroschen Tours Tours Matapan // Grosso Grosso Venedig Großpfennig Bonn Bonn Denar Denar Soest Soest Denar Denar Brabant Brabant Brakteat
More informationAtomic Structure & Nuclear Chemistry Unit 3 Notes
Atomic Structure & Nuclear Chemistry Unit 3 Notes Academic Chemistry Name 52 24 Cr Mass Number Symbol Atomic Number Unit #3 Test Date You can never learn less, you can only learn more. R. Buckminster Fuller
More informationObservation information obtained through the senses; observation in science often involves measurement
Review Sheet Unit 1: The Atom Chemistry the study of the composition of matter and the changes matter undergoes Scientific Method Scientific method a logical, systematic approach to the solution of a scientific
More informationCharacterisation of vibrational modes of adsorbed species
17.7.5 Characterisation of vibrational modes of adsorbed species Infrared spectroscopy (IR) See Ch.10. Infrared vibrational spectra originate in transitions between discrete vibrational energy levels of
More informationINDUSTRIAL RADIOGRAPHY
1 BASICS INDUSTRIAL RADIOGRAPHY -Dr.O.Prabhakar, OP-TECH INTRODUCTION From the time Roentgen discovered X-rays and used it to radiograph his rifle, X-rays are being used in the industry to reveal internal
More informationQuantitative Assessment of Scattering Contributions in MeV-Industrial X-ray Computed Tomography
11th European Conference on Non-Destructive Testing (ECNDT 2014), October 6-10, 2014, Prague, Czech Republic More Info at Open Access Database www.ndt.net/?id=16530 Quantitative Assessment of Scattering
More informationGaetano L Episcopo. Scanning Electron Microscopy Focus Ion Beam and. Pulsed Plasma Deposition
Gaetano L Episcopo Scanning Electron Microscopy Focus Ion Beam and Pulsed Plasma Deposition Hystorical background Scientific discoveries 1897: J. Thomson discovers the electron. 1924: L. de Broglie propose
More informationShielded Scintillator for Neutron Characterization
Shielded Scintillator for Neutron Characterization A Thesis Submitted in Partial Fulfillment of the Requirements for Graduation with Research Distinction in Engineering Physics By Patrick X. Belancourt
More informationDEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS
DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS TSOKOS OPTION I-2 MEDICAL IMAGING Reading Activity Answers IB Assessment Statements Option I-2, Medical Imaging: X-Rays I.2.1. I.2.2. I.2.3. Define
More informationIsotopes: atoms with the same Z but different A s (number of neutrons varies)
All atomic nuclei have protons and neutrons, except hydrogen. Z = atomic number = number of protons in the nucleus A = mass number = Z + number of neutrons A Z X Isotopes: atoms with the same Z but different
More informationParticle-Induced X-Ray Emission Spectrometry (PIXE)
Particle-Induced X-Ray Emission Spectrometry (PIXE) Edited by SVEN A. E. JOHANSSON Department of Nuclear Physics Lund Institute of Technology Lund, Sweden JOHN L. CAMPBELL Department of Physics University
More informationMeasurements of Neutron Total and Capture Cross Sections at the TOF spectrometers of the Moscow Meson Factory
Measurements of Neutron Total and Capture Cross Sections at the TOF spectrometers of the Moscow Meson Factory Yu.V. Grigoriev 1,2, D.V. Khlustin 1, Zh.V. Mezentseva 2, Yu.V. Ryabov 1 1 Institute for Nuclear
More information8/24/2018. Bio 1101 Lecture 2 (guided) Chapters 2: Essential Chemistry. Chapter 2: Essential Chemistry for Biology
1 2 3 4 5 Bio 1101 Lecture 2 (guided) Chapters 2: Essential Chemistry Chapter 2: Essential Chemistry for Biology Levels of biological organization Ecosystem (e.g. savanna) Community (e.g. the organisms
More informationOverview of X-Ray Fluorescence Analysis
Overview of X-Ray Fluorescence Analysis AMPTEK, INC., Bedford, MA 01730 Ph: +1 781 275 2242 Fax: +1 781 275 3470 sales@amptek.com 1 What is X-Ray Fluorescence (XRF)? A physical process: Emission of characteristic
More informationBeam diagnostics: Alignment of the beam to prevent for activation. Accelerator physics: using these sensitive particle detectors.
