Electron Microscopy SEM and TEM
|
|
|
- Austin Boyd
- 9 years ago
- Views:
Transcription
1 Electron Microscopy SEM and TEM
2 Content 1. Introduction: Motivation for electron microscopy 2. Interaction with matter 3. SEM: Scanning Electron Microscopy 3.1 Functional Principle 3.2 Examples 3.3 EDX (Energy Dispersive X ray spectroscopy) 4. TEM: Transmission Electron Microscopy 4.1 Functional Principle 4.2 Examples 4.3 Comparing SEM and TEM 4.4 HAADF (High Angle Annular Dark Field Imaging)
3 1. Motivation for EM Resolution of light microscope is limited: λ sin Θ = D wavelenght of visible light less diffraction for smaller wavelenghts possible magnification: ~ [1]
4 1. Motivation for EM Different approach: use electrons instead of light Access to much smaller wavelengths h λ = (3.7 pm for 100 kev) p electrostatic/electromagnetic t ti l t ti lenses instead of glass lenses possible magnification: ~ [2]
5 2. Interaction with matter Backscattered electrons Secondary electrons Auger electrons Transmitted electrons specimen X Rays phonons
6 2. Interaction with matter Topography and composition Topography p Backscattered electrons Secondary electrons Structure and composition Composition Transmitted electrons X Rays
7 2. Interaction with matter 2 different approaches: Backscattered and Transmitted electrons secondary electrons SEM TEM
8 3. SEM Scanning Electron Microscopy
9 31Functional 3.1 Principle Electron source Condenser lens Scan coil Objective lens Specimen + Detectors 2 25 kv e
10 31Functional 3.1 Principle Electron gun e Condenser lens Scan coil Objective lens coils N coils Specimen + Detectors S N
11 31Functional 3.1 Principle Electron gun e Condenser lens Scan coil Objective lens Waveform generator Specimen + Detectors Detector signal
12 31Functional 3.1 Principle Electron gun Condenser lens e Scan coil coils coils Objective lens Specimen + Detectors f
13 31Functional 3.1 Principle Electron gun Condenser lens e Electron and Lightdetectors Scan coil Objective lens Specimen + Detectors
14 32Examples 3.2 Photonic crystal in silicon substrate Nanowires in silicon substrate WSI, D. Dorfner WSI, D. Pedone
15 33Energy 3.3 Dispersive Systems (EDX) e e Bremsstrahlung X ray Continuum Electron filling holes Characteristic X rays Information about chemical composition
16 33Energy 3.3 Dispersive Systems (EDX) Solidstate X ray Detector N 2 Si(Li) X ray coldfinger X ray creates hole/electron pairs (3.8 ev necessary per pair) Number of pairs and current are a measure for X ray energy
17 33Energy 3.3 Dispersive Systems (EDX) Alloy of aluminum and tungsten [3]
18 reminder 2 different approaches: Backscattered and Transmitted electrons secondary electrons SEM TEM
19 4. TEM Transmission Electron Microscopy
20 41Functional 4.1 principles Electron gun Condenser lenses Object Objective lens + intermediate lens + projective lense kv e
21 41Functional 4.1 principles Electron gun Condenser lenses e Object Objective lens + intermediate lens + projective lense
22 41Functional 4.1 principles Electron gun e Condenser lenses Object ~100nm specimen Objective lens + intermediate lens + projective lense scattered direct beam
23 41Functional 4.1 principles Electron gun Condenser lenses Object Objective lens + intermediate lens + projective lense
24 42Example 4.2 Crossectional analysis of a conductor nanogap device WSI, S. Strobel WSI, D. Pedone
25 43Comparison 4.3 of SEM and TEM SEM: scans with a focused point TEM: illumantes whole sample
26 44High 4.4 Angle Annular Dark Field Imaging g( (HAADF) used in STEM (scanning transmission electron microscopy) rayleigh scattering at high angles Angle depends on the atomic number Z: 2 electron intesity: I Z by messuring the electron intensity, while scanning over the sample, information about the chemical compositio can be aquired
