Emerging Science and Technology of Antimatter Plasmas and Trap-Based Beamsa… C
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Physical Mechanism of Superconductivity
Physical Mechanism of Superconductivity Part 1 – High Tc Superconductors Xue-Shu Zhao, Yu-Ru Ge, Xin Zhao, Hong Zhao ABSTRACT The physical mechanism of superconductivity is proposed on the basis of carrier-induced dynamic strain effect. By this new model, superconducting state consists of the dynamic bound state of superconducting electrons, which is formed by the high-energy nonbonding electrons through dynamic interaction with their surrounding lattice to trap themselves into the three - dimensional potential wells lying in energy at above the Fermi level of the material. The binding energy of superconducting electrons dominates the superconducting transition temperature in the corresponding material. Under an electric field, superconducting electrons move coherently with lattice distortion wave and periodically exchange their excitation energy with chain lattice, that is, the superconducting electrons transfer periodically between their dynamic bound state and conducting state, so the superconducting electrons cannot be scattered by the chain lattice, and supercurrent persists in time. Thus, the intrinsic feature of superconductivity is to generate an oscillating current under a dc voltage. The wave length of an oscillating current equals the coherence length of superconducting electrons. The coherence lengths in cuprates must have the value equal to an even number times the lattice constant. A superconducting material must simultaneously satisfy the following three criteria required by superconductivity. First, the superconducting materials must possess high – energy nonbonding electrons with the certain concentrations required by their coherence lengths. Second, there must exist three – dimensional potential wells lying in energy at above the Fermi level of the material. Finally, the band structure of a superconducting material should have a widely dispersive antibonding band, which crosses the Fermi level and runs over the height of the potential wells to ensure the normal state of the material being metallic. -
4. Particle Generators/Accelerators
Joint innovative training and teaching/ learning program in enhancing development and transfer knowledge of application of ionizing radiation in materials processing 4. Particle Generators/Accelerators Diana Adlienė Department of Physics Kaunas University of Technolog y Joint innovative training and teaching/ learning program in enhancing development and transfer knowledge of application of ionizing radiation in materials processing This project has been funded with support from the European Commission. This publication reflects the views only of the author. Polish National Agency and the Commission cannot be held responsible for any use which may be made of the information contained therein. Date: Oct. 2017 DISCLAIMER This presentation contains some information addapted from open access education and training materials provided by IAEA TABLE OF CONTENTS 1. Introduction 2. X-ray machines 3. Particle generators/accelerators 4. Types of industrial irradiators The best accelerator in the universe… INTRODUCTION • Naturally occurring radioactive sources: – Up to 5 MeV Alpha’s (helium nuclei) – Up to 3 MeV Beta particles (electrons) • Natural sources are difficult to maintain, their applications are limited: – Chemical processing: purity, messy, and expensive; – Low intensity; – Poor geometry; – Uncontrolled energies, usually very broad Artificial sources (beams) are requested! INTRODUCTION • Beams of accelerated particles can be used to produce beams of secondary particles: Photons (x-rays, gamma-rays, visible light) are generated from beams -
Guide to Understanding Condensation
Guide to Understanding Condensation The complete Andersen® Owner-To-Owner™ limited warranty is available at: www.andersenwindows.com. “Andersen” is a registered trademark of Andersen Corporation. All other marks where denoted are marks of Andersen Corporation. © 2007 Andersen Corporation. All rights reserved. 7/07 INTRODUCTION 2 The moisture that suddenly appears in cold weather on the interior We have created this brochure to answer questions you may have or exterior of window and patio door glass can block the view, drip about condensation, indoor humidity and exterior condensation. on the floor or freeze on the glass. It can be an annoying problem. We’ll start with the basics and offer solutions and alternatives While it may seem natural to blame the windows or doors, interior along the way. condensation is really an indication of excess humidity in the home. Exterior condensation, on the other hand, is a form of dew — the Should you run into problems or situations not covered in the glass simply provides a surface on which the moisture can condense. following pages, please contact your Andersen retailer. The important thing to realize is that if excessive humidity is Visit the Andersen website: www.andersenwindows.com causing window condensation, it may also be causing problems elsewhere in your home. Here are some other signs of excess The Andersen customer service toll-free number: 1-888-888-7020. humidity: • A “damp feeling” in the home. • Staining or discoloration of interior surfaces. • Mold or mildew on surfaces or a “musty smell.” • Warped wooden surfaces. • Cracking, peeling or blistering interior or exterior paint. -
