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    ELECTRON

    DETECTORS FOR SEMPRESENTED BY

    Engr. Naeem Basra(MM-06, 2006-07)

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    What is a SEM?

    Is a microscope that uses electrons rather than light

    to form an image and to examine objects on a very finescale.

    This examination can yield the following information:

    Topography surface features

    Morphology shape and size

    Composition elements and compounds/ relativeamount of them

    Crystallographic information how the atoms are arranged in the sample

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    How the SEM Works

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    Microstructure evaluationSmall feature measurements

    Fracture mode preliminary identification

    Grain size

    Corrosion failure inspection

    Surface contamination evaluationChemical Composition

    Crystallographic information

    Applications

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    Interaction between electron beam and sampleThe interactions may be elastic or inelastic.

    The elastic interactions:incident electrons and nucleus a large-angle deflection

    of incident electrons. little energy loss

    The inelastic interactions: incident electrons andorbital shell electrons a small-angle deflectionof incident electrons. heavy energy loss

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    Secondary electrons (SE)

    Generated when a primary electron dislodges a

    specimen electron from the specimen surface. Produced by inelastic interactions. SE energy level is only 3 ~ 5 eV. Can be easily collected

    The maximum escape depth is about 5 nm inmetal and 50 nm in insulators.

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    Backscattered electrons (BSE)

    Produced by elastic interactions. BSE energy level is about 60 ~80 % of incident

    one. Special detector is required to collect BSE. The maximum escape depth varies inversely with

    the average atomic number,

    the range from a fraction of micrometer to severalmicrometers.(Larger atomic number, larger escape depth).

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    X-rays

    Generated when electron are dislodge fromspecific orbits of an atom in the specimen.

    Large escape depth due to difficulty of x-rayabsorption

    Energy and wavelength of x-ray can be used

    for chemical analysis.1.energy-dispersive spectroscopy, EDS,2.wavelength-dispersive spectroscopy, WDS

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    Electron Detectors

    Hi hi SEM

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    Hitachi SEMDetectors

    View from inside, looking up obliquelyima e taken b handheld di ital camera

    Annular

    BSEdetector

    IRChamber

    scope

    E-T SEdetector

    EDS

    detector

    ESED

    detector

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    Detectors used to amplify the signalrather than detected secondary and

    backscattered electrons directly

    i.e. Electrons Photons Electrons

    Backscattered electrons are high energy

    (i.e. 1 - 40 keV) Secondary electrons are low energy

    (~0 - 50 eV)

    Detecting electrons

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    Must use different detectors to collect thebackscattered and secondary electronsignals.

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    Detecting backscattered

    electrons

    Two specialized detectors are used todetect BSE

    Detector sits directly beneath theobjective lens.

    Large surface area to maximize collection

    efficiency.

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    Backscatter electron detector

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    Scintillator detectors

    These comprise a scintillator (phosphor)with a light pipe and a photomultiplier

    Fast response time and high gain, which

    makes them suitable for use at TV rates.

    Bulky and may restrict the workingdistance of the microscope.

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    Solid state detectors

    Si p-n junction which forms electron-holepairs on the impingement of a BSE.

    A reverse bias separates the electron holepairs, giving rise to a detectable current.

    Much smaller than a scintillator

    Cheap to make Slow response time makes them unsuitable

    for operation at TV scan rates

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    Limitations

    Slow response time

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    Detecting secondary electrons

    used an Everhardt-Thornley detector

    based on a scintillator-photomultipliersystem

    Energy of the secondary electrons is toolow to be detected directly

    accelerated by applying a bias of ~ +10kV to a thin Al film on the scintillator

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    A collector grid which is biased to ~200 Vis also used to attract the secondaryelectrons

    This collector screens the scintillator fromthe incident beam and improves thecollection efficiency of the detector

    Light is converted into pulses of electronsin the photomultiplier which are used tomodulate the intensity on a CRT

    Detecting secondary electrons

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    Secondary ElectronDetector

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    THANKS