27 Thanks for your attention.
28 reference TUM chemie department: tum htm wikipedia: electron microscope dispersive_x ray_spectroscopy Transmission Electron Microscopy, D. B. Williams and C. B. Carter Scanning electron microscopy and X ray Microanalysis, G. Lowes electron microscopy in solid state physics, H. Bethge and J. Heydenreich
29 reference [1] [2] [3] edx.htm tum edx htm
Scanning Electron Microscopy: an overview on application and perspective
Scanning Electron Microscopy: an overview on application and perspective Elvio Carlino Center for Electron Microscopy - IOM-CNR Laboratorio Nazionale TASC - Trieste, Italy Location of the Center for Electron
Electron Microscopy 3. SEM. Image formation, detection, resolution, signal to noise ratio, interaction volume, contrasts
Electron Microscopy 3. SEM Image formation, detection, resolution, signal to noise ratio, interaction volume, contrasts 3-1 SEM is easy! Just focus and shoot "Photo"!!! Please comment this picture... Any
View of ΣIGMA TM (Ref. 1)
Overview of the FESEM system 1. Electron optical column 2. Specimen chamber 3. EDS detector [Electron Dispersive Spectroscopy] 4. Monitors 5. BSD (Back scatter detector) 6. Personal Computer 7. ON/STANDBY/OFF
EDS system. CRF Oxford Instruments INCA CRF EDAX Genesis EVEX- NanoAnalysis Table top system
EDS system Most common X-Ray measurement system in the SEM lab. Major elements (10 wt% or greater) identified in ~10 secs. Minor elements identifiable in ~100 secs. Rapid qualitative and accurate quantitative
Nanoelectronics 09. Atsufumi Hirohata Department of Electronics. Quick Review over the Last Lecture
Nanoelectronics 09 Atsufumi Hirohata Department of Electronics 12:00 Wednesday, 4/February/2015 (P/L 006) Quick Review over the Last Lecture ( Field effect transistor (FET) ): ( Drain ) current increases
Chapter 4. Microscopy, Staining, and Classification. Lecture prepared by Mindy Miller-Kittrell North Carolina State University
Chapter 4 Microscopy, Staining, and Classification 2012 Pearson Education Inc. Lecture prepared by Mindy Miller-Kittrell North Carolina State University Microscopy and Staining 2012 Pearson Education Inc.
Lenses and Apertures of A TEM
Instructor: Dr. C.Wang EMA 6518 Course Presentation Lenses and Apertures of A TEM Group Member: Anup Kr. Keshri Srikanth Korla Sushma Amruthaluri Venkata Pasumarthi Xudong Chen Outline Electron Optics
Preface Light Microscopy X-ray Diffraction Methods
Preface xi 1 Light Microscopy 1 1.1 Optical Principles 1 1.1.1 Image Formation 1 1.1.2 Resolution 3 1.1.3 Depth of Field 5 1.1.4 Aberrations 6 1.2 Instrumentation 8 1.2.1 Illumination System 9 1.2.2 Objective
Ion Beam Sputtering: Practical Applications to Electron Microscopy
Ion Beam Sputtering: Practical Applications to Electron Microscopy Applications Laboratory Report Introduction Electron microscope specimens, both scanning (SEM) and transmission (TEM), often require a
Introduction to EDX. Energy Dispersive X-ray Microanalysis (EDS, Energy dispersive Spectroscopy) Basics of EDX
Introduction to EDX Energy Dispersive X-ray Microanalysis (EDS, Energy dispersive Spectroscopy) EDX Marco Cantoni 1 Basics of EDX a) Generation of X-rays b) Detection Si(Li) Detector, SDD Detector, EDS
CSCI 4974 / 6974 Hardware Reverse Engineering. Lecture 8: Microscopy and Imaging
CSCI 4974 / 6974 Hardware Reverse Engineering Lecture 8: Microscopy and Imaging Data Acquisition for RE Microscopy Imaging Registration and stitching Microscopy Optical Electron Scanning Transmission Scanning
The Basics of Scanning Electron Microscopy
The Basics of Scanning Electron Microscopy The small scanning electron microscope is easy to use because almost every variable is pre-set: the acceleration voltage is always 15kV, it has only a single
Physics 441/2: Transmission Electron Microscope