Installation of the Cyclotron Based Clinical Neutron Therapy System in Seattle
Proceedings of the Tenth International Conference on Cyclotrons and their Applications, East Lansing, Michigan, USA INSTALLATION OF THE CYCLOTRON BASED CLINICAL NEUTRON THERAPY SYSTEM IN SEATTLE R. Risler, J. Eenmaa, J. Jacky, I. Kalet, and P. Wootton Medical Radiation Physics RC-08, University of Washington, Seattle ~ 98195, USA S. Lindbaeck Instrument AB Scanditronix, Uppsala, Sweden Sumnary radiation areas is via sliding shielding doors rather than a maze, mai nl y to save space. For the same reason A cyclotron facility has been built for cancer a single door is used to alternately close one or the treatment with fast neutrons. 50.5 MeV protons from a other therapy room. All power supplies and the control conventional, positive ion cyclotron are used to b0m computer are located on the second floor, above the bard a semi-thick Beryllium target located 150 am from maintenance area. The cooler room contains a heat the treatment site. Two treatment rooms are available, exchanger and other refrigeration equipment. Not shown one with a fixed horizontal beam and one with an iso in the diagram is the cooling tower located in another centric gantry capable of 360 degree rotation. In part of the building. Also not shown is the hot lab addition 33 51 MeV protons and 16.5 - 25.5 MeV now under construction an an area adjacent to the deuterons are generated for isotope production inside cyclotron vault. It will be used to process radio the cyclotron vault. The control computer is also used isotopes produced at a target station in the vault. to record and verify treatment parameters for indi vidual patients and to set up and monitor the actual radiation treatment. -
Chapter 3 Bose-Einstein Condensation of an Ideal
Chapter 3 Bose-Einstein Condensation of An Ideal Gas An ideal gas consisting of non-interacting Bose particles is a ¯ctitious system since every realistic Bose gas shows some level of particle-particle interaction. Nevertheless, such a mathematical model provides the simplest example for the realization of Bose-Einstein condensation. This simple model, ¯rst studied by A. Einstein [1], correctly describes important basic properties of actual non-ideal (interacting) Bose gas. In particular, such basic concepts as BEC critical temperature Tc (or critical particle density nc), condensate fraction N0=N and the dimensionality issue will be obtained. 3.1 The ideal Bose gas in the canonical and grand canonical ensemble Suppose an ideal gas of non-interacting particles with ¯xed particle number N is trapped in a box with a volume V and at equilibrium temperature T . We assume a particle system somehow establishes an equilibrium temperature in spite of the absence of interaction. Such a system can be characterized by the thermodynamic partition function of canonical ensemble X Z = e¡¯ER ; (3.1) R where R stands for a macroscopic state of the gas and is uniquely speci¯ed by the occupa- tion number ni of each single particle state i: fn0; n1; ¢ ¢ ¢ ¢ ¢ ¢g. ¯ = 1=kBT is a temperature parameter. Then, the total energy of a macroscopic state R is given by only the kinetic energy: X ER = "ini; (3.2) i where "i is the eigen-energy of the single particle state i and the occupation number ni satis¯es the normalization condition X N = ni: (3.3) i 1 The probability -
22 Thesis Cyclotron Design and Construction Design and Construction of a Cyclotron Capable of Accelerating Protons
22 Thesis Cyclotron Design and Construction Design and Construction of a Cyclotron Capable of Accelerating Protons to 2 MeV by Leslie Dewan Submitted to the Department of Nuclear Science and Engineering in Partial Fulfillment of the Requirements for the Degree of Bachelor of Science in Nuclear Science and Engineering at the Massachusetts Institute of Technology June 2007 © 2007 Leslie Dewan All rights reserved The author hereby grants to MIT permission to reproduce and to distribute publicly paper and electronic copies of this thesis document in whole or in part in any medium now known or hereafter created. Signature of Author: Leslie Dewan Department of Nuclear Science and Engineering May 16, 2007 Certified by: David G. Cory Professor of Nuclear Science and Engineering Thesis Supervisor Accepted by: David G. Cory Professor of Nuclear Science and Engineering Chairman, NSE Committee for Undergraduate Students Leslie Dewan 1 of 23 5/16/07 22 Thesis Cyclotron Design and Construction Design and Construction of a Cyclotron Capable of Accelerating Protons to 2 MeV by Leslie Dewan Submitted to the Department of Nuclear Science and Engineering on May 16, 2007 in Partial Fulfillment of the Requirements for the Degree of Bachelor of Science in Nuclear Science and Engineering ABSTRACT This thesis describes the design and construction of a cyclotron capable of accelerating protons to 2 MeV. A cyclotron is a charged particle accelerator that uses a magnetic field to confine particles to a spiral flight path in a vacuum chamber. An applied electrical field accelerates these particles to high energies, typically on the order of mega-electron volts. -
Atom-Light Interaction and Basic Applications
