COMPARISON BETWEEN PULSED AND CONTINUOUS SOURCES FOR SMALL ANGLE NEUTRON SCATTERING (SANS) Tjatji Tjebane, Dolly Langa, Lolan Naicker, Daphney Singo Joint.

Slides:



Advertisements
Similar presentations
STRUCTURE OF MATTER According to the modern atomic model, protons and neutrons are found in the nucleus, and electrons are found outside the nucleus in.
Advertisements

Energy Consumption Fossil Fuel Contribution to Global Energy Demand Year.
Ion Beam Analysis techniques:
Student Practice in JINR Fields of Research Dubna Vlasta Zdychová, Martina Benešová CTU in Prague Czech Republic Pavol Blahušiak, Alexander.
Direct Reactions. Optical model Represent the target nucleus by a potential -- Attenuation length.
Nuclear Physics Selected Topics 5 –Fission and Fusion.
Neutron Generation and Detection Lee Robertson Instrument & Source Division Oak Ridge National Laboratory 17 th National School on Neutron and X-ray Scattering.
Prepared by: Mohapi Thebe(UWC & Necsa-SA) Supervisor: Prof. M. V. Frontasyeva(JINR-RU) 1 Neutron Activation Analysis Summer School Practice Joint Institute.
23.4 Nuclear energy NUCLEARNUCLEAR POWERPOWER Millstone Station.
23.4 Nuclear energy NUCLEARNUCLEAR POWERPOWER Millstone Station.
ANSTO is Australia’s only nuclear science and technology facility
General, Organic, and Biological ChemistryCopyright © 2010 Pearson Education, Inc.1 Chapter 4 Nuclear Chemistry 4.6 Nuclear Fission and Fusion.
Radiation Protection III NUCP 2331
Chapter 21: Nuclear Chemistry The study of nuclear reactions with an emphasis on their uses in chemistry and their effects on biological systems.
Small Angle Neutron Scattering SANS (Neutron scattering) by Samuel Ghebru.
The Chemistry of Life. Section 2.1 Atoms The basic unit of matter are atoms. 100 million atoms would make a row only about 1 cm long! Consists of subatomic.
Ion Beam Analysis Dolly Langa Physics Department, University of Pretoria, South Africa Blane Lomberg Physics Department, University of the Western Cape,
Radioactive ion beam facilities How does they work ? 2012 Student Practice in JINR Fields of Research 9.oct.2012 I. Sivacekflerovlab.jinr.ru.
Studies of neutron cross-sections by activation method in Nuclear Physics Institute Řež and in The Svedberg Laboratory Uppsala and experimental determination.
Small-angle Scattering Study of Mohair Fibres Tjatji Tjebane Instrument Scientist (SANS) NECSA-Wits workshop, NVC, 2015/09/11.
TIME 0F FLIGHT (TOF) METHOD IN SANS TECHNIQUE MBULE P.S 1,MALINDISA C 2, KOAO L.F 1 Supervisor : Dr. KUKLIN A.L 3 1.UNIVERSITY OF THE FREESTATE 2.UNIVERSITY.
Students: Carmen Breazu, Univ. of Craiova, Romania
Reconstruction of Molecule Shape from Data Obtained by Small Angle Neutron Scattering (SANS) E. Badita 1, C. Biris 2, I. Patrascu 1 1 University of Bucharest,
Egypt, Cairo, Tahrir Square, 25 Jan Huge lattice for calibration of SANS instrument Ahmed Esmail Shalan Ahmed Kamel Mohamed Ahmed Eid Hamed Hossam.
Resident Physics Lectures Christensen, Chapter 4 Basic Interactions Between X-Rays and Matter George David Associate Professor Medical College of Georgia.
Introduction to Neutron Scattering Jason T. Haraldsen Advanced Solid State II 2/27/2007.
NUCLEAR CHEMISTRY. Introduction to Nuclear Chemistry  Nuclear chemistry is the study of the structure of and the they undergo.
Managed by UT-Battelle for the Department of Energy Dynamically Polarized Solid Target for Neutron Scattering Josh Pierce, J.K. Zhao Oak Ridge National.