Beam Loss Monitors When energetic beam particles penetrates matter, secondary particles are emitted: this can be e, γ, protons, neutrons, excited nuclei, fragmented nuclei... Spontaneous radiation and
More informationThe diagram below shows a radioactive isotope going through several half-lives as it decays.
By what process do most stars release energy? A. Electromagnetic induction resulting from strong magnetic fields B. Radioactivity in the interior of the star C. Nuclear fusion in the interior of the star
More informationNeutron Instruments I & II. Ken Andersen ESS Instruments Division
Neutron Instruments I & II ESS Instruments Division Neutron Instruments I & II Overview of source characteristics Bragg s Law Elastic scattering: diffractometers Continuous sources Pulsed sources Inelastic
More informationCHAPTER 2 RADIATION INTERACTIONS WITH MATTER HDR 112 RADIATION BIOLOGY AND RADIATION PROTECTION MR KAMARUL AMIN BIN ABDULLAH
HDR 112 RADIATION BIOLOGY AND RADIATION PROTECTION CHAPTER 2 RADIATION INTERACTIONS WITH MATTER PREPARED BY: MR KAMARUL AMIN BIN ABDULLAH SCHOOL OF MEDICAL IMAGING FACULTY OF HEALTH SCIENCE Interactions
More informationProperties of the nucleus. 8.2 Nuclear Physics. Isotopes. Stable Nuclei. Size of the nucleus. Size of the nucleus
Properties of the nucleus 8. Nuclear Physics Properties of nuclei Binding Energy Radioactive decay Natural radioactivity Consists of protons and neutrons Z = no. of protons (Atomic number) N = no. of neutrons
More informationEXAMINATION QUESTIONS (6)
1. What is a beta-particle? A a helium nucleus B a high-energy electron C four protons D two neutrons EXAMINATION QUESTIONS (6) 2. The diagram shows part of a circuit used to switch street lamps on and
More informationProduction of X-rays. Radiation Safety Training for Analytical X-Ray Devices Module 9
Module 9 This module presents information on what X-rays are and how they are produced. Introduction Module 9, Page 2 X-rays are a type of electromagnetic radiation. Other types of electromagnetic radiation
More informationTHE SLOWPOKE-2 NUCLEAR REACTOR AT THE ROYAL MILITARY COLLEGE OF CANADA: APPLICATIONS FOR THE CANADIAN ARMED FORCES
THE SLOWPOKE-2 NUCLEAR REACTOR AT THE ROYAL MILITARY COLLEGE OF CANADA: APPLICATIONS FOR THE CANADIAN ARMED FORCES P.C. Hungler 1, M. T. Andrews 1, D.G. Kelly 1 and K.S. Nielsen 1 1 Royal Military College
More informationIntroduction to ESS - NIUS
Paul Scherrer Institut W. Wagner, Eberhard H. Lehmann Wir schaffen Wissen heute für morgen Introduction to ESS - NIUS PSI, 25. April 2012 OUTLINE Purpose of ESS-NIUS Situation in Neutron Imaging TODAY
More informationUnit title: Atomic and Nuclear Physics for Spectroscopic Applications
Unit title: Atomic and Nuclear Physics for Spectroscopic Applications Unit code: Y/601/0417 QCF level: 4 Credit value: 15 Aim This unit provides an understanding of the underlying atomic and nuclear physics
More informationMichael Dunn Nuclear Data Group Leader Nuclear Science & Technology Division Medical Physics Working Group Meeting October 26, 2005
Nuclear Data Michael Dunn Nuclear Data Group Leader Nuclear Science & Technology Division Medical Physics Working Group Meeting October 26, 2005 ORELA LANSCE 0.1 00 Data Analyses ORELA data 0.0 75 Basic
More informationDepartment of Chemistry, University of Rochester, Rochester, N.Y POC:
A Mobile Accelerator-Based Neutron Diagnostics Instrument W. Udo Schröder and Jan Tōke Department of Chemistry, University of Rochester, Rochester, N.Y. 14627 POC: schroeder@chem.rochester.edu Project
More informationYear 12 Notes Radioactivity 1/5
