All You Wanted to Know About Electron Microscopy
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Cathode-Ray Tube Displays for Medical Imaging
DIGITAL IMAGING BASICS Cathode-Ray Tube Displays for Medical Imaging Peter A. Keller This paper will discuss the principles of cathode-ray crease the velocity of the electron beam for tube displays in medical imaging and the parameters increased light output from the screen; essential to the selection of displays for specific 4. a focusing section to bring the electron requirements. A discussion of cathode-ray tube fun- beam to a sharp focus at the screen; damentals and medical requirements is included. 9 1990bu W.B. Saunders Company. 5. a deflection system to position the electron beam to a desired location on the screen or KEY WORDS: displays, cathode ray tube, medical scan the beam in a repetitive pattern; and irnaging, high resolution. 6. a phosphor screen to convert the invisible electron beam to visible light. he cathode-ray tube (CRT) is the heart of The assembly of electrodes or elements mounted T almost every medical display and its single within the neck of the CRT is commonly known most costly component. Brightness, resolution, as the "electron gun" (Fig 2). This is a good color, contrast, life, cost, and viewer comfort are analogy, because it is the function of the electron gun to "shoot" a beam of electrons toward the all strongly influenced by the selection of a screen or target. The velocity of the electron particular CRT by the display designer. These beam is a function of the overall accelerating factors are especially important for displays used voltage applied to the tube. For a CRT operating for medical diagnosis in which patient safety and at an accelerating voltage of 20,000 V, the comfort hinge on the ability of the display to electron velocity at the screen is about present easily readable, high-resolution images 250,000,000 mph, or about 37% of the velocity of accurately and rapidly. -
Sculpturing the Electron Wave Function
Sculpturing the Electron Wave Function Roy Shiloh, Yossi Lereah, Yigal Lilach and Ady Arie Department of Physical Electronics, Fleischman Faculty of Engineering, Tel Aviv University, Tel Aviv 6997801, Israel Coherent electrons such as those in electron microscopes, exhibit wave phenomena and may be described by the paraxial wave equation1. In analogy to light-waves2,3, governed by the same equation, these electrons share many of the fundamental traits and dynamics of photons. Today, spatial manipulation of electron beams is achieved mainly using electrostatic and magnetic fields. Other demonstrations include simple phase-plates4 and holographic masks based on binary diffraction gratings5–8. Altering the spatial profile of the beam may be proven useful in many fields incorporating phase microscopy9,10, electron holography11–14, and electron-matter interactions15. These methods, however, are fundamentally limited due to energy distribution to undesired diffraction orders as well as by their binary construction. Here we present a new method in electron-optics for arbitrarily shaping of electron beams, by precisely controlling an engineered pattern of thicknesses on a thin-membrane, thereby molding the spatial phase of the electron wavefront. Aided by the past decade’s monumental leap in nano-fabrication technology and armed with light- optic’s vast experience and knowledge, one may now spatially manipulate an electron beam’s phase in much the same way light waves are shaped simply by passing them through glass elements such as refractive and diffractive lenses. We show examples of binary and continuous phase-plates and demonstrate the ability to generate arbitrary shapes of the electron wave function using a holographic phase-mask. -
Design and Emission Uniformity Studies of a 1.5-MW Gyrotron Electron Gun
