JEOL JXA-8200 Superprobe

Similar documents
Electron Probe Micro-Analysis (EPMA)

Task 3: Actinide targets properties after irradiation

EMSE Weak-Beam Dark-Field Technique

JSM-7800F Field Emission Scanning Electron Microscope

Microanalysis with high spectral resolution: the power of QUANTAX WDS for SEM

Wavelength-dispersive X-ray fluorescence spectrometer

The principles and practice of electron microscopy

Physical structure of matter. Monochromatization of molybdenum X-rays X-ray Physics. What you need:

3. EXPERIMENTAL PROCEDURE

What is SEM? TM-1000 Tabletop Microscope

Observation in the GB (Gentle Beam) Capabilities

EBSD Basics EBSD. Marco Cantoni 021/ Centre Interdisciplinaire de Microscopie Electronique CIME. Phosphor Screen. Pole piece.

Microstructural Characterization of Materials

X-ray Diffraction (XRD)

Carnegie Mellon MRSEC

Examination of Analytical Conditions for Trace Elements Based on the Detection Limit of EPMA (WDS)

TEM and Electron Diffraction Keith Leonard, PhD (1999) U. Cincinnati

CHAPTER 7 MICRO STRUCTURAL PROPERTIES OF CONCRETE WITH MANUFACTURED SAND

Wavelength Dispersive XRF Spectrometer

High-Energy Resolution Microcalorimeter EDS System for Electron Beam Excitation

EBSD Electron BackScatter Diffraction Principle and Applications

Diffraction Basics. The qualitative basics:

This lecture is part of the Basic XRD Course.

S2 RANGER LE: Analysis of Light Elements in Cement, Slags and Feldspar

X-Ray Fluorescence Lab Report

ATTACHMENTES FOR APD 2000 PRO POWDER X-RAY DIFFRACTOMETER. Monochromators

Image Formation and Interpretation

Growth Of TiO 2 Films By RF Magnetron Sputtering Studies On The Structural And Optical Properties

Identification of Crystal Structure and Lattice Parameter. for Metal Powders Using X-ray Diffraction. Eman Mousa Alhajji

METHOD FOR IMPROVING FIB PREPARED TEM SAMPLES BY VERY LOW ENERGY Ar + ION MILL POLISHING

INDEX DETAILED. STP292-EB/Jan. 1962

RIX3100. Fully Automated Sequential X-ray Spectrometer System. Product Information

Formation of High-quality Aluminum Oxide under Ion Beam Irradiation

Physics 6180: Graduate Physics Laboratory. Experiment CM5: X-ray diffraction and crystal structures

Visualization of Nano-precipitate in Low-alloy Steel by Using Energy-filtered Transmission Electron Microscopy

Advanced Methods for Materials Research. Materials Structure Investigations Materials Properties Investigations

The object of this experiment is to test the de Broglie relationship for matter waves,

This experiment is included in the upgrade packages: XRC 4.0 X-ray characteristics and XRS 4.0 X-ray structural analysis.

Introduction to Electron Backscattered Diffraction. TEQIP Workshop HREXRD Feb 1 st to Feb 5 th 2016

Installation of a Scanning Electron Microscope in the Hot-cell Laboratory of NRG Petten

Supporting Information

Neutron Detector development at the ILL Based on 3 He and alternative convertors

INGE Engineering Materials. Chapter 3 (cont.)

Analytical characteristics of a multilayer dispersion element (2d = 60 A) in the determination of fluorine in minerals by electron microprobe

ENERGY-DISPERSIVE X-RAY FLUORESCENCE ANALYSIS OF MONO- AND POLYCRYSTALS OF SELENIDE SPINELS BY FUNDAMENTAL PARAMETER METHOD

Fundamentals of X-ray diffraction and scattering

Practical 2P8 Transmission Electron Microscopy

Crystallographic Textures Measurement

Application of Scanning Electron Microscope to Dislocation Imaging in Steel

Electron Microscopy Sciences

XRF DRIFT MONITORS DATA CALIBRATION MATERIAL

Transmission Electron Microscopy (TEM) Prof.Dr.Figen KAYA

ElvaX ProSpector in Exploration & Mining

UNIT V -CRYSTAL STRUCTURE

A NEW APPROACH TO STUDYING CAST CB2 STEEL USING SLOW AND VERY SLOW ELECTRONS

GSA Data Repository

UNIVERSITY OF OSLO. Faculty of Mathematics and Natural Sciences

A Parametric Study on the Electrodeposition of Copper Nanocrystals on a Gold Film Electrode. Andrea Harmer Co-op term #1 April 25, 2003

