Electrical systems
1924 De Broglie wave theory: electrons can move as particles or waves
1930 Knoll and Ruska first electromagnetic lens
Sources of electrons
- low electron emission
- as electrons are removed, the metal becomes more positive and resists giving up more electrons
cold process
heat tungsten 2200 Kelvin=>boils off electrons
3400K =>melts wire
FOR DIAGRAM OF BIASED CAP, SEE FIG 2.1
With resistor, makes the guard cap more negative, pushing the electrons closer to the filament, so more see the anode plate and come down column. Too much bias prevents the electrons from leaving the filament
Can increase the efficiency of current production compared to unbiased cap
==> isn't changing the number of electrons emitted, only the number that come down the column
Anode plate: electrons leave the filament with a charge usually less than
1 electron volt. See anode at very positive value compared to electron and
accelerate down the column. The difference between the filament current and
the anode plate is called the accelerating voltage. This ranges from
less than 1 eV to 30,000 eVolts (1-30 kV)
Filament saturation/longevity curves (FIG 2.3). Saturation is the point
of maximum electron emission at a minimum current or source temperature.
Increasing
the current to the source does not produce any more electrons--it sharply
decreases the lifetime of the filament.
The smaller the area from which the electrons are emitted, the smaller the spot to start and the brighter it is
--v-shaped standard, or pointed wire tip
--crystal tip
tungsten filament cheap and easy to use, replace
lanthanum hexaboride crystal on a wire (Fig2.6)
Pro Con longer life very expensive to replace smaller spot harder to saturate brighter emission needs very high vacuum better resolution
field emission cold cathode (Fig 2.7)
Pro Con very bright needs ultra-high vacuum smaller spot can't be retrofitted smaller energy spread unstable beam current long long life
LENSES
Electrons entering a magnetic field in a lens are deflected in direction but there is no change in velocity.
wrap wire around tube, get magnetic field inside, strongest along sides, weakest in the middle. Electrons entering the field are delected perpendicular and end up spiraling down the tube (Fig. 2.8).
To increase lens power:
1. more wire wraps2. more metal in casings
pole pieces to concentrate field into smaller area3. more current
Lens aberrations
Astigmatism: non symmetrical lens--Circles look like ovalsCorrection: add equal and opposite distortion from additional lenses, called stigmator coils. These are arranged around the lens in 2 sets of coilsChromatic aberration: different wavelengths focus at different distancesCorrection:Spherical aberration: electrons at edge don't focus at same spot as electrons in center1) Stabilize electron source2) Increase lens current
3) Use thinner sections in TEM since specimen interactions slow electrons down variably
Correction:1) Increase lens current2) Use aperture to prevent electrons from contributing to image
Aperatures: Metal disks with a center hole (Fig. 2.9)
1. Apertures limit the outer edge of lenses (can correct spherical aberration).2. Reduce the amount of illumination on sample.
3. Increase contrast by removing inelastically-scattered electrons (IN TEM)
4. Effect the depth of field
Column Configurations--SEM (Fig. 5.3)
TEM --lenses focus image on viewing screenSEM --lenses focus illumination spot on sample surface, image subsequently formed on view CRT outside column--lenses magnify image in floodbeam formed at sample and project on viewscreen within microscope column--illuminating spot is moved by magnetic coils deflecting beam aimed at sample.
--Magnification changes as area scanned is changed