Physics 441/2: Transmission Electron Microscope Introduction In this experiment we will explore the use of transmission electron microscopy (TEM) to take us into the world of ultrasmall structures. This
Properties of Electrons, their Interactions with Matter and Applications in Electron Microscopy
Properties of Electrons, their Interactions with Matter and Applications in Electron Microscopy By Frank Krumeich Laboratory of Inorganic Chemistry, ETH Zurich, Vladimir-Prelog-Weg 1, 8093 Zurich, Switzerland
PHYSICAL METHODS, INSTRUMENTS AND MEASUREMENTS Vol. III - Surface Characterization - Marie-Geneviève Barthés-Labrousse
SURFACE CHARACTERIZATION Marie-Geneviève Centre d Etudes de Chimie Métallurgique, CNRS, Vitry-sur-Seine, France Keywords: Surface Analysis, Surface imaging, Surface composition, Surface chemical analysis,
Reflection Electron Microscopy and Spectroscopy for Surface Analysis
Reflection Electron Microscopy and Spectroscopy for Surface Analysis by Zhong Lin Wang 1 Introduction In 1986, E. Ruska was awarded the Nobel Physics Prize for his pioneering work of building the world's
Keywords: Planar waveguides, sol-gel technology, transmission electron microscopy
Structural and optical characterisation of planar waveguides obtained via Sol-Gel F. Rey-García, C. Gómez-Reino, M.T. Flores-Arias, G.F. De La Fuente, W. Assenmacher, W. Mader ABSTRACT Planar waveguides
Forensic Science: The Basics. Microscopy
Forensic Science: The Basics Microscopy Chapter 6 Jay A. Siegel,Ph.D. Power point presentation by Greg Galardi, Peru State College, Peru Nebraska Presentation by Greg Galardi, Peru State College CRC Press,
Electron Microscopy 3. SEM. Image formation, detection, resolution, signal to noise ratio, interaction volume, contrasts
Electron Microscopy 3. SEM Image formation, detection, resolution, signal to noise ratio, interaction volume, contrasts SEM is easy! Just focus and shoot "Photo"!!! Please comment this picture... Any idea
Introduction to Energy Dispersive X-ray Spectrometry (EDS)
Introduction to Energy Dispersive X-ray Spectrometry (EDS) 1. Introduction 1.1 Principles of the technique EDS makes use of the X-ray spectrum emitted by a solid sample bombarded with a focused beam of
Microscopy. MICROSCOPY Light Electron Tunnelling Atomic Force RESOLVE: => INCREASE CONTRAST BIODIVERSITY I BIOL1051 MAJOR FUNCTIONS OF MICROSCOPES
BIODIVERSITY I BIOL1051 Microscopy Professor Marc C. Lavoie [email protected] MAJOR FUNCTIONS OF MICROSCOPES MAGNIFY RESOLVE: => INCREASE CONTRAST Microscopy 1. Eyepieces 2. Diopter adjustment
Use the BET (after Brunauer, Emmett and Teller) equation is used to give specific surface area from the adsorption
Number of moles of N 2 in 0.129dm 3 = 0.129/22.4 = 5.76 X 10-3 moles of N 2 gas Module 8 : Surface Chemistry Objectives Lecture 37 : Surface Characterization Techniques After studying this lecture, you
7. advanced SEM. Latest generation of SEM SEM
7. advanced SEM SEM Low voltage SE imaging Condition of the surface, coatings, plasma cleaning Low voltage BSE imaging Polishing for BSE, EDX and EBSD, effect of ion beam etching/polishing 1 Latest generation
Lectures about XRF (X-Ray Fluorescence)
1 / 38 Lectures about XRF (X-Ray Fluorescence) Advanced Physics Laboratory Laurea Magistrale in Fisica year 2013 - Camerino 2 / 38 X-ray Fluorescence XRF is an acronym for X-Ray Fluorescence. The XRF technique
Scanning Electron Microscopy Primer
Scanning Electron Microscopy Primer Bob Hafner This primer is intended as background for the Introductory Scanning Electron Microscopy training offered by the University of Minnesota s Characterization
Energy Dispersive Spectroscopy on the SEM: A Primer
Energy Dispersive Spectroscopy on the SEM: A Primer Bob Hafner This primer is intended as background for the EDS Analysis on the SEM course offered by the University of Minnesota s Characterization Facility.
