If $n_i$ is the concentration of intrinsic charge carriers in a pure semiconductor and $n_e$ and $n_h$ be the concentrations of electrons and holes, respectively after the semiconductor is doped, then at thermal equilibrium. |
$n_e\, n_h = n_i$ $n_e\, n_h = {n_i}^2$ $\frac{n_e}{n_h}= {n_i}^2$ $\frac{n_h}{n_e}= {n_i}^2$ |
$n_e\, n_h = {n_i}^2$ |
The correct answer is Option (2) → $n_e\, n_h = {n_i}^2$ For a doped semiconductor at thermal equilibrium, the product of electron and hole concentrations remains constant and equal to the square of the intrinsic carrier concentration: $n_e \cdot n_h = n_i^2$ This is known as the mass-action law for semiconductors. Here: - $n_i$ = intrinsic carrier concentration - $n_e$ = electron concentration after doping - $n_h$ = hole concentration after doping Final Answer: $n_e \cdot n_h = n_i^2$ |