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1. Free electrons are created in the Electron Gun by heating a tungsten filament (Cathode) 2. Electrons are accelerated down the electron optical column by means of a high voltage potential at the Anode Energy Dispersive X-ray Analyzer: 3. The electron flux is shaped into a beam by the Condenser Lenses x-rays resolved on the basis of their energies 4. The beam current is controlled by the Beam Regulation Aperture (and the condenser lenses) 5. The beam current is measured with, or permitted down the column by removing, the Faraday Cup 6. Beam ellipticity is corrected by the Stigmator 7. The beam is scanned or fixed into a probe spot by the Final Condensing (“objective”) Lens diffraction crystal 8. The beam impacts the sample, giving rise to various signals including secondary electrons, backscattered electrons, x-rays, and cathodoluminescent energy. Current absorbed by the sample also can be imaged. x-rays sample scintillation counter Wavelength Dispersive Spectrometer x-rays resolved by diffraction, through a regular periodic solid, to a gas-filled counter Secondary Electron Detector: detects low-energy electrons liberated from near the sample surface, providing an image of sample topography Backscattered Electron Detector detects higher-energy electrons “bounced out” of the sample, providing an image based on average atomic mass (related to density); hence, the image is based on the compositions of Absorbed Current:Meter constituent components images electrical conductivity within the sample Press “Back” to return to the web page