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The New Tescan LVSTD Detector

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True Everhart-Thornley Secondary Electron (SE) Imaging in Low Vacuum conditions

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SE imaging of non-conductive and 'wet' samples with coating or special sample preparation

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High resolution images of fine surface topography

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Compact design allows fast and easy interfacing to any of the Vega SEM models

 

Tescan's unique patented design utilizes a standard Everhart-Thornley secondary electron detector housed in a separately pumped detector chamber. This innovative design keeps the SE detector under good vacuum and provides several benefits over conventional VPSE detectors that rely on gas amplification (G-A) effects:

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The LVSTD detector works very well at all scan rates, including TV-rate - just like your normal E-T secondary electron detector. VPSE detectors that rely on G-A effects don't work well (or at all) at fast scan rates.

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The LVSTD detector behavior does not depend on gas pressure, allowing you to optimize the pressure to suit your sample, not the detector.

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G-A detector efficiency is worst at the gas pressures that are optimum for VP imaging.

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The LVSTD detector behavior is not sensitive to gas species, allowing you to optimize the gas to suit your sample, not the detector

 

University of York LVSTD Poster presented at EMAG '03, Oxford, UK (right click to download pdf, approx. 2MB)

 

 

 

 
Comparison of BSE and VPSE Images acquired with the Tescan LVSTD Detector - All samples were imaged in their natural state (Click to enlarge)


Earwig Claw imaged at 80Pa


Automotive Valve imaged at 80Pa.


Carbon film, only 3nm thick, deposited through a square grid onto a silicon substrate, demonstrating true SE detection and excellent surface contrast of the LVSTD detector.

 
 
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