Introduction to microstructure
Introduction to microstructure 1.1 What is microstructure? When describing the structure of a material, we make a clear distinction between its crystal structure and its microstructure. The term crystal
Polarization Dependence in X-ray Spectroscopy and Scattering. S P Collins et al Diamond Light Source UK
Polarization Dependence in X-ray Spectroscopy and Scattering S P Collins et al Diamond Light Source UK Overview of talk 1. Experimental techniques at Diamond: why we care about x-ray polarization 2. How
Microscopic Techniques
Microscopic Techniques Outline 1. Optical microscopy Conventional light microscopy, Fluorescence microscopy, confocal/multiphoton microscopy and Stimulated emission depletion microscopy 2. Scanning probe
Sensors & Instruments for station. returned samples. Chun Chia Tan
Sensors & Instruments for station based materials characterization of returned samples Chun Chia Tan 04/01/2009 Outline Introduction to materials characterization General overview of the equipment used
NEAR FIELD OPTICAL MICROSCOPY AND SPECTROSCOPY WITH STM AND AFM PROBES
Vol. 93 (1997) A CTA PHYSICA POLONICA A No. 2 Proceedings of the 1st International Symposium on Scanning Probe Spectroscopy and Related Methods, Poznań 1997 NEAR FIELD OPTICAL MICROSCOPY AND SPECTROSCOPY
Fundamentals of Scanning Electron Microscopy
1 Fundamentals of Scanning Electron Microscopy Weilie Zhou, Robert P. Apkarian, Zhong Lin Wang, and David Joy 1. Introduction The scanning electron microscope (SEM) is one of the most versatile instruments
Near-field scanning optical microscopy (SNOM)
Adviser: dr. Maja Remškar Institut Jožef Stefan January 2010 1 2 3 4 5 6 Fluorescence Raman and surface enhanced Raman 7 Conventional optical microscopy-limited resolution Two broad classes of techniques
Supporting Information
Supporting Information Simple and Rapid Synthesis of Ultrathin Gold Nanowires, Their Self-Assembly and Application in Surface-Enhanced Raman Scattering Huajun Feng, a Yanmei Yang, a Yumeng You, b Gongping
DOE Solar Energy Technologies Program Peer Review. Denver, Colorado April 17-19, 2007
DOE Solar Energy Technologies Program Peer Review Evaluation of Nanocrystalline Silicon Thin Film by Near-Field Scanning Optical Microscopy AAT-2-31605-05 Magnus Wagener and George Rozgonyi North Carolina
for Low power Energy Harvesting Sun to fiber' Solar Devices
Nanostructured Energy Conversion for Low power Energy Harvesting Devices and Beyond for High power Sun to fiber' Solar Devices Michael Oye and Nobuhiko Nobby Kobayashi Advanced Studies Laboratories and
Electron Microprobe Analysis X-ray spectrometry:
Electron Microprobe Analysis X-ray spectrometry: 1. X-ray generation and emission 2. X-ray detection and measurement X-ray energy and wavelength E=hν h : Planck's constant (6.626x10-34 Joule.sec or, 6.626x10-34
h e l p s y o u C O N T R O L
contamination analysis for compound semiconductors ANALYTICAL SERVICES B u r i e d d e f e c t s, E v a n s A n a l y t i c a l g r o u p h e l p s y o u C O N T R O L C O N T A M I N A T I O N Contamination
Nanometer-scale imaging and metrology, nano-fabrication with the Orion Helium Ion Microscope
[email protected] Nanometer-scale imaging and metrology, nano-fabrication with the Orion Helium Ion Microscope Bin Ming, András E. Vladár and Michael T. Postek National Institute of Standards and Technology
Optical Microscope; Scanning Electron Microscope (SEM); Transmission Electron Microscope (TEM);
Lecture 3 Brief Overview of Traditional Microscopes Optical Microscope; Scanning Electron Microscope (SEM); Transmission Electron Microscope (TEM); Comparison with scanning probe microscope (SPM) General
Microscopy: Principles and Advances
Microscopy: Principles and Advances Chandrashekhar V. Kulkarni University of Central Lancashire, Preston, United kingdom May, 2014 University of Ljubljana Academic Background 2005-2008: PhD-Chemical Biology
Testing and characterization of anti-reflection coatings on glass