Year Notes Radioactivity /5 Radioactivity Stable and Unstable Nuclei Radioactivity is the spontaneous disintegration of certain nuclei, a random process in which particles and/or high-energy photons are
More informationPart 12- Physics Paper 1 Atomic Structure Knowledge Questions
Part 12- Physics Paper 1 Atomic Structure Knowledge Questions Internal energy and energy transfers Internal energy and energy transfers Changes of state and the particle model Particle Model of Matter
More informationNuclear Physics. AP Physics B
Nuclear Physics AP Physics B Nuclear Physics - Radioactivity Before we begin to discuss the specifics of radioactive decay we need to be certain you understand the proper NOTATION that is used. To the
More informationSOURCES of RADIOACTIVITY
Section 9: SOURCES of RADIOACTIVITY This section briefly describes various sources of radioactive nuclei, both naturally occurring and those produced artificially (man-made) in, for example, reactors or
More informationCross-Sections for Neutron Reactions
22.05 Reactor Physics Part Four Cross-Sections for Neutron Reactions 1. Interactions: Cross-sections deal with the measurement of interactions between moving particles and the material through which they
More informationNeutron Physics. The De Broglie relation for matter is: h mv (1) λ =
Neutron Physics Emily P. Wang MIT Department of Physics (Dated: November 11, 2004) Thermal neutrons in a beam emerging from the MIT research reactor were used to study the Maxwell-Boltzmann distribution,
More informationAtomic Theory. Democritus to the Planetary Model
Atomic Theory Democritus to the Planetary Model Democritus Greek philosopher (460-370 BCE) Believed in the philosophy of materialism With Leucippus, they though that matter can not be divided infinitely.
More informationMT Electron microscopy Scanning electron microscopy and electron probe microanalysis
MT-0.6026 Electron microscopy Scanning electron microscopy and electron probe microanalysis Eero Haimi Research Manager Outline 1. Introduction Basics of scanning electron microscopy (SEM) and electron
More informationChemistry 311: Instrumentation Analysis Topic 2: Atomic Spectroscopy. Chemistry 311: Instrumentation Analysis Topic 2: Atomic Spectroscopy
Topic 2b: X-ray Fluorescence Spectrometry Text: Chapter 12 Rouessac (1 week) 4.0 X-ray Fluorescence Download, read and understand EPA method 6010C ICP-OES Winter 2009 Page 1 Atomic X-ray Spectrometry Fundamental
More informationASTM E545 TUTORIAL ON PROPER IMAGE QUALITY INDICATOR USAGE
ASTM E545 IQI USAGE TUTORIAL Page 1 of 9 ASTM E545 TUTORIAL ON PROPER IMAGE QUALITY INDICATOR USAGE Neutron radiography is a non-destructive testing method similar to the more familiar x- ray, but which
More informationChapter Six: X-Rays. 6.1 Discovery of X-rays
Chapter Six: X-Rays 6.1 Discovery of X-rays In late 1895, a German physicist, W. C. Roentgen was working with a cathode ray tube in his laboratory. He was working with tubes similar to our fluorescent
More informationNeutron and Gamma Ray Imaging for Nuclear Materials Identification
Neutron and Gamma Ray Imaging for Nuclear Materials Identification James A. Mullens John Mihalczo Philip Bingham Oak Ridge National Laboratory Oak Ridge, Tennessee 37831-6010 865-574-5564 Abstract This
More informationAuger Electron Spectroscopy (AES)
1. Introduction Auger Electron Spectroscopy (AES) Silvia Natividad, Gabriel Gonzalez and Arena Holguin Auger Electron Spectroscopy (Auger spectroscopy or AES) was developed in the late 1960's, deriving
