447 25
DTSA-II Monte Carlo simulation
40Cu-60Au
E 0 = 20 keV
4 mm gas path lengthHigh_vacum_40Cu-60Au_20keVHigh_vacum_40Cu-60Au_20keV53Pa_H2O_40Cu-60Au_20keV16x1200Pa_H2O_40Cu-60Au_20keV1600Pa_H2O_40Cu-60Au_20keV
133Pa_H2O_40Cu-60Au_20keV53Pa_H2O_40Cu-60Au_20keV16x
400Pa_H2O_40Cu-60Au_20keV800Pa_H2O_40Cu-60Au_20keVH 2 O53 Pa H 2 O
High vacuum1600 Pa H 2 O
1200 Pa H 2 O
800 Pa H 2 O
400 Pa H 2 O
133 Pa H 2 O
53 Pa H 2 O
High vacuumScaled to AuMPhoton energy (eV)Photon energy (eV)CountsRelative Counts16000
14000
12000
10000
8000
6000
4000
2000
0
0 500 1000 1500 20002500300035004000450050000 500 1000 1500 2000250030003500400045005000. Fig. 25.7 DTSA-II Monte Carlo simulations of the specimen and gas scattering conditions of. Fig. 25.6. Upper plot: high vacuum and 53 Pa
(4 mm GPL, H 2 O). Lower plot: high vacuum and various pressures from 53 Pa to 1600 Pa
EDS
detectorWindowCollimator &
electron trapFinal
lensChamber
wallBSEBSERemote X-raysSpecimen X-raysGreen =
Extent of
specimen
X-ray sources
NOT excluded
by collimatorSeveral mm Several mm. Fig. 25.8 Schematic diagram
showing the acceptance area of
the EDS collimator
25.1 · Gas Scattering Effects in the VPSEM