PART 4 • DOPING AND THE TRANSISTOR
Doping and the Transistor
Diffusion
The oldest way to move dopant into silicon: heat and time
Implantation
The modern way: fire dopant atoms in as a beam of ions
The transistor
Wells, junctions, and a gate stack, put together
A CRYSTAL THAT BARELY CONDUCTS
The whole point of all that purity
Part 1 spent six units getting silicon to nine nines pure, because an impurity anywhere in the crystal is a defect you can't control. Doping flips that: once the crystal is flawless, a fab adds back a tiny, exact, deliberate amount of a different element, in only the spots it wants.
TWO FLAVORS
Pick your carrier
n-type
Phosphorus or arsenic donates a free electron to the lattice
p-type
Boron accepts an electron, leaving a mobile hole behind
Typical dose
As few as one dopant atom per 10,000 to 100,000 silicon atoms
CARRIERS
Majority and minority
THE P-N JUNCTION
Where two doped regions meet
Put p-type and n-type silicon side by side and the boundary between them becomes a p-n junction. Mobile carriers near the boundary diffuse across and cancel out, leaving a depletion region with almost no free carriers and a built-in electric field.
FROM JUNCTION TO TRANSISTOR
A MOSFET is built from junctions
A transistor's source and drain are doped regions of one type, sitting inside a well of the opposite type. That arrangement is two back-to-back junctions, held off by a gate. The rest of this part covers how a fab actually places that doping: diffusion, implantation, and the finished device.
UNIT 19 STUDY COMPLETE
Ready for the Fab Challenge?
You've covered why pure silicon needs controlled impurities, and what a p-n junction does.