More informationNuclear Physics Applications in industry, medicine, and liberal arts
Nuclear Physics Applications in industry, medicine, and liberal arts Energy Sources Nuclear Forensics Homeland Security Imaging and Diagnostics Radiation Treatment Material Science Art and Archaeology
More informationBasic physics of nuclear medicine
Basic physics of nuclear medicine Nuclear structure Atomic number (Z): the number of protons in a nucleus; defines the position of an element in the periodic table. Mass number (A) is the number of nucleons
More informationNeutron Imaging at Spallation Neutron Sources
1 AP/IE-06 E.H. Lehmann, A. Kaestner Neutron Imaging at Spallation Neutron Sources Spallation Neutron Source Division, Paul Scherrer Institut, CH-5232 Villigen, Switzerland Email contact of main author:
More informationAtomic Theory. Contribution to Modern Atomic Theory
Alief High School Chemistry STAAR Review Reporting Category 2: Atomic Structure and Nuclear Chemistry C.6.A Understand the experimental design and conclusions used in the development of modern atomic theory,
More informationPhysics Dept. PHY-503-SEMESTER 112 PROJECT. Measurement of Carbon Concentration in Bulk Hydrocarbon Samples
Physics Dept. PHY-503-SEMESTER 112 PROJECT Measurement of Carbon Concentration in Bulk Hydrocarbon Samples Prepared by: Hasan Mohammed Hasan ID: 201002200 Supervisor: Prof. A.A. Naqvi Coordinator: Prof.
More informationExtreme Light Infrastructure - Nuclear Physics ELI - NP
Extreme Light Infrastructure - Nuclear Physics ELI - NP Nicolae-Victor Zamfir National Institute for Physics and Nuclear Engineering (IFIN-HH) Bucharest-Magurele, Romania www.eli-np.ro Bucharest-Magurele
More informationPrecision neutron flux measurement with a neutron beam monitor
Journal of Physics: Conference Series OPEN ACCESS Precision neutron flux measurement with a neutron beam monitor To cite this article: T Ino et al 2014 J. Phys.: Conf. Ser. 528 012039 View the article
More informationCHAPTER 1: Atom and Luminescence
PREPARED BY: MR KAMARUL AMIN BIN ABDULLAH SCHOOL OF MEDICAL IMAGING FACULTY OF HEALTH SCIENCES PHYSICS FOR RADIOGRAPHERS 2 CHAPTER 1: Atom and Luminescence LEARNING OUTCOMES At the end of the lesson, the
More information4.4 Atomic structure Notes
4.4 Atomic structure Notes Ionising radiation is hazardous but can be very useful. Although radioactivity was discovered over a century ago, it took many nuclear physicists several decades to understand
More informationData Acquisition. What choices need to be made?
1 Specimen type and preparation Radiation source Wavelength Instrument geometry Detector type Instrument setup Scan parameters 2 Specimen type and preparation Slide mount Front loading cavity Back loading
More informationRadioactivity III: Measurement of Half Life.
PHY 192 Half Life Spring 2010 1 Radioactivity III: Measurement of Half Life. Introduction This experiment will once again use the apparatus of the first experiment, this time to measure radiation intensity
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 informationNeutron Interactions Part I. Rebecca M. Howell, Ph.D. Radiation Physics Y2.5321
Neutron Interactions Part I Rebecca M. Howell, Ph.D. Radiation Physics rhowell@mdanderson.org Y2.5321 Why do we as Medical Physicists care about neutrons? Neutrons in Radiation Therapy Neutron Therapy
More informationHe-3 Neutron Detectors
Application He-3 Neutron Detectors General Considerations, Applications: He-3 filled proportional counters are standard neutron detectors and are most suitable for the detection of thermal neutrons. Larger
More information