Testing and characterization of anti-reflection coatings on glass Diagnostic approaches at CSP M.Turek, M. Dyrba, S. Großer, V. Naumann, Ch. Hagendorf contact: [email protected] Tests and methods
CREOL, College of Optics & Photonics, University of Central Florida
OSE6650 - Optical Properties of Nanostructured Materials Optical Properties of Nanostructured Materials Fall 2013 Class 3 slide 1 Challenge: excite and detect the near field Thus far: Nanostructured materials
CALCULATION METHODS OF X-RAY SPECTRA: A COMPARATIVE STUDY
243 CALCULATION METHODS OF X-RAY SPECTRA: A COMPARATIVE STUDY B. Chyba, M. Mantler, H. Ebel, R. Svagera Technische Universit Vienna, Austria ABSTRACT The accurate characterization of the spectral distribution
Introduction to the Scanning Electron Microscope
Introduction to the Scanning Electron Microscope Theory, Practice, & Procedures Prepared by Michael Dunlap & Dr. J. E. Adaskaveg Presented by the FACILITY FOR ADVANCED INSTRUMENTATION, U. C. Davis 1997
Looking through the fish-eye the Electron Ronchigram. Duncan T.L. Alexander CIME seminar May 24, 2012
Looking through the fish-eye the Electron Ronchigram Duncan T.L. Alexander CIME seminar May 24, 2012 Introduction Aim of the seminar: open a discussion on the Electron Ronchigram How is it formed? What
Scanning Electron Microscopy tools for material characterization
5th International Workshop on Mechanisms of Vacuum Arcs 02-04/09/2015 Scanning Electron Microscopy tools for material characterization Focus on EBSD for characterisation of dislocation structures Floriane
EXPERIMENT #1: MICROSCOPY
EXPERIMENT #1: MICROSCOPY Brightfield Compound Light Microscope The light microscope is an important tool in the study of microorganisms. The compound light microscope uses visible light to directly illuminate
Basic principles and mechanisms of NSOM; Different scanning modes and systems of NSOM; General applications and advantages of NSOM.
Lecture 16: Near-field Scanning Optical Microscopy (NSOM) Background of NSOM; Basic principles and mechanisms of NSOM; Basic components of a NSOM; Different scanning modes and systems of NSOM; General
Detailed Alignment Procedure for the JEOL 2010F Transmission Electron Microscope
Detailed Alignment Procedure for the JEOL 2010F Transmission Electron Microscope by Wendy Sarney ARL-MR-603 December 2004 Approved for public release; distribution unlimited. NOTICES Disclaimers The findings
Advanced Physics Laboratory. XRF X-Ray Fluorescence: Energy-Dispersive analysis (EDXRF)
Advanced Physics Laboratory XRF X-Ray Fluorescence: Energy-Dispersive analysis (EDXRF) Bahia Arezki Contents 1. INTRODUCTION... 2 2. FUNDAMENTALS... 2 2.1 X-RAY PRODUCTION... 2 2. 1. 1 Continuous radiation...
Introduction to X-Ray Powder Diffraction Data Analysis
Introduction to X-Ray Powder Diffraction Data Analysis Center for Materials Science and Engineering at MIT http://prism.mit.edu/xray An X-ray diffraction pattern is a plot of the intensity of X-rays scattered
Crystal Structure of High Temperature Superconductors. Marie Nelson East Orange Campus High School NJIT Professor: Trevor Tyson
Crystal Structure of High Temperature Superconductors Marie Nelson East Orange Campus High School NJIT Professor: Trevor Tyson Introduction History of Superconductors Superconductors are material which
Measuring the Point Spread Function of a Fluorescence Microscope
Frederick National Laboratory Measuring the Point Spread Function of a Fluorescence Microscope Stephen J Lockett, PhD Principal Scientist, Optical Microscopy and Analysis Laboratory Frederick National
How To Understand Light And Color
PRACTICE EXAM IV P202 SPRING 2004 1. In two separate double slit experiments, an interference pattern is observed on a screen. In the first experiment, violet light (λ = 754 nm) is used and a second-order
PHOTOELECTRIC EFFECT AND DUAL NATURE OF MATTER AND RADIATIONS
PHOTOELECTRIC EFFECT AND DUAL NATURE OF MATTER AND RADIATIONS 1. Photons 2. Photoelectric Effect 3. Experimental Set-up to study Photoelectric Effect 4. Effect of Intensity, Frequency, Potential on P.E.