Summary Report Report Written By: Wesley Powell (MS Industrial Engineering, BS Materials Engineering) SEM/EDS Operator: Wesley Powell

SEM (SCANNING ELECTRON MICROSCOPE)

Synthesis and Characterization of Cadmium Sulfide Nanoparticles

Synchrotron X-Ray Topography Measurements on 4H-SiC Epitaxial Layer

Reduction of the Sample Size in the Analysis of Rock by EDXRF

Instytut Fizyki Doświadczalnej Wydział Matematyki, Fizyki i Informatyki UNIWERSYTET GDAŃSKI

RESPONSIVITY IMPROVEMENT OF PHOTOCONDUCTIVE INFRARED DETECTROS LA.ELFALLAL, A.H.ZAKI (ARE Armed Forces)

Lesson 1 X-rays & Diffraction

Scanning Electron Microscope & Surface Analysis. Wageningen EM Centre Marcel Giesbers

UNIVERSITY OF OSLO. Faculty of Mathematics and Natural Sciences

The first measurement will be performed with a sample temperature of 35 by executing the following steps:

Comparison of Off-peak vs. MAN vs. Nth Point background measurements John Donovan,

Spatially resolved crystal domain identification: Implementing Laue-mapping technique on the M4 TORNADO spectrometer

LiNi 0.5 Mn 1.5 O 4 porous nanorods as high-rate and long-life cathode for Li-ion batteries

Supporting Information. Solution-Processed 2D PbS Nanoplates with Residual Cu 2 S. Exhibiting Low Resistivity and High Infrared Responsivity

Structural reorganization on amorphous ice films below 120 K revealed by near-thermal (~1 ev) ion scattering

ZEISS Mineralogic Mining Iron Oxide Analysis by Automated Mineralogy. Technology Note

Atomic Densities. Linear Density Number of atoms per length whose centers lie on the direction vector for a specific crystallographic direction.

ANALYTICAL PERFORMANCE OF A HANDHELD EDXRF SPECTROMETER WITH MINIATURE X-RAY TUBE EXCITATION

Supporting Information for The Influence of the CTAB Surfactant on the Colloidal Seed-Mediated Synthesis of Gold Nanorods

LECTURE 8. Dr. Teresa D. Golden University of North Texas Department of Chemistry

VOLUME FRACTION ANALYSIS

Stress Mitigation of X-ray Beamline Monochromators using a Topography Test Unit

An anti-galvanic replacement reaction of DNA templated silver. nanoclusters monitored by light-scattering technique

9/29/2014 8:52 PM. Chapter 3. The structure of crystalline solids. Dr. Mohammad Abuhaiba, PE

Supporting Information

Atomic Densities. Linear Density. Planar Density. Linear Density. Outline: Planar Density

Lecture C4b Microscopic to Macroscopic, Part 4: X-Ray Diffraction and Crystal Packing

9/28/2013 9:26 PM. Chapter 3. The structure of crystalline solids. Dr. Mohammad Abuhaiba, PE

High Resolution XPS Study of a Thin CoO 111 Film Grown on Co 0001

S8 TIGER Series 2. Lab Report XRF 144. Innovation with Integrity. Accurate Quality Control of Tool Steels XRF

Kinematical theory of contrast

QEMSCAN. XPS Consulting & Testwork Services 6 Edison Road, Falconbridge, Ontario, Canada P0M 1S0. Process Mineralogy

The application of scanning electron beam anomalous transmission patterns in mineralogy

THE DIFFERENTIATION OF FLOAT GLASS USING REFRACTIVE INDEX AND ELEMENTAL ANALYSIS: COMPARISONS OF TECHNIQUES

X-Ray-Fluorescence Analysis Major Eiements in Silicate Minerals

What is a positron moderator?

