Pn Junction Diode - what happens to carrier profiles when voltage biases are applied?
The pn Diode Circuit Symbol and Terminal Characteristics(6.1)
There are 3 regions of operations of the pn diode
Zero Bias- diode current \(I_D>0\) with the diode voltage \(V_D\approx 0.7 v\)
Forward bias- diode current \(I_D\approx 0\)
Backward Bias- diode current \(I_D<0\) and the diode voltage \(V_D< V_{BD}\) where \(V_{BD}\) is the diode’s breakdown voltage
The transport of holes from the p side across the depletion region into the n side under a forward bias is called hole injection
The transport of electrons from the n side to p side of the junction under a forward bias is called electron injection
Let us see what is happening in the different regions
We have \[|J_\text{drift}| = |J_\text{diff}|\]
We have \[|J_\text{drift}| < |J_\text{diff}|\] This means we have a net diffusion current in the space charge region or into the QNRs
Net diffusion hole current \(J_h\) to the right
Net diffusion electron current \(J_e\) to the left
Both of which in the direction of the SCR towards the ohmic contacts
We have \[|J_\text{drift}|>|J_\text{diff}|\] This means we have a net drift current in the space charge region or from the QNRs
Net drift hole current \(J_h\) to the left
Net drift electron current \(J_e\) to the right
Both of which in the direction of away from ohmic contacts into the SCR
To sum up
In forward bias: injected minority carriers diffuse through QNR and recombine at semiconductor surface
In reverse bias, minority carriers generated at the semiconductor surface diffuse through the QNR and extracted by SCR
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