Oxford Instruments Analytical technical briefing. Wavelength Dispersive X-ray Microanalysis
Oxford Instruments Analytical technical briefing Wavelength Dispersive X-ray Microanalysis Oxford Instruments Analytical technical briefing Introduction Electron probe X-ray microanalysis techniques (Wavelength
Fundamentals of modern UV-visible spectroscopy. Presentation Materials
Fundamentals of modern UV-visible spectroscopy Presentation Materials The Electromagnetic Spectrum E = hν ν = c / λ 1 Electronic Transitions in Formaldehyde 2 Electronic Transitions and Spectra of Atoms
bulk 5. Surface Analysis Why surface Analysis? Introduction Methods: XPS, AES, RBS
5. Surface Analysis Introduction Methods: XPS, AES, RBS Autumn 2011 Experimental Methods in Physics Marco Cantoni Why surface Analysis? Bulk: structural function Electrical/thermal conduction Volume increases
Usage of AFM, SEM and TEM for the research of carbon nanotubes
Usage of AFM, SEM and TEM for the research of carbon nanotubes K.Safarova *1, A.Dvorak 2, R. Kubinek 1, M.Vujtek 1, A. Rek 3 1 Department of Experimental Physics, Faculty of Science, Palacky University,
Diffraction Course Series 2015
Diffraction Course Series 2015 Mark Wainwright Analytical Centre Kensington Campus, Chemical Sciences Building F10, Room G37 The Mark Wainwright Analytical Centre is offering a new series of courses covering
Name: Due: September 21 st 2012. Physics 7230 Laboratory 3: High Resolution SEM Imaging
Name: Due: September 21 st 2012 Physics 7230 Laboratory 3: High Resolution SEM Imaging 1. What is meant by the term resolution? How does this differ from other image variables, such as signal to noise
Metrics of resolution and performance for CD-SEMs
Metrics of resolution and performance for CD-SEMs David C Joy a,b, Yeong-Uk Ko a, and Justin J Hwu a a EM Facility, University of Tennessee, Knoxville, TN 37996 b Oak Ridge National Laboratory, Oak Ridge,
A Guide to Acousto-Optic Modulators
A Guide to Acousto-Optic Modulators D. J. McCarron December 7, 2007 1 Introduction Acousto-optic modulators (AOMs) are useful devices which allow the frequency, intensity and direction of a laser beam
Chapter 13 Confocal Laser Scanning Microscopy C. Robert Bagnell, Jr., Ph.D., 2012
Chapter 13 Confocal Laser Scanning Microscopy C. Robert Bagnell, Jr., Ph.D., 2012 You are sitting at your microscope working at high magnification trying to sort out the three-dimensional compartmentalization
Raman spectroscopy Lecture
Raman spectroscopy Lecture Licentiate course in measurement science and technology Spring 2008 10.04.2008 Antti Kivioja Contents - Introduction - What is Raman spectroscopy? - The theory of Raman spectroscopy
vii TABLE OF CONTENTS CHAPTER TITLE PAGE DECLARATION DEDICATION ACKNOWLEDGEMENT ABSTRACT ABSTRAK
vii TABLE OF CONTENTS CHAPTER TITLE PAGE DECLARATION DEDICATION ACKNOWLEDGEMENT ABSTRACT ABSTRAK TABLE OF CONTENTS LIST OF TABLES LIST OF FIGURES LIST OF SYMBOLS / ABBREVIATIONS LIST OF APPENDICES ii iii
The Focused Ion Beam Scanning Electron Microscope: A tool for sample preparation, two and three dimensional imaging. Jacob R.
