Semiconductor Electronics

On this page
  1. Direct answer
  2. What you must remember
  3. Following the junction through bias
  4. Where students slip
  5. Frequently asked questions
  6. Related topics

Direct answer

Silicon doped with phosphorus acquires spare conduction electrons; doped with boron it acquires holes; the junction between the two regions conducts one way only — and every device in this chapter grows from that junction. The band picture sets the rules (Si gap 1.1 eV, Ge 0.7 eV), the junction's one-way behaviour rectifies and regulates, and the device set — Zener, LED, photodiode, solar cell — carries the questions.

What you must remember

  • Bands: the valence band fills, the conduction band sits an energy gap Eg above; insulators have Eg > 3 eV, semiconductors near 1 eV (Si 1.1 eV, Ge 0.7 eV), and heat promotes electrons across the gap, leaving mobile holes behind — both carriers conduct.
  • Intrinsic silicon: electron and hole densities equal; extrinsic: pentavalent donors (P, As, Sb) give n-type with electrons majority; trivalent acceptors (B, Al, In) give p-type with holes majority; either way the crystal stays neutral overall.
  • Junction formation: majority carriers diffuse across, recombine, and leave a depletion region of immobile ions with a barrier potential — about 0.7 V for silicon, 0.2-0.3 V for germanium — where drift finally balances diffusion.
  • Forward bias narrows the depletion layer and lets a large diffusion current flow beyond the knee voltage; reverse bias widens it, leaving only a tiny minority-carrier saturation current until breakdown.
  • Rectification: one diode gives half-wave output; two diodes with a centre-tapped transformer give full-wave, and the ripple frequency doubles to 100 Hz on 50 Hz mains; a capacitor across the load smooths the ripple.
  • Zener diode: heavily doped, operated in reverse breakdown which is sharp and non-destructive — the standard voltage regulator.
  • Photodiode: reverse-biased; incident light generates carriers, so the reverse current grows with illumination — light detection, smoke alarms, optocouplers.
  • LED: forward-biased junction emitting photons on electron-hole recombination (GaAs, GaP and related compounds); solar cell: the same physics run as a generator, delivering an emf under light with no external bias.

Following the junction through bias

At equilibrium, majority-carrier diffusion across the fresh junction is exactly balanced by minority-carrier drift, and the depletion region's charged wall holds the barrier. Forward-bias it (positive to the p-side): the barrier lowers and the wall thins, majority electrons pour from n to p, holes from p to n, and current climbs steeply past the knee. Reverse-bias it and the wall grows taller and thicker: majority diffusion is extinguished outright, and the only current is the small, bias-insensitive drift of thermally generated minority carriers — a trickle that avalanches only at the designed Zener voltage. The asymmetry is absolute, and every application is a pose on it. The rectifier lets the forward half-cycles through and starves the reverse ones; in full-wave, the two diodes alternate by half-cycle and the ripple runs at double the mains frequency. The Zener exploits the breakdown rather than fearing it; the photodiode turns the reverse trickle into a light meter; the LED and solar cell run the same engine in opposite directions along the bias axis.

Where students slip

Majority-carrier naming trips first: an n-type sample still contains some holes — they are its minority carriers — and "n-type is negatively charged" is false, since donor ions in the lattice balance the donated electrons. Second, the depletion region contains immobile ions, not free charges; it is called depleted because its mobile carriers have recombined away. Third, the reverse saturation current flows because of minority carriers and so is almost independent of the reverse voltage — options claiming it grows steadily with reverse bias confuse the flat pre-breakdown region with the breakdown knee. Fourth, the device census: the LED is forward-biased to emit, the photodiode reverse-biased to detect, and the solar cell unbiased to generate — the exam pairs wrong biases with devices to test exactly this. Fifth, the ripple-frequency question: full-wave rectification of 50 Hz mains gives 100 Hz, and answering "50" is the planted error.

Frequently asked questions

What distinguishes n-type from p-type doping?

Pentavalent atoms (P, As, Sb) donate electrons to the conduction band, making electrons the majority carriers; trivalent atoms (B, Al, In) create acceptor levels and holes become majority — the crystal remains electrically neutral in both cases.

What is the depletion region at a p-n junction?

The region straddling the junction where mobile carriers have recombined, leaving fixed ionised donors and acceptors; it supports the barrier potential and widens under reverse bias.

Why is the reverse current of a diode so small and nearly constant?

It is carried only by thermally generated minority carriers, whose supply is fixed by temperature; it barely responds to the reverse voltage until breakdown intervenes.

How does a Zener diode regulate voltage?

Operated in reverse breakdown, it conducts whatever current the circuit offers while holding a nearly constant voltage across itself; the sharp, non-destructive breakdown comes from its heavy doping.

How do an LED and a photodiode differ in operation?

The LED is forward-biased and converts current to light by electron-hole recombination; the photodiode is reverse-biased and converts incident light into current by generating carriers — emission and detection, opposite jobs.

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