PSFC/JA-03-1 Design and Emission Uniformity Studies of a 1.5-MW Gyrotron Electron Gun Anderson, J. P., Korbly, S. E., Temkin, R. J., Shapiro, M. A., Felch, K. L.*, Cauffman, S.* December 2002 Plasma Science and Fusion Center Massachusetts Institute of Technology Cambridge, MA 02139 USA * Microwave Power Products Division Communications and Power Industries Palo Alto, CA 94303 USA This work was supported by the U.S. Department of Energy, Office of Fusion Sciences and Virtual Laboratory for Technology. Reproduction, translation, publication, use and disposal, in whole or in part, by or for the United States government is permitted. Submitted for publication to IEEE Transactions on Plasma Science. 1 Design and Emission Uniformity Studies of a 1.5 MW Gyrotron Electron Gun James P. Anderson1, Stephen E. Korbly1, Richard J. Temkin1, Michael A. Shapiro1, K. L. Felch2, and S. Cauffman2 1Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, MA 02139 2Microwave Power Products Division, Communications and Power Industries, Palo Alto, CA 94303 Abstract We present the design and initial operation of a 96 kV, 40 A Magnetron Injection Gun (MIG) for a 1.5 MW, 110 GHz gyrotron. A critical parameter for the successful application of this electron gun is the uniformity of electron emission. The I-V curve of emission, at a series of temperatures, is measured. Analysis indicates that the work function of the emitter is 1.6 eV with a (total) spread of 0.07 +/- 0.01 eV. Measurement of the azimuthal emission uniformity with a rotating probe indicates that the work function variation around the azimuth, the global spread, is 0.04+/- 0.02 eV. -
Recent Progress in Scanning Electron Microscopy for the Characterization of fine Structural Details of Nano Materials
Progress in Solid State Chemistry 42 (2014) 1e21 Contents lists available at ScienceDirect Progress in Solid State Chemistry journal homepage: www.elsevier.com/locate/pssc Recent progress in scanning electron microscopy for the characterization of fine structural details of nano materials Mitsuo Suga a,*, Shunsuke Asahina a, Yusuke Sakuda a, Hiroyoshi Kazumori a, Hidetoshi Nishiyama a, Takeshi Nokuo a, Viveka Alfredsson b, Tomas Kjellman b, Sam M. Stevens c, Hae Sung Cho d, Minhyung Cho d, Lu Han e, Shunai Che e, Michael W. Anderson f, Ferdi Schüth g, Hexiang Deng h, Omar M. Yaghi i, Zheng Liu j, Hu Young Jeong k, Andreas Stein l, Kazuyuki Sakamoto m, Ryong Ryoo n,o, Osamu Terasaki d,p,** a JEOL Ltd., SM Business Unit, Tokyo, Japan b Physical Chemistry, Lund University, Sweden c Private Contributor, UK d Graduate School of EEWS, KAIST, Republic of Korea e School of Chemistry & Chemical Engineering, Shanghai Jiao Tong University, China f Centre for Nanoporous Materials, School of Chemistry, University of Manchester, UK g Department of Heterogeneous Catalysis, Max-Planck-Institut für Kohlenforschung, Mülheim, Germany h College of Chemistry and Molecular Sciences, Wuhan University, China i Department of Chemistry, University of California, Berkeley, USA j Nanotube Research Center, AIST, Tsukuba, Japan k UNIST Central Research Facilities/School of Mechanical & Advanced Materials Engineering, UNIST, Republic of Korea l Department of Chemistry, University of Minnesota, Minneapolis, USA m Department of Nanomaterials Science, Chiba University, -
Transmission Electron Microscope
GG 711: Advanced Techniques in Geophysics and Materials Science Lecture 14 Transmission Electron Microscope Pavel Zinin HIGP, University of Hawaii, Honolulu, USA www.soest.hawaii.edu\~zinin Resolution of SEM Transmission electron microscopy (TEM) is a microscopy technique whereby a beam of electrons is transmitted through an ultra thin specimen, interacting with the specimen as it passes through. An image is formed from the interaction of the electrons transmitted through the specimen; the image is magnified and focused onto an imaging device, such as a fluorescent screen, on a layer of photographic film, or to be detected by a sensor such as a CCD camera. The first TEM was built by Max Kroll and Ernst Ruska in 1931, with this group developing the first TEM with resolution power greater than that of light in 1933 and the first commercial TEM in 1939. The first practical TEM, Originally installed at I. G Farben-Werke and now on display at the Deutsches Museum in Munich, Germany Comparison of LM and TEM Both glass and EM lenses subject to same distortions and aberrations Glass lenses have fixed focal length, it requires to change objective lens to change magnification. We move objective lens closer to or farther away from specimen to focus. EM lenses to specimen distance fixed, focal length varied by varying current through lens LM: (a) Direct observation TEM: (a) Video imaging (CRT); (b) image of the image; (b) image is is formed by transmitted electrons impinging formed by transmitted light on phosphor coated screen Transmission Electron Microscope: Principle Ray diagram of a conventional transmission electron microscope (top Positioning of signal path) and of a scanning transmission electron microscope (bottom path). -