The Focused Ion Beam Scanning Electron Microscope: A tool for sample preparation, two and three dimensional imaging Jacob R. Bowen Contents Components of a FIB-SEM Ion interactions Deposition & patterns
Production 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
X Ray Flourescence (XRF)
X Ray Flourescence (XRF) Aspiring Geologist XRF Technique XRF is a rapid, relatively non destructive process that produces chemical analysis of rocks, minerals, sediments, fluids, and soils It s purpose
Usage of Carbon Nanotubes in Scanning Probe Microscopes as Probe. Keywords: Carbon Nanotube, Scanning Probe Microscope
International Journal of Arts and Sciences 3(1): 18-26 (2009) CD-ROM. ISSN: 1944-6934 InternationalJournal.org Usage of Carbon Nanotubes in Scanning Probe Microscopes as Probe Bedri Onur Kucukyildirim,
Image Formation in the Electron Microscope
T H E U N I V E R S I T Y of T E X A S S C H O O L O F H E A L T H I N F O R M A T I O N S C I E N C E S A T H O U S T O N Image Formation in the Electron Microscope For students of HI 6001-125 Computational
Acquiring molecular interference functions of X-ray coherent scattering for breast tissues by combination of simulation and experimental methods
Short report Acquiring molecular interference functions of X-ray coherent scattering for breast tissues by combination of simulation and experimental methods A. Chaparian 1*,M.A. Oghabian 1, V. Changizi
Lecture 3: Fibre Optics
Lecture 3: Fibre Optics Lecture aims to explain: 1. Fibre applications in telecommunications 2. Principle of operation 3. Single- and multi-mode fibres 4. Light losses in fibres Fibre is a transparent
Generation of X-Rays (prepared by James R. Connolly, for EPS400-002, Introduction to X-Ray Powder Diffraction, Spring 2005)
A Bit of History A good discussion of the early x-ray discoveries may be found in Chapter 1 of Moore and Reynolds (1997). I have borrowed freely from a variety of sources for this section. An online sketch
THEORY OF XRF. Getting acquainted with the principles. Peter Brouwer
THEORY OF XRF Getting acquainted with the principles Peter Brouwer THEORY OF XRF Getting acquainted with the principles Peter Brouwer First published in The Netherlands under the title Theory of XRF. Copyright
Experiment: Crystal Structure Analysis in Engineering Materials
Experiment: Crystal Structure Analysis in Engineering Materials Objective The purpose of this experiment is to introduce students to the use of X-ray diffraction techniques for investigating various types
Physics 111 Homework Solutions Week #9 - Tuesday
Physics 111 Homework Solutions Week #9 - Tuesday Friday, February 25, 2011 Chapter 22 Questions - None Multiple-Choice 223 A 224 C 225 B 226 B 227 B 229 D Problems 227 In this double slit experiment we
Microscope Lab Introduction to the Microscope Lab Activity
Microscope Lab Introduction to the Microscope Lab Activity Wendy Kim 3B 24 Sep 2010 http://www.mainsgate.com/spacebio/modules/gs_resource/ CellDivisionMetaphase.jpeg 1 Introduction Microscope is a tool
- the. or may. scales on. Butterfly wing. magnified about 75 times.
Lecture Notes (Applications of Diffraction) Intro: - the iridescent colors seen in many beetles is due to diffraction of light rays hitting the small groovess of its exoskeleton - these ridges are only
It has long been a goal to achieve higher spatial resolution in optical imaging and
Nano-optical Imaging using Scattering Scanning Near-field Optical Microscopy Fehmi Yasin, Advisor: Dr. Markus Raschke, Post-doc: Dr. Gregory Andreev, Graduate Student: Benjamin Pollard Department of Physics,
STM and AFM Tutorial. Katie Mitchell January 20, 2010
STM and AFM Tutorial Katie Mitchell January 20, 2010 Overview Scanning Probe Microscopes Scanning Tunneling Microscopy (STM) Atomic Force Microscopy (AFM) Contact AFM Non-contact AFM RHK UHV350 AFM/STM
UNIVERSITY OF SOUTHAMPTON. Scanning Near-Field Optical Microscope Characterisation of Microstructured Optical Fibre Devices.
