PPT-Electron Optics Basic Introduction

Bob Ashley 6142013 Overview Why electrons Wavelength and visible light Effects of diffraction and resolution Lens design Defects and distortions Magnification Electron Duality Electrons have a particle and wave nature. They can various functions like phase amplitude and polarization modulation and also wavelength filters The main material which made these devices possible is Lithium Niobate LiNbO3 In the early optical systems where the data rate was low the lasers Jim Schwiegerling PhD. College of Optical Sciences. University of Arizona. Tucson, Arizona. Euclid. Raphael’s . School of Athens. Euclid ~300BC. Greek mathematician. His book . Elements. used to teach geometry for over 2000 years.. Energy Loss . Spectroscopy. Xiaozhe. Zhang. 10/31/2014. Electron . Energy. Loss Spectroscopy. Inelastic . scattering. is a fundamental scattering process in which the kinetic energy of an incident particle is not conserved (in contrast to elastic scattering).. Fire Protection Laboratory Methods Day. June 25, 2014. Paul M. Anderson. Graduate Research Assistant. University of Maryland. Department of Fire Protection Engineering. Transmission Electron Microscopy. Honors senior undergraduate and graduate level course.. Approximately 24-26 lecture hours + 3 seminars.. Lectures 2-4:15 Saturday, Sunday, Tuesday and Wednesday. Designed to provide a . working. knowledge of Nonlinear Optics.. Real-time. Rendering of Physically Based Optical Effects in Theory and Practice. Masanori KAKIMOTO. Tokyo University of Technology. . Table of Contents. Introduction. Basic geometrical . optics. Brief overview of . Fire Protection Laboratory Methods Day. June 25, 2014. Paul M. Anderson. Graduate Research Assistant. University of Maryland. Department of Fire Protection Engineering. Transmission Electron Microscopy. Tutor: Peter Harris. Click on the buttons to move between slides. .. (Make sure you are in “Slide Show” mode). The aims of this course are:. ● . to explain how X-rays are generated in the electron microscope. Secondary Electron D etector Ana Zehtabi Oskuie Introduction Secondary electron secondary electron detector The electron beam interaction with near surface specimen atoms will make a signal which results in the SEM image Andrea Franchi (ESRF, Grenoble). on behalf of the . Beam Dynamics & Diagnostics groups. TW-DULER 2018, DIAMOND, 19. th. -20. th. April 2018. Andrea Franchi Optics Measurements @ ESRF. 2. Outlines. The LEOK-1 Optics Experiment Kit is developed for general physics education in universities and colleges It can be used to construct eight experiments covering the basic experiments in geometrical opt UCRL-PRES-226145Alan Conder Terry Alger Jim Chang Warren Massey Jack Nguyen Ben PeraltaSteve Azevedo Steve Glenn Laura Kegelmeyer Judy Liebman Scott LernerNIF Optics Inspection TeamImagine the scale o The aims of this course are:. ● . to introduce the principles of scanning electron microscopy. ● . to describe the components of the microscope and explain how they work. ● . to highlight some of the problems which can arise during imaging. Three rules:. electrons fill orbitals starting with lowest n and moving upwards;. The order is: 1s, 2s, 2p, 3s, 3p, 4s, 3d, 4p, 5s, 4d etc.. Orbital Diagram. The . electron configuration. of an atom is a shorthand method of writing the location of electrons by sublevel..