Light and Electron Microscopy of the Exocrine Pancreas in the Chronically Reserpinized Rat1
003 1 -3998/89/2505-0482$02.00/0 PEDIATRIC RESEARCH Vol. 25, No. 5, 1989 Copyright O 1989 International Pediatric Research Foundation, Inc. Printed rn U.S.A. Light and Electron Microscopy of the Exocrine Pancreas in the Chronically Reserpinized Rat1 GILLES GRONDIN, FRANCOIS A. LEBLOND, JEAN MORISSET, AND DENIS LEBEL Centre de Recherche sur Ies Micanismes de Sicrition, Faculty of Science, University of Sherbrooke, Sherbrooke, QC, Canada, JIK 2RI ABSTRACT. The effects of reserpine injections were stud- been the most studied (1-8). The main effects induced by the ied on the morphology of the pancreas in an experimental reserpine treatment on the ultrastructure of the pancreas are the model for cystic fibrosis, the chronically reserpinized rat. following: an accumulation of granules in the acinar cell, an A detailed examination of the tissue was carried out at the alteration of the granule ultrastructure, a slight diminution of light and electron microscopic levels. The nonspecific ef- the RER and Golgi apparatus, the presence of autophagic bodies, fects of secondary malnutrition induced by the drug were and an augmentation of lysosomal bodies (3,5,9, 10). In another assessed with a group of animals pair fed with the treated paper (1 I), we report the effects of such a treatment on pancreatic animals. In a companion paper, we show that pancreatic growth and on the amount of a glycoprotein characteristic of the wt, lipase, and GP-2 contents also are affected by reserpine zymogen granule membrane, the GP-2. In this study, we specif- treatment. In this study, we report that no morphologic ically report the effects of chronic reserpine treatment at two differences were observed between the exocrine pancreatic doses, on the structure and ultrastructure of the rat pancreas. -
Low Emittance Thermionic Electron Gun at Slri
9th International Particle Accelerator Conference IPAC2018, Vancouver, BC, Canada JACoW Publishing ISBN: 978-3-95450-184-7 doi:10.18429/JACoW-IPAC2018-THPMK088 LOW EMITTANCE THERMIONIC ELECTRON GUN AT SLRI ∗ K. Kittimanapun , N. Juntong, C. Dhammatong, W. Phacheerak, and M. Phanak Synchrotron Light Research Institute (SLRI), Nakhon Ratchasima, Thailand Abstract • Fast beam deflector allowing nanosecond-pulsed elec- The Synchrotron Light Research Institute (SLRI) has de- tron beam to transport to the bunching section and to veloped a new thermionic electron gun producing low emit- deflect undesired electrons to the collimator. tance electron beam for the future upgrade of the existing • Pre-buncher and buncher to adiabatically bunch and one. The thermionic cathode made of a CeB single crys- 6 accelerate electrons to higher energy and minimize tal is selected due to its properties providing high electron the effect from the Radio-Frequency (RF) field that beam current, uniform current density, and high resistance potentially causes the emittance growth. to contamination. In addition, the CeB6 cathode of 3 mm in diameter can produce up to a few Amperes of electron beam ELECTRON GUN current. The electron gun is pulsed at 500 kV with a few microseconds wide to avoid high voltage breakdown as well Three main parts that have to be carefully considered for as to reduce space charge effect resulting in the emittance building the high-performance thermionic electron guns are growth of the extracted electron beam. The preliminary sim- an electron gun cathode, extraction of high-current electron ulation and design of the electron gun together with the high beam, and a high-voltage system. -
Electron and Ion Sources Layout
