Intrinsic vs Extrinsic Semiconductor: Carriers, Fermi Level and Temperature Compared
An intrinsic semiconductor is a pure semiconductor with almost no impurities. It contains equal numbers of electrons, lifted by heat from the valence band into the conduction band, and the holes they leave behind. An extrinsic semiconductor has donors or acceptors deliberately added, so either electrons or holes become the majority carriers. The intrinsic carrier density of silicon at room temperature is only about 1×10¹⁰ cm⁻³, so real devices add impurities to set the carrier density and conductivity type.
| Aspect | Intrinsic semiconductor | Extrinsic semiconductor (n-type, p-type) |
|---|---|---|
| Impurities | None added on purpose (ideally perfectly pure) | Donors (phosphorus, arsenic, etc.) or acceptors (boron, etc.) are added |
| Origin of carriers | Only thermal generation of electron–hole pairs | Mainly ionization of impurities, plus a small amount of thermal pair generation |
| Electrons vs holes | Equal (n = p = ni) | One type dominates: n ≈ ND in n-type, p ≈ NA in p-type |
| Carrier density (silicon at room temperature) | About 1×10¹⁰ cm⁻³ | Set mostly by the impurity concentration; can be many orders of magnitude above the intrinsic density |
| Product of electron and hole densities | n × p = ni² | Also n × p = ni² in thermal equilibrium. Minority carrier density is ni² / impurity concentration |
| Fermi level | Near the middle of the band gap (intrinsic Fermi level) | Shifts toward the conduction band in n-type and toward the valence band in p-type |
| Resistivity (silicon at room temperature) | High (on the order of 10⁵ Ω·cm) | Low; drops by orders of magnitude depending on impurity concentration |
| As temperature rises | Carriers increase exponentially and resistivity falls sharply | Carrier density is nearly constant over a middle temperature range that includes room temperature. At very low temperatures impurities stop ionizing and carriers decrease (freeze-out); at high temperatures thermally generated carriers take over and it behaves like an intrinsic semiconductor |
| How it is used | Rarely used in devices as is; it is the high-purity crystal that doping starts from | Nearly every device: transistors, diodes, wells, sources and drains |
Figures are typical orders of magnitude and vary by process generation and product.