355 21
EDS
detector
window
Collimator &
electron trap
Final
lens
Chamber
wall
BSE
Aperture
scattering
Conventional SEM,
pathological scattering
Spectrum from high purity flat
scattering target, e.g., C, Ta,
surrounded by different materials,
e.g., Ag-epoxy, Ti, Al
Green =
Extent of
specimen
X-ray sources
NOT excluded
by collimator
Multi-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 counts
Ag
0 1.0 2.0 3.0 4.0 5.0
Photon energy (keV)
6.07.0 8.09.0
FullamplainC_20kV25nAME
112kHz12DT500s10kx_02-09-09
10.0
Ti
Si K-
edge
C K
C K + C K
Counts
. 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