Electron and Ion Sources Layout • Electron Sources o Thermionic o Photo-Cathodes • Ion Sources o Particle motion in plasmas o Protons o ECR Ion Source o Negative Ions Richard Scrivens, BE Dept, CERN. CAS@CERN, February 2017 1 Electron and Ion Sources Every accelerator chain needs a source! 2 Electron and Ion Sources Every accelerator chain needs a source! Protons Ions Principles of the electron guns, with thermionic and photo Principles of ion sources, and the cathodes types used at CERN. 3 Electron and Ion Sources • Electron Sources o Thermionic o Photo-Cathodes • Ion Sources o Particle motion in plasmas o Protons o ECR Ion Source o Negative Ions o Radioactive Ions 4 Electron and Ion Sources Electron Sources - Basics Insulator Chamber E-field Beam Cathode (Electron source) HT Power Supply The classic Cathode Ray Experiment 5 Electron and Ion Sources • Electron Sources o Thermionic o Photo-Cathodes • Ion Sources o Particle motion in plasmas o Protons o ECR Ion Source o Negative Ions o Radioactive Ions 6 Electron and Ion Sources Electrons – Thermionic Emission Electrons within a material are heated to energies above that needed to escape the material. Cathode emission is dominated by the Richardson Dushmann equation. Energy difference Energy between highest energy electron and vacuum Electrons Work Function fs Material 7 Electron and Ion Sources Electrons – Thermionic Emission (the maths) Conducting materials contain free electrons, who follow the Fermi-Dirac These electrons can energy distribution inside the material. escape the material When a material is heated, the electrons 8 energy distribution shifts from the zero 8 T=2000K T=1000K temperature Fermi distribution. -
The Future of Electron Microscopy
BNL-108108-2015-JA Feature Article for Physics Today The Future of Electron Microscopy Yimei Zhu and Hermann Dürr Seeing is believing. So goes the old adage, and seen evidence is undoubtedly satisfying in that it can be interpreted readily, though not necessarily always correctly. For centuries, humans have tried continuously to improve their abilities of seeing things, from developing telescopes to observe our solar systems, to microscopes to reveal bacteria and viruses. The 2014 Nobel Prize in Chemistry was awarded to Eric Betzig, Stefan Hell and William Moerner for their pioneering work on super-resolution fluorescence microscopy, overcoming Abbe’s diffraction limit in the resolution of conventional light microscopes. It was a breakthrough that enabled ground-breaking discoveries in biological research and also is testimony of the importance of modern microscopy. In February 2014 the US Department of Energy’s Office of Basic Energy Science held a two day workshop that brought together experts from various fields to identify new science that will be enabled by advances in electron microscopy. [1] The workshop focused on studies of ultrafast processes, atomic resolution, sample environments and measuring functionality at nanoscales. This article captures some of the exciting discussions the workshop generated. Seeing with electrons Electrons, photons and neutrons are three fundamental probes of condensed matter. They are routinely used to study complementary physical properties of materials. Neutrons interact with nuclei and atomic spins, x-ray photons with electron clouds and electron probes with electrostatic potentials, i.e., positively charged nuclei screened by negatively charged electrons. Compared with x-rays and neutrons, one advantage of electrons is their much stronger interaction with matter (105 times stronger than elastically scattered x-rays due to the coulomb interaction); hence, for a very small probing volume, the interaction generates strong signals, making it far easier to image and detect individual atoms, molecules, and nanoscale objects. -
Electron Microscopy
Electron microscopy 1 Plan 1. De Broglie electron wavelength. 2. Davisson – Germer experiment. 3. Wave-particle dualism. Tonomura experiment. 4. Wave: period, wavelength, mathematical description. 5. Plane, cylindrical, spherical waves. 6. Huygens-Fresnel principle. 7. Scattering: light, X-rays, electrons. 8. Electron scattering. Born approximation. 9. Electron-matter interaction, transmission function. 10. Weak phase object (WPO) approximation. 11. Electron scattering. Elastic and inelastic scattering 12. Electron scattering. Kinematic and dynamic diffraction. 13. Imaging phase objects, under focus, over focus. Transport of intensity equation. 2 Electrons are particles and waves 3 De Broglie wavelength PhD Thesis, 1924: “With every particle of matter with mass m and velocity v a real wave must be associated” h p 2 h mv p mv Ekin eU 2 2meU Louis de Broglie (1892 - 1987) – wavelength h – Planck constant hc eU – electron energy in eV eU eU2 m c2 eU m0 – electron rest mass 0 c – speed of light The Nobel Prize in Physics 1929 was awarded to Prince Louis-Victor Pierre Raymond de Broglie "for his discovery of the wave nature of electrons." 