Electron Sample Interactions
When the electron beam strikes the sample, both photon and electron signals are emitted
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Key Applications of Energy Dispersive X-Ray Spectroscopy (EDS)
• Near surface and bulk elemental information
• Particles and small area analysis
Strengths and Weaknesses
Strengths
- Quick, ‘first look’ analysis
- Versatile & inexpensive
- Quantitative for some samples (flat, polished, homogeneous)
Weaknesses
- Quantification
o samples must be flat, polished & homogeneous
- Size restrictions on samples
- Samples must be vacuum compatible
- Analysis (and coating) may spoil subsequent surface analysis
Wavelength Dispersive X-Ray Spectrometry (WDS)
X-Ray diffraction eq
nlamda=2dsin (theta)
lamda= wavelength of interest
d= interplanar spacing of the diffractor
(theta) angle of x-ray incidence
n= an integer
The wavelength of X-ray is measured which is related to the energy according to the Planck’s law:
E= h*c/ lamda
E= energy of xray photon
h=plancks constant 6.6262*10^34 Js
lamda= wavelength of xray photon
c= speed of light= 3.0*10^8
applications of xray diffraction
• Applications include
WDS vs EDS
• X-ray microanalysis in the scanning electron microscope is accomplished using EDS and/or WDS.
• EDS is more commonly applied due to its simplicity and speed.
• WDS offers an important and often critical refinement of EDS data by providing:
o Analysis for light elements with at least an order of magnitude higher sensitivity than available (ultra thin X-ray window) EDS instruments
o Resolution of severely overlapped spectrum peaks for improved element specificity
o Lowered detection limits over the entire periodic table
o More accurate quantitative analyses.
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