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section:
Introduction Fundamentals of the TEM technique Beam-sample interaction The Analytical TEM Detector Protection Qualitative Analysis Quantitative Analysis Microanalysis Examples (1) Microanalysis Examples (2) Microanalysis Examples (3) Summary
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Detector Protection
If a specimen support grid passes under the beam or the sample is viewed
under low magnification conditions where the whole grid is exposed to high
beam currents, a large flux of backscattered electrons is generated. The
close proximity of the detector to the sample can cause an excess of these
backscattered electrons to enter the detector. This not only overloads the
electronics but may also deposit excess charge in the detector. As a result,
the detection system is effectively paralyzed and may take many minutes to
recover.
It is possible
to initiate automatic detector withdrawal if counts exceed an acceptable
value. However, this can cause vibration and image distortion, and due to
the fact that the detector actually protrudes into the polepiece, it may
also change the stigmation conditions of the microscope at high
magnifications. Another option is to use a shutter between the sample and
the crystal that closes when a high count rate is exceeded (Figure 4). The
shutter does not cause the mechanical disturbance or stigmation problems
associated with withdrawal and will prevent overload of the detection
system. The detector is therefore ready to use immediately on return to
normal analysis conditions and analysis throughput is improved.
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