4 De Broigle “Recherches sur la Théorie des Quanta (Researches on the quantum theory)” (1924) Electron wavelength 142 pm 80 keV – 300 keV 5 Davisson – Germer experiment (1923 – 1929) The first direct evidence confirming de Broglie's hypothesis that particles can have wave properties as well 6 C. Davisson, L. H. Germer, "The Scattering of Electrons by a Single Crystal of Nickel" Nature 119(2998), 558 (1927) Davisson – Germer experiment (1923 – 1929) The first direct evidence confirming de Broglie's hypothesis that particles can have wave properties as well Clinton Joseph Davisson (left) and Lester Germer (right) George Paget Thomson Nobel Prize in Physics 1937: Davisson and Thomson 7 C. -
Super-Resolution Imaging by Dielectric Superlenses: Tio2 Metamaterial Superlens Versus Batio3 Superlens
hv photonics Article Super-Resolution Imaging by Dielectric Superlenses: TiO2 Metamaterial Superlens versus BaTiO3 Superlens Rakesh Dhama, Bing Yan, Cristiano Palego and Zengbo Wang * School of Computer Science and Electronic Engineering, Bangor University, Bangor LL57 1UT, UK; [email protected] (R.D.); [email protected] (B.Y.); [email protected] (C.P.) * Correspondence: [email protected] Abstract: All-dielectric superlens made from micro and nano particles has emerged as a simple yet effective solution to label-free, super-resolution imaging. High-index BaTiO3 Glass (BTG) mi- crospheres are among the most widely used dielectric superlenses today but could potentially be replaced by a new class of TiO2 metamaterial (meta-TiO2) superlens made of TiO2 nanoparticles. In this work, we designed and fabricated TiO2 metamaterial superlens in full-sphere shape for the first time, which resembles BTG microsphere in terms of the physical shape, size, and effective refractive index. Super-resolution imaging performances were compared using the same sample, lighting, and imaging settings. The results show that TiO2 meta-superlens performs consistently better over BTG superlens in terms of imaging contrast, clarity, field of view, and resolution, which was further supported by theoretical simulation. This opens new possibilities in developing more powerful, robust, and reliable super-resolution lens and imaging systems. Keywords: super-resolution imaging; dielectric superlens; label-free imaging; titanium dioxide Citation: Dhama, R.; Yan, B.; Palego, 1. Introduction C.; Wang, Z. Super-Resolution The optical microscope is the most common imaging tool known for its simple de- Imaging by Dielectric Superlenses: sign, low cost, and great flexibility. -
Production of X Rays / Clinical Radiation Generators
External Beam Delivery Systems Argonne National Laboratory Course: 3DCRT for Technologists Karl L. Prado, Ph.D., FACR, FAAPM Professor, Department of Radiation Oncology X-Ray Production X rays, fundamentals, etc. Production of X Rays The X-Ray Tube Components (Figure 3.1 of Khan) Glass tube – maintains vacuum necessary to minimize electron interactions outside of the target area Cathode – contains filament and focusing cup Anode – contains x-ray target The X-Ray Tube The Cathode Tungsten filament (high melting point – 3370 C) Thermionic emission – electron production as a consequence of heating Focusing cup – “directs” electrons to anode Dual filaments (diagnostic tubes) – necessary to balance small focal spots and larger tube currents The X-Ray Tube The Anode Tungsten target High melting point High Z (74) – preferred since bremsstrahlung production Z2 Heat dissipation Copper anode – heat conducted outside glass into oil / water / air Rotating anode (diagnostic tubes) – larger dissipation area Anode hood – copper and tungsten shields intercept stray electrons and x rays Basic X-Ray Circuit Simplified diagram (Khan Figure 3.3) Consists of two parts: High-voltage circuit – provides x-ray tube accelerating potential Filament circuit – provides filament current X-Ray Production Bremsstrahlung (“braking” radiation) Schematics (Khan Figure 3.6) Electromagnetic radiation emitted when an electron losses energy as a consequence of coulomb interaction with the nucleus of an atom X-Ray Energy Spectrum The bremsstrahlung