UNIVERSITY OF SOUTHAMPTON Scanning Near-Field Optical Microscope Characterisation of Microstructured Optical Fibre Devices. Christopher Wyndham John Hillman Submitted for the degree of Doctor of Philosophy
Scanning He + Ion Beam Microscopy and Metrology. David C Joy University of Tennessee, and Oak Ridge National Laboratory
Scanning He + Ion Beam Microscopy and Metrology David C Joy University of Tennessee, and Oak Ridge National Laboratory The CD-SEM For thirty years the CD-SEM has been the tool for metrology But now, as
NATIONAL NETWORK OF ELECTRON MICROSCOPY RNME. NETWORK MANAGEMENT MODEL a ARTICULATION AND GENERAL OPERATION. (English translation draft)
NATIONAL NETWORK OF ELECTRON MICROSCOPY RNME NETWORK MANAGEMENT MODEL a ARTICULATION AND GENERAL OPERATION (English translation draft) 1. Introduction 2 2. Objectives 2 3. Constitution 2 4. Organization
Physics 30 Worksheet # 14: Michelson Experiment
Physics 30 Worksheet # 14: Michelson Experiment 1. The speed of light found by a Michelson experiment was found to be 2.90 x 10 8 m/s. If the two hills were 20.0 km apart, what was the frequency of the
Scanning Electron Microscopy Services for Pharmaceutical Manufacturers
Scanning Electron Microscopy Services for Pharmaceutical Manufacturers Author: Gary Brake, Marketing Manager Date: August 1, 2013 Analytical Testing Laboratory www.atl.semtechsolutions.com Scanning Electron
Biomedical & X-ray Physics Kjell Carlsson. Light Microscopy. Compendium compiled for course SK2500, Physics of Biomedical Microscopy.
Biomedical & X-ray Physics Kjell Carlsson Light Microscopy Compendium compiled for course SK2500, Physics of Biomedical Microscopy by Kjell Carlsson Applied Physics Dept., KTH, Stockholm, 2007 No part
LIFE SCIENCE I TECHNICAL BULLETIN ISSUE N 11 /JULY 2008
LIFE SCIENCE I TECHNICAL BULLETIN ISSUE N 11 /JULY 2008 PARTICLE CHARACTERISATION IN EXCIPIENTS, DRUG PRODUCTS AND DRUG SUBSTANCES AUTHOR: HILDEGARD BRÜMMER, PhD, CUSTOMER SERVICE MANAGER, SGS LIFE SCIENCE
Atomic Force Microscopy. Long Phan Nanotechnology Summer Series May 15, 2013
Atomic Force Microscopy Long Phan Nanotechnology Summer Series May 15, 2013 1 World s Smallest Movie 2 Outline What is AFM? How does AFM Work? 3 Modes: Contact mode Non contact mode Tapping mode Imaging
Acoustic GHz-Microscopy: Potential, Challenges and Applications
Acoustic GHz-Microscopy: Potential, Challenges and Applications A Joint Development of PVA TePLa Analytical Systems GmbH and Fraunhofer IWM-Halle Dr. Sebastian Brand (Ph.D.) Fraunhofer CAM Fraunhofer Institute
Scanning Near-Field Optical Microscopy for Measuring Materials Properties at the Nanoscale
Scanning Near-Field Optical Microscopy for Measuring Materials Properties at the Nanoscale Outline Background Research Design Detection of Near-Field Signal Submonolayer Chemical Sensitivity Conclusions
5. Scanning Near-Field Optical Microscopy 5.1. Resolution of conventional optical microscopy
5. Scanning Near-Field Optical Microscopy 5.1. Resolution of conventional optical microscopy Resolution of optical microscope is limited by diffraction. Light going through an aperture makes diffraction
Laboratory #3 Guide: Optical and Electrical Properties of Transparent Conductors -- September 23, 2014
Laboratory #3 Guide: Optical and Electrical Properties of Transparent Conductors -- September 23, 2014 Introduction Following our previous lab exercises, you now have the skills and understanding to control
Tecnai on-line help Working with a FEG 1 FEG_A4.doc Software version 2
Tecnai on-line help Working with a FEG 1 Tecnai on-line help manual -- Working with a FEG Table of Contents 1 Introduction...2 2 FEG Safety...2 2.1 The column valves...2 3 FEG States...3 4 Starting the
The Physics of Energy sources Renewable sources of energy. Solar Energy
The Physics of Energy sources Renewable sources of energy Solar Energy B. Maffei [email protected] Renewable sources 1 Solar power! There are basically two ways of using directly the radiative
Optical Communications
Optical Communications Telecommunication Engineering School of Engineering University of Rome La Sapienza Rome, Italy 2005-2006 Lecture #2, May 2 2006 The Optical Communication System BLOCK DIAGRAM OF
Electromagnetic Radiation (EMR) and Remote Sensing
Electromagnetic Radiation (EMR) and Remote Sensing 1 Atmosphere Anything missing in between? Electromagnetic Radiation (EMR) is radiated by atomic particles at the source (the Sun), propagates through