Materials Lab 1(MT344) X-ray Diffractometer Operation and Data Analysis. Instructor: Dr. Xueyan Wu ( 吴雪艳 )


9/16/ :30 PM. Chapter 3. The structure of crystalline solids. Mohammad Suliman Abuhaiba, Ph.D., PE

EDX 600. Atomic Absorption Spectrometry

New Advances using Handheld XRF Technology for the Prevention of Flow-Accelerated Corrosion (FAC)

Transcription:

JEOL JXA-8200 Superprobe Electron gun Liq N 2 for EDS Electron gun Condenser lens Optical Microscope Optical Microscope EDS WDS SE Liq N 2 EDS BSE Objective lens WDS Sample exchange chamber Stage High vacuum Perpendicular geometry

Back-scattered electron detector Top view of specimen

Compositional and topographic imaging with BSE A+B Compositional mode A-B Topographic mode

Secondary electrons Specimen electrons mobilized by electron beam through inelastic scattering Secondary electrons have lower energy compared to backscattered electrons (useful in studying surface topography)

Secondary electron detector Side view of specimen

Secondary electron imaging -ve Faraday cage bias less SE less topographic contrast +ve Faraday cage bias more SE better topographic contrast

Cathodoluminescence Light generated from sample through electron beam interaction Band gap energy, E gap, is a property of the semiconductor Trace impurities change E gap by adding additional energy states in the band gap

Cathodoluminescence detector JXA-733 Optical microscope light turned off Front view Side view Photomultiplier for secondary electron imaging is used as CL detector Optical arrangement is the same as for the optical microscope

Cathodoluminescence spectrometer Optical microscope camera (not used) Optical microscope light (turned off) JXA-8200 Optical spectrometer

Integrated CL and X-ray CL spectrum spectrometry Intensity Energy 3 band CL map 3 element X-ray map Scatter plot CL wavelength band may be correlated with an element

Wavelength Dispersive Spectrometer (WDS) WDS WDS detector crystal

WDS Analyzing crystal Flipping motor

Bragg s Law d = lattice spacing q = angle of diffraction nl = 2d sin q = path length ABC n = order of reflection (any integer)

First and second order reflections Same element n=1 n=2 q 1 q 2 D F A C B E 1l = 2d sinq 1 2l = 2d sinq 2 =ABC =DEF path DEF = 2* path ABC

Diffraction angle l Different elements 1 2 (Element 1) (Element 2) l q 1 q 2 nl 1 = 2d sinq 1 nl 2 = 2d sinq 2 Diffraction angle changes with wavelength being diffracted (for the same order of reflection, n)

WDS Analyzing crystals with different d spacings Name 2d (Å) Type Elements usually analyzed LDEC 98 Ni/C Multi-layer B-O (K ), optimized for C analysis STE 100.4 Pb stearate B-O (K ), optimized for C analysis LDE1 59.8 W/Si Multi-layer C-F (K ), optimized for O analysis TAP 25.8 Thallium acid phthalate Na-P (K ); Cu-Zr (L ); Sm-Au (M ) PET 8.742 Pentaerythritol S-Mn (K ); Nb-Pm (L ); Hg-U (M ) LIF 4.028 Lithium fluoride Ti-Rb (K ); Ba-U (L )

WDS detector: Proportional counter Count rate depends on bias and gas used Tungsten collection wire set at 1-3 kv bias Flow counter: 90% Ar +10% CH 4 (P-10); poly-propylene window Sealed counter: Xe or Kr; Be window

Bias in proportional counter best count rate

Counting efficiency of gas Heavy elements Light elements

WDS signal processing Single channel analyzer (SCA) and pulse height analysis (PHA) window baseline Only pulses in this voltage interval are counted

WDS Focusing geometry angle of diffraction take-off angle L = nl.r/d

Curved diffracting crystals Johansson type bending curvature: 2R polished and ground to R R Johan type only bent to 2R, not ground FWHM of fully focusing Johansson-type crystal ~10 ev Some defocusing in Johan-type, but resolution is not compromised

Defocusing in beam-rastered WDS X-ray maps

WDS: changing the angle of diffraction or, n 2 l 1 = 2d sin q 2 L 2 = n 2 l 1.R/d

Theoretical and actual limits of spectrometer movement 2R L 0

EPMA: Quantitative analysis procedure Sample preparation Qualitative analysis with EDS Standard intensity measurement (calibration) Measurement of X-ray intensities in the specimen Data reduction through matrix corrections

Sample preparation Sample cut and mounted in epoxy Polished first with coarse SiC paper, then with alumina grit slurry (final size: 0.25 mm) 1 Washed with water in ultrasonic cleaner 2 Dried with blow duster and air Carbon coated 3 1: diamond paste or colloidal silica for some samples; dry polishing paper for water-soluble samples 2: ethanol may be used sparingly; cleaned with blow duster and cloth for samples that dissolve in water 3: for insulators; if standards are coated, however, all samples must be coated

Sample prep: carbon coating Sample chamber (bell jar)

MIT OpenCourseWare http://ocw.mit.edu 12.119 Analytical Techniques for Studying Environmental and Geologic Samples Spring 2011 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms.