355 21
EDS
detectorwindowCollimator &
electron trapFinal
lensChamber
wallBSEAperture
scattering
Conventional SEM,
pathological scatteringSpectrum from high purity flat
scattering target, e.g., C, Ta,
surrounded by different materials,
e.g., Ag-epoxy, Ti, AlGreen =
Extent of
specimen
X-ray sources
NOT excluded
by collimatorMulti-material “flat scatter” test specimen. Fig. 21.15 Schematic
diagram of the “in-hole”
configuration with a pure
element target placed at the
center of a multi-material target
Carbon
E 0 = 20 keV
12% deadtime, 112 kHz
500s (12,500 nA-s)
0.1 – 20 keV integral
= 56 million countsAg0 1.0 2.0 3.0 4.0 5.0
Photon energy (keV)6.07.0 8.09.0FullamplainC_20kV25nAME
112kHz12DT500s10kx_02-09-0910.0TiSi K-edgeC K
C K + C KCounts. Fig. 21.16 Measurement of
high purity C surrounded by Ag
(doped epoxy) and titanium; no
significant signals for Ag or Ti are
observed
21.4 · Pathological Electron Scattering Can Produce “Trace” Contributions to EDS Spectra