ICTP-SAIFR school 16.-27. of September 2019 on the Interaction of Light with Cold Atoms Lecture on Atom-Light Interaction and Basic Applications Ph.W. Courteille Universidade de S~aoPaulo Instituto de F´ısicade S~aoCarlos 07/01/2021 2 . 3 . 4 Preface The following notes have been prepared for the ICTP-SAIFR school on 'Interaction of Light with Cold Atoms' held 2019 in S~aoPaulo. They are conceived to support an introductory course on 'Atom-Light Interaction and Basic Applications'. The course is divided into 5 lectures. Cold atomic clouds represent an ideal platform for studies of basic phenomena of light-matter interaction. The invention of powerful cooling and trapping techniques for atoms led to an unprecedented experimental control over all relevant degrees of freedom to a point where the interaction is dominated by weak quantum effects. This course reviews the foundations of this area of physics, emphasizing the role of light forces on the atomic motion. Collective and self-organization phenomena arising from a cooperative reaction of many atoms to incident light will be discussed. The course is meant for graduate students and requires basic knowledge of quan- tum mechanics and electromagnetism at the undergraduate level. The lectures will be complemented by exercises proposed at the end of each lecture. The present notes are mostly extracted from some textbooks (see below) and more in-depth scripts which can be consulted for further reading on the website http://www.ifsc.usp.br/∼strontium/ under the menu item 'Teaching' −! 'Cursos 2019-2' −! 'ICTP-SAIFR pre-doctoral school'. The following literature is recommended for preparation and further reading: Ph.W. -
Taxonomy of Belarusian Educational and Research Portal of Nuclear Knowledge
Taxonomy of Belarusian Educational and Research Portal of Nuclear Knowledge S. Sytova� A. Lobko, S. Charapitsa Research Institute for Nuclear Problems, Belarusian State University Abstract The necessity and ways to create Belarusian educational and research portal of nuclear knowledge are demonstrated. Draft tax onomy of portal is presented. 1 Introduction President Dwight D. Eisenhower in December 1953 presented to the UN initiative "Atoms for Peace" on the peaceful use of nuclear technology. Today, many countries have a strong nuclear program, while other ones are in the process of its creation. Nowadays there are about 440 nuclear power plants operating in 30 countries around the world. Nuclear reac tors are used as propulsion systems for more than 400 ships. About 300 research reactors operate in 50 countries. Such reactors allow production of radioisotopes for medical diagnostics and therapy of cancer, neutron sources for research and training. Approximately 55 nuclear power plants are under construction and 110 ones are planned. Belarus now joins the club of countries that have or are building nu clear power plant. Our country has a large scientific potential in the field of atomic and nuclear physics. Hence it is obvious the necessity of cre ation of portal of nuclear knowledge. The purpose of its creation is the accumulation and development of knowledge in the nuclear field as well as popularization of nuclear knowledge for the general public. *E-mail:[email protected] 212 Wisdom, enlightenment Figure 1: Knowledge management 2 Nuclear knowledge Since beginning of the XXI century the International Atomic Energy Agen cy (IAEA) gives big attention to the nuclear knowledge management (NKM) [1]-[3] . -
It's Just a Phase!
BASIS Lesson Plan Lesson Name: It’s Just a Phase! Grade Level Connection(s) NGSS Standards: Grade 2, Physical Science FOSS CA Edition: Grade 3 Physical Science: Matter and Energy Module *Note to teachers: Detailed standards connections can be found at the end of this lesson plan. Teaser/Overview Properties of matter are illustrated through a series of demonstrations and hands-on explorations. Students will learn to identify solids, liquids, and gases. Water will be used to demonstrate the three phases. Students will learn about sublimation through a fun experiment with dry ice (solid CO2). Next, they will compare the propensity of several liquids to evaporate. Finally, they will learn about freezing and melting while making ice cream. Lesson Objectives ● Students will be able to identify the three states of matter (solid, liquid, gas) based on the relative properties of those states. ● Students will understand how to describe the transition from one phase to another (melting, freezing, evaporation, condensation, sublimation) ● Students will learn that matter can change phase when heat/energy is added or removed Vocabulary Words ● Solid: A phase of matter that is characterized by a resistance to change in shape and volume. ● Liquid: A phase of matter that is characterized by a resistance to change in volume; a liquid takes the shape of its container ● Gas: A phase of matter that can change shape and volume ● Phase change: Transformation from one phase of matter to another ● Melting: Transformation from a solid to a liquid ● Freezing: Transformation -
Canadian-Built Laser Chills Antimatter to Near Absolute Zero for First Time Researchers Achieve World’S First Manipulation of Antimatter by Laser
