Diode junction breakdowns above 5 V are caused by:
Avalanche effect
A diode junction breakdown is a critical phenomenon that occurs when a diode is subjected to a reverse bias voltage exceeding a certain limit. This leads to a sharp increase in current flowing through the diode in the reverse direction. There are primarily two mechanisms responsible for this breakdown: the Zener effect and the Avalanche effect. The specific mechanism that dominates depends largely on the magnitude of the breakdown voltage.
The Zener effect is a breakdown mechanism that occurs in heavily doped p-n junctions. When a sufficiently large reverse bias voltage is applied, the electric field across the depletion region becomes very strong. This intense electric field can directly pull electrons from their covalent bonds, creating electron-hole pairs. These liberated electrons then contribute to the reverse current.
The Avalanche effect is another breakdown mechanism that occurs in p-n junctions, particularly at higher reverse bias voltages. When the reverse bias voltage is increased, free electrons and holes in the depletion region gain significant kinetic energy. These energetic carriers then collide with atoms in the crystal lattice.
The distinction between the Zener effect and the Avalanche effect as the primary cause of diode junction breakdown is largely determined by the breakdown voltage.
| Feature | Zener Effect | Avalanche Effect |
|---|---|---|
| Dominant Voltage Range | < 5 V to 6 V | > 5 V |
| Mechanism | Direct field emission (tunneling) | Impact ionization (carrier multiplication) |
| Doping Level | Heavily doped junctions | Lightly doped junctions |
| Temperature Coefficient | Negative | Positive |
Based on the distinct characteristics of these breakdown mechanisms, when a diode junction breakdown occurs at voltages above 5 V, the primary cause is the Avalanche effect. This is because at these higher voltages, carriers gain sufficient energy to cause impact ionization, leading to the rapid multiplication of charge carriers and the characteristic sharp increase in reverse current.
In a semiconductor diode, the cut-in voltage is the voltage:
The leakage current in a pn junction is of the order of:
The width of the depletion layer in a P-N junction diode
ln a p-n junction diode the forward current
The diffusion capacitance of a PN junction diode