Concept:
A clean P-N junction forms an internal depletion layer at its interface. Free electrons from the n-type region diffuse across the junction into the p-type region, where they recombine with available holes. This migration leaves behind uncompensated positive donor ions on the n-side edge and negative acceptor ions on the p-side edge.
This localized region of uncovered ions is depleted of free charge carriers, creating the depletion region. These opposite ions generate an internal electric field (\(E_i\)) pointing from the n-side to the p-side. This field creates a built-in potential barrier (\(V_0\)) that stops further diffusion, stabilizing the junction.
Step 1: Analyze how forward biasing affects the internal electric field.
In a forward bias setup, you connect an external battery so its positive terminal attaches to the p-type side and its negative terminal attaches to the n-type side.
This external voltage sets up an electric field (\(E_e\)) that points from the p-side to the n-side. Because this external field runs directly opposite to the built-in internal electric field (\(E_i\)), it weakens the overall field at the junction.
Step 2: Evaluate changes to the barrier potential height.
Since the external voltage opposes the built-in potential barrier, it lowers the net barrier height. If the built-in barrier potential is \(V_0\) and you apply a forward voltage \(V\), the effective potential barrier drops to:
\[
V_{\text{effective}} = V_0 - V
\]
This reduction lowers the electrical barrier, making it much easier for majority charge carriers to cross the junction.
Step 3: Evaluate changes to the depletion region width.
The negative terminal of the external battery repels free electrons in the n-region toward the junction, while the positive terminal repels holes in the p-region toward the junction.
This forcing action drives majority carriers into the depletion zone, neutralizing some of the exposed boundary ions. As a result, the width of the depletion layer shrinks.
Consequently, both the depletion region width and the barrier potential height decrease under a forward bias configuration.