UNDER EMBARGO UNTIL 8:00 AM PT ON WED MARCH 31, 2021 DO NOT DISTRIBUTE BEFORE EMBARGO LIFT Canadian-built laser chills antimatter to near absolute zero for first time Researchers achieve world’s first manipulation of antimatter by laser Vancouver, BC – Researchers with the CERN-based ALPHA collaboration have announced the world’s first laser-based manipulation of antimatter, leveraging a made-in-Canada laser system to cool a sample of antimatter down to near absolute zero. The achievement, detailed in an article published today and featured on the cover of the journal Nature, will significantly alter the landscape of antimatter research and advance the next generation of experiments. Antimatter is the otherworldly counterpart to matter; it exhibits near-identical characteristics and behaviours but has opposite charge. Because they annihilate upon contact with matter, antimatter atoms are exceptionally difficult to create and control in our world and had never before been manipulated with a laser. “Today’s results are the culmination of a years-long program of research and engineering, conducted at UBC but supported by partners from across the country,” said Takamasa Momose, the University of British Columbia (UBC) researcher with ALPHA’s Canadian team (ALPHA-Canada) who led the development of the laser. “With this technique, we can address long-standing mysteries like: ‘How does antimatter respond to gravity? Can antimatter help us understand symmetries in physics?’. These answers may fundamentally alter our understanding of our Universe.” Since its introduction 40 years ago, laser manipulation and cooling of ordinary atoms have revolutionized modern atomic physics and enabled several Nobel-winning experiments. -
Cyclotrons: Old but Still New
Cyclotrons: Old but Still New The history of accelerators is a history of inventions William A. Barletta Director, US Particle Accelerator School Dept. of Physics, MIT Economics Faculty, University of Ljubljana US Particle Accelerator School ~ 650 cyclotrons operating round the world Radioisotope production >$600M annually Proton beam radiation therapy ~30 machines Nuclear physics research Nuclear structure, unstable isotopes,etc High-energy physics research? DAEδALUS Cyclotrons are big business US Particle Accelerator School Cyclotrons start with the ion linac (Wiederoe) Vrf Vrf Phase shift between tubes is 180o As the ions increase their velocity, drift tubes must get longer 1 v 1 "c 1 Ldrift = = = "# rf 2 f rf 2 f rf 2 Etot = Ngap•Vrf ==> High energy implies large size US Particle Accelerator School ! To make it smaller, Let’s curl up the Wiederoe linac… Bend the drift tubes Connect equipotentials Eliminate excess Cu Supply magnetic field to bend beam 1 2# mc $ 2# mc " rev = = % = const. frf eZion B eZion B Orbits are isochronous, independent of energy ! US Particle Accelerator School … and we have Lawrence’s* cyclotron The electrodes are excited at a fixed frequency (rf-voltage source) Particles remain in resonance throughout acceleration A new bunch can be accelerated on every rf-voltage peak: ===> “continuous-wave (cw) operation” Lawrence, E.O. and Sloan, D.: Proc. Nat. Ac. Sc., 17, 64 (1931) Lawrence, E.O. & Livingstone M.S.: Phys. Rev 37, 1707 (1931). * The first cyclotron patent (German) was filed in 1929 by Leó Szilard but never published in a journal US Particle Accelerator School Synchronism only requires that τrev = N/frf “Isochronous” particles take the same revolution time for each turn. -
Capillary Condensation of Colloid–Polymer Mixtures Confined
INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS: CONDENSED MATTER J. Phys.: Condens. Matter 15 (2003) S3411–S3420 PII: S0953-8984(03)66420-9 Capillary condensation of colloid–polymer mixtures confined between parallel plates Matthias Schmidt1,Andrea Fortini and Marjolein Dijkstra Soft Condensed Matter, Debye Institute, Utrecht University, Princetonplein 5, 3584 CC Utrecht, The Netherlands Received 21 July 2003 Published 20 November 2003 Onlineatstacks.iop.org/JPhysCM/15/S3411 Abstract We investigate the fluid–fluid demixing phase transition of the Asakura–Oosawa model colloid–polymer mixture confined between two smooth parallel hard walls using density functional theory and computer simulations. Comparing fluid density profiles for statepoints away from colloidal gas–liquid coexistence yields good agreement of the theoretical results with simulation data. Theoretical and simulation results predict consistently a shift of the demixing binodal and the critical point towards higher polymer reservoir packing fraction and towards higher colloid fugacities upon decreasing the plate separation distance. This implies capillary condensation of the colloid liquid phase, which should be experimentally observable inside slitlike micropores in contact with abulkcolloidal gas. 1. Introduction Capillary condensation denotes the phenomenon that spatial confinement can stabilize a liquid phase coexisting with its vapour in bulk [1, 2]. In order for this to happen the attractive interaction between the confining walls and the fluid particles needs to be sufficiently strong. Although the main body of work on this subject has been done in the context of confined simple liquids, one might expect that capillary condensation is particularly well suited to be studied with colloidal dispersions. In these complex fluids length scales are on the micron rather than on the ångstrom¨ scale which is typical for atomicsubstances.