Electron Microprobe Analysis 1 Nilanjan Chatterjee, Ph.D. Principal Research Scientist
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1 Electron Microprobe Analysis 1 Nilanjan Chatterjee, Ph.D. Principal Research Scientist Massachusetts Institute of Technology Electron Microprobe Facility Department of Earth, Atmospheric and Planetary Sciences Massachusetts Institute of Technology
2 Uses of the EPMA 2 Spot mode operation for quantitative analysis: Micron-scale, complete chemical analysis Be to U (10-50 ppm under favorable conditions) Raster mode operation for high resolution imaging: Back-scattered electron: composition and topography Secondary electron: topography Cathodoluminescence (light): trace elements, defects X-ray map: spatial distribution of elements
3 An example: Compositional imaging with back-scattered electrons 3 Back-scattered electron Plane polarized transmitted light Low-Z elements High-Z Polished surface Function of composition Thin section Function of optical properties
4 Qualitative analysis 4 Visual characterization of phases in image (shape, size, surface topography, etc.) Qualitative identification of elements in each phase
5 Semi-quantitative analysis 5 Quick and approximate concentration measurement at a spot Elemental mapping of a surface to determine spatial distribution of elements
6 Quantitative analysis 6 Complete chemical analysis of a micron-sized spot to determine concentration of all elements Concentration mapping to determine the abundance of all elements at every pixel of an image
7 JEOL JXA-8200 Superprobe 7 Condenser lens Electron gun Optical Microscope LN 2 SE EDS Objective lens BSE Stage WDS High vacuum
8 Electron emitting source: Tungsten hairpin 8 Cathode: Filament at negative potential Tungsten has a high melting point and a low work-function energy barrier; heated by filament current, i f, until electrons overcome the barrier Wehnelt Cylinder at a slightly higher negative potential than the filament because of the Bias Resistor Bias voltage (V bias ) automatically adjusts with changes in i e to stabilize emission; the grid cap also focuses the electron beam Anode: Plate at ground potential Self-biased thermionic electron gun Potential difference (accelerating voltage, V 0 ) causes electron emission (current, i e )
9 Electron probe parameters 9 Sample Accelerating voltage, V 0 (V 0 of 15 kv generates electron beam with 15 kev energy) Final beam current, or probe current, i p Final beam diameter, or probe diameter, d p Final beam convergence angle, or probe convergence angle, a p
10 d p (nm) 10 Different electron sources W hairpin Field Emission LaB 6 Probe diameter decreases with decrease in Probe current increase in Accelerating voltage W > LaB6 > Field Emission source Higher probe current improves signal but results in poorer image resolution Tungsten hairpin, 15 kv, 10 na, d p 100 nm
11 Depth of focus 11 Large depth of focus Small depth of focus
12 Spatial resolution: electron interaction volume 12 Vertical electron beam, probe diameter = 0.1 mm Horizontal sample surface 1 2 Depth (mm) mm 2.25 mm Low atomic number: large tear-drop shape Monte Carlo simulations of electron trajectories in the sample High atomic number: small hemisphere Width of interaction volume >> probe diameter (interaction volume can be reduced by reducing the probe diameter using a lower accelerating voltage)
13 Electron interaction depth (range) 13 R : Kanaya-Okayama electron range E : beam energy A : atomic weight r : density Z : atomic number Electron range increases as E increases, and decreases as r and rz increase E.g., at 20 kv, R = 4.29 mm in Carbon (Z = 6, A = 12.01, r = 2.26 g/cc) R = 0.93 mm in Uranium (Z = 92, A = , r = g/cc)
14 Electron interaction depth (range) 14 Electron range increases as E increases, and decreases as r and rz increase
15 Electron beam 15
16 Spatial resolution for different signals kev, W filament diameter ~150 nm 150 nm 450 nm Fluorescence of CoKa by CuKa ~60 mm (not to scale) CuKa ~1 mm CuLa ~1.5 mm Production volume for different signals is different The onion shell model: Cu-10%Co alloy
17 Spatial resolution for cathodoluminescence 17 2 mm Gallium Nitride
18 Electron-specimen interactions: Elastic scattering 18 Back-scattered electron
19 Electron-specimen interactions: Inelastic scattering 19 Inner shell interactions: Characteristic X-rays Secondary electron Outer shell interactions: Continuum X-rays Secondary electron Cathodoluminescence
20 Back-scattered electron (BSE) 20 Beam electrons scattered elastically at high angles Commonly scattered multiple times, so energy of BSE beam energy
21 Electron backscatter coefficient 21 Fraction of beam electrons scattered backward high-z W Au (74) (79) low-z K (19) Si (14) (Z) Large differences between high- and low-atomic number elements Larger differences among low-z elements than among high-z elements
22 Back-scattered electron detector 22 Objective Lens BSE detector A B
23 Back-scattered electron detector 23 Solid-state diode
24 Compositional and topographic imaging with BSE 24 A+B Compositional mode A-B Topographic mode
25 Secondary electron (SE) 25 Specimen electrons mobilized by beam electrons by inelastic scattering (both outer and inner shell interactions) Emitted at low energies (typical: <10 ev) (recall BSE have high energies up to that of the electron beam)
26 Secondary electron detector 26 Located on the side wall of the sample chamber
27 Secondary electron detector 27 (+ve bias)
28 Imaging with the Everhart-Thornley detector 28 Negative Faraday cage bias only BSE Positive Faraday cage bias BSE + SE Surfaces in direct line of sight are illuminated All surfaces are illuminated
29 Cathodoluminescence (CL) 29 Caused by inelastic scattering of beam electrons in semiconductors Filled valence band is separated from an empty conduction band by E gap, characteristic of the compound Electron recombines with the valence band to generate light with energy E gap Electron beam interacts: Valence electron is promoted to the conduction band Trace element impurities produce additional energy levels outside the conduction band, and enable other electron transitions; emitted light has different colors with energies E E gap
30 Cathodoluminescence spectrometer 30 Optical microscope camera (not used) Optical microscope light (turned off) Optical spectrometer (CCD array detector)
31 Intensity Cathodoluminescence spectrum 31 Mn Light wavelength (nm) Dolomite with trace of Mn
32 Hyperspectral CL imaging 32 A continuous (l = 200 to 950 nm) light spectrum is collected at each point of the image area Intensity of nm light: counts (blue shades) Intensity range of nm light: counts (red shades) Intensity of nm light: counts (green shades) Intensity of nm light: counts (red shades)
33 Hyperspectral CL imaging 33 Intensity range of light (all wavelengths) in grey scale Black: no light White: maximum intensity Intensity range of nm light in multicolor scale: Blue ( 0 counts): no light Red (9884 counts): maximum intensity
34 The X-ray spectrum 34 Characteristic X-rays Continuum X-rays
35 Energy Dispersive Spectrometer (EDS) 35 EDS detector: solid-state semiconductor, window and aperture Multichannel analyzer (MCA) processes the X-ray signal
36 Negatively biased surface repels electrons Energy Dispersive Spectrometer (EDS) 36 electron hole X-ray A single crystal of silicon Pure Si is a semiconductor. But impurity of boron, a p-type dopant, makes it a conductor Lithium, an n-type dopant, counteracts the effect of boron and produces an intrinsic semiconductor Lithium-drifted silicon, or Si(Li), p-i-n detector
37 Mean Atomic Number Qualitative analysis with BSE and EDS ilmenite 37 hornblende plagioclase
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