Basic Concepts of Nuclear Physics Part II By Benjamin Thayer PHY3091.
Accelerator Physics, JU, First Semester, (Saed Dababneh). 1 Electron pick-up. ~1/E What about fission fragments????? Bragg curve stochastic energy.
NCNR and NIST Neutron research and probing matter with cold neutrons OR Neutrons ignored no longer!
The Resolution of Small Angle Neutron Scattering (SANS): Theory and the Experimental Authors: E. L. Maweza (University of Fort Hare in SA) A. KUKLIN (Supervisor:
NE Introduction to Nuclear Science Spring 2012 Classroom Session 4: Radioactive Decay Types Radioactive Decay and Growth Isotopes and Decay Diagrams.
Radiation and the Environment Nuclear Changes. Fission vs. Fusion.
1 Neutron Effective Dose calculation behind Concrete Shielding of Charge Particle Accelerators with Energy up to 100 MeV V. E Aleinikov, L. G. Beskrovnaja,
Nuclear Reactions: FISSION & FUSION ã Nuclear reactions deal with interactions between the nuclei of atoms ã Both fission and fusion processes deal with.
Dynamically Polarized Solid Target for Neutron Scattering at the SNS PST 07 J.K. Zhao Neutron Scattering Sciences Division, Spallation Neutron Source Oak.
Thermal Multifragmentation: Experimental Study of Process Dynamics Spinodal State of Nuclear Matter Project FASA-3 Summer practice 2011, JINR Dubna.
NEEP 541 – Neutron Damage Fall 2002 Jake Blanchard.
Small angle neutron scattering
Calculation dependence of shift and size of the sample for X-ray diffraction and SANS Supervisor Dr A. I. Kuklin Rafał Idczak University of Wrocław JINR.
Determination of some features of apoferritin using small angle neutron scattering The whole list of the participants: 1. Marek Rataj JINR group where.
Resolution function for small angle neutron scattering Khaled Gad Mostafa ashshoush supervisor Dr.Alexander Kuklin.
Nuclear energy Summary of period 1. Parts of the atom Mass (A.M.U)Charge Proton1+1 Neutron10 Electron1/1830 Add/subtract a proton: creates a different.
Nuclear Reactions 1.To investigate the composition of gold foil using alpha particles (i.e. to explain the model of an atom).
Spallation Eric Pitcher Head of Target Division February 19, 2016.
Summer Student Practice, 2009, JINR Dubna1 Neutron spectroscopy by time of flight method and determination of neutron beam Prepared by: Sameh Hassan, Yomna.
CLICK HERE TO BEGIN! Directions: Click the term that correctly matches the definition in each question.
Unit 4 Lesson 3 Nuclear Reactions
Unit 4 Lesson 3 Nuclear Reactions
Basic Chemistry.
Basic Chemistry.
User Demands on the Parameters of Future Neutron Source at JINR
Calibration, Simulations, and “Remaining” Issues
Chemistry of Life Ms. Rosendo Biology 10th B.
Basic Chemistry.
1) Which radiation has no electric charge associated with it?
JOINT INSTITUTE FOR NUCLEAR RESEARCH
The splitting of nuclei is _______________.
Outside the nucleus, the beta decay {image} will not occur because the neutron and electron have more total mass than the proton. This process can occur.
The positively charged particle located in the nucleus of an atom
Copyright © Cengage Learning. All rights reserved Review Atomic Number (Z) – number of protons Mass Number (A) – sum of protons and neutrons Copyright.
Chapter 10 Radioactivity and Nuclear reactions
Large Time Scale Molecular Paths Using Least Action.
Nuclear Reactions: FISSION & FUSION.
Unit 4 Lesson 3 Nuclear Reactions
Basic Chemistry.
Basic Chemistry.
Three kinds of particle emission
Advanced Pharmaceutical Analysis
Presentation transcript:

COMPARISON BETWEEN PULSED AND CONTINUOUS SOURCES FOR SMALL ANGLE NEUTRON SCATTERING (SANS) Tjatji Tjebane, Dolly Langa, Lolan Naicker, Daphney Singo Joint Institute for Nuclear Research, Dubna – South African StudentS Summer Practice 2008 Supervisor: Aleksander Kuklin

OUTLINE  Introduction  SANS Principles  Contrast Variation Method  Neutron Sources  IBR-2 and ILL Fission Reactors  SANS Equipment  Main Parameters of YuMO and D22 Instruments  Typical SANS Application  Remarks  Acknowledgements 9/21/20152 SA-JINR Summer School 2008

 Neutron scattering is the process of collision between neutrons emitted by a source and a target which is the studied sample.  When the scattering angles of these collisions are very small (the emerging beam is very close to the axis of the emitted neutrons), it is referred to as Small Angle Neutron Scattering (SANS)  Why Neutrons?  No charge, very penetrating, and non destructive to samples  Neutron wavelengths are comparable to atomic sizes and inter-distance spacing  Neutron interactions with hydrogen and deuterium are widely different making the deuterium labeling method an advantage INTRODUCTION 9/21/20153 SA-JINR Summer School 2008

SANS PRINCIPLE 9/21/20154

CONTRAST VARIATION METHOD  Contrast is the difference in the scattering length density (  ) values between that part of the sample of interest (  p ), and the surrounding media or matrix (  m ), i.e.    p   m  When the contrast is zero, the scattering bodies are said to be at contrast matching.  For example, a sample containing three compounds. Using contrast matching, the contrast between the two parts could be erased, allowing analysis of the third compound. 9/21/20155 SA-JINR Summer School 2008

NEUTRONS SOURCES  Fragmentation Source 2.5 neutrons per event 1 neutron consumed in sustaining reaction 0.5 absorbed High power load per neutron (~ 180 MeV)  Spallation source High energy incoming particle (typically protons) Heavy metal target (Ta, W, U, e.t.c) Neutrons cascade >10 neutrons per incident proton Low power load per outgoing neutron (~ 55 MeV) 9/21/2015

 Radioactive Sources  Nuclear Explosions Californium-252 A typical Cf-252 neutron source emits between 1×10 7 to 1×10 9 neutrons per second It results from a rapid release of energy from an intentionally high-speed nuclear reaction. The driving reaction may be nuclear fission, nuclear fusion or a multistage cascading combination 9/21/20157 SA-JINR Summer School 2008

IBR-2 and ILL Fission Reactors Pulsed Beam Reactor Power output ~ 2 MW 1 X neutrons/(cm 2.s) IBR-2ILL Continuous Beam Reactor Power output ~ 58 MW 1.5 x neutrons/(cm 2.s) 9/21/20158 SA-JINR Summer School 2008

SANS EQUIPMENT AT FLNP (JINR) AND ILL (Grenoble) YuMO 9/21/20159 SA-JINR Summer School 2008 (D22)

MAIN PARAMETERS OF YUMO AND D22 INSTRUMENTS 9/21/ Name of parameterYuMOD22 1Flux at sample ~ 10 7  x 10 7 n.cm  2.s  1 ~ 1.2 x 10 8 n.cm  2 s  1 2Q-Range 7x10  3  0.5 Å -1 4 x 10  4 to 0.44 Å  1 3Dynamic Q-Range 7x10  3  0.5 Å  1 _____ 4Used wavelength0.5A to 8A4.5 to 40 Å 5Calibration standardVanadium (during the experiment)H 2 0 (Placed in sample position) 6Resolution 5  10 % 7Pulse repetition frequency5 HzContinuous 8Specific features Two detector systems: He 3  filled, home made, 8 independent wires. Direct beam: 6Li-convertor (home made preparation) One large area detector system (1m 2 ) movable (

 Biology Organization of biomolecular complexes in solution Mechanisms and pathways for protein folding  Polymers Conformation of polymer molecules in solution Structure of microphase for separated block polymers  Chemistry Structure and interactions in colloid suspensions Mechanisms of molecular self-assembly in solutions  Materials Engineering Analysis of ferrofluids Crystalline structure investigations TYPICAL SANS APPLICATIONS INCLUDE 9/21/ SA-JINR Summer School 2008

REMARKS 9/21/ SA-JINR Summer School 2008

ACKNOWLEDGEMENT The authors would like to acknowledge the following:  Kuklin Aleksander  Kuklin Aleksander  Murugova Tat’yana  Kovalev Yurii  Raul Erhan All of the above from the YuMO Group, Condensed Matter Department  We would also like to extend our regards to the organizer of the Summer Student Practice and all members of the JINR involved in this project. 9/21/ SA-JINR Summer School 2008

THANK YOU!!! 9/21/ SA-JINR Summer School 2008