Physics · Semiconductor Electronics : Materials, Devices And Simple Circuits · NEET
| Depletion width | Narrows (thinner) | Widens (thicker) |
| Effective barrier | V0 minus V (lower) | V0 plus V (higher) |
| Applied field vs built-in field | Opposes built-in field | Adds to built-in field |
| Current | Large (mA), rises fast | Very small (microamp) |
Forward bias DECREASES (narrows) the depletion width. The battery pushes majority carriers toward the junction. These carriers move into the depletion region and neutralise some of the exposed immobile ions, so the charged region becomes thinner. At the same time the potential barrier (built-in voltage) drops from V0 to about (V0 minus V). Thinner wall plus lower barrier means current can flow easily.
In reverse bias the positive terminal connects to the n-side and the negative terminal to the p-side. This pulls majority carriers AWAY from the junction. As they leave, more immobile donor and acceptor ions are exposed on both sides, so the space-charge region gets wider. The barrier rises to about (V0 plus V). A wider region and higher barrier is why almost no current flows in reverse bias.
The built-in barrier V0 (about 0.3 V for Ge, about 0.7 V for Si) is not fixed once you apply a voltage. Forward bias lowers the effective barrier to (V0 minus V). Reverse bias raises it to (V0 plus V). Barrier height and depletion width always move together: lower barrier goes with a thinner region, higher barrier goes with a wider region.
No. The depletion region is 'depleted' of free electrons and holes. It contains only fixed (immobile) positive donor ions on the n-side and fixed negative acceptor ions on the p-side. Because there are no mobile carriers, this region acts like an insulator and sets up the internal electric field and potential barrier.
Raising temperature generates more electron-hole pairs (more intrinsic carriers, ni increases). More carriers are available near the junction, which slightly reduces the built-in potential barrier V0 and tends to make the depletion region a little narrower. Higher temperature also increases the reverse saturation current, because minority carriers become more plentiful.
Yes. A more heavily doped side has more ions packed close together, so fewer atomic layers are needed to build up the same charge, making the depletion region penetrate less into the heavily doped side. The depletion region extends more into the lightly doped side. So width depends on both the applied bias AND the doping concentration.
The increase in the width of the depletion region in a p-n junction diode is due to:
Three identical p-n junction diodes D1, D2 and D3 are connected across a battery (each in series with a 1 kilo-ohm resistor). If the widths of the depletion regions of D1, D2, D3 are W1, W2, W3 respectively, then the correct option is:
Try the real previous-year questions from this chapter — each with the answer and a full solution.
The applied bias: forward bias makes it thinner, reverse bias makes it thicker.
About one-tenth of a micrometre (0.1 micrometre) at equilibrium, per NCERT. It changes with applied bias.
Because the tiny reverse (saturation) current is carried only by minority carriers, and their number is very small and set by temperature, not by the applied voltage.
Yes. It is about 0.3 V for germanium and about 0.7 V for silicon at room temperature.
It behaves like an insulator because it has no free charge carriers, only fixed ions.