The width of the depletion layer in a P-N junction diode
increases when a reverse bias is applied
A P-N junction diode is a fundamental semiconductor device formed by joining P-type and N-type semiconductor materials. At the interface of these two materials, a region known as the depletion layer is formed.
The depletion layer is created due to the diffusion of majority charge carriers across the junction. Holes from the P-side diffuse to the N-side, and electrons from the N-side diffuse to the P-side. When they cross the junction, they recombine, leaving behind uncompensated immobile ions (positive ions on the N-side and negative ions on the P-side). This region, which is depleted of free charge carriers, acts as an insulating layer and presents a built-in barrier potential.
The width of the depletion layer is significantly influenced by the type of external bias voltage applied across the P-N junction diode.
| Bias Type | External Voltage Connection | Effect on Barrier Potential | Effect on Depletion Layer Width | Current Flow |
|---|---|---|---|---|
| Forward Bias | P-type to positive, N-type to negative | Decreases | Decreases | High (easily flows) |
| Reverse Bias | P-type to negative, N-type to positive | Increases | Increases | Very low (leakage current) |
Based on the analysis, the width of the depletion layer in a P-N junction diode increases when a reverse bias is applied because the reverse bias adds to the built-in barrier potential, requiring the depletion region to widen to accommodate the larger potential difference.
In a semiconductor diode, the cut-in voltage is the voltage:
The leakage current in a pn junction is of the order of:
Diode junction breakdowns above 5 V are caused by:
ln a p-n junction diode the forward current
The diffusion capacitance of a PN junction diode