Charge Carriers in Intrinsic Semiconductors
Electrical Conduction in Intrinsic Semiconductors
Uses and Applications
Movement of Charge Carriers
The movement of charge carriers, specifically electrons, is crucial in determining the current flow within a semiconductor. In an intrinsic semiconductor, some electrons gain enough energy to break free from their atomic bonds through various mechanisms such as applied electric field, thermal excitation, and exposure to light. These free electrons become mobile and contribute to the conductivity of the material.
Carrier Concentration
For an intrinsic semiconductor, the concentration of electrons in the conduction band is equal to the concentration of holes in the valence band. Suppose ne is the intrinsic electron concentration, and nh is the intrinsic hole concentration. Then, ne = nh = ni Where ni is the intrinsic carrier concentration, which refers to either the intrinsic electron or hole concentration. The table below shows the intrinsic carrier concentrations of a few semiconductors at room temperature. The free electron density of copper, which is a pure conductor, is also shown for comparison. Absolute zero is the lowest possible temperature at which a material has no thermal energy. At this temperature, all electrons in an intrinsic semiconductor are tightly bound to their atoms, so there are no free electrons or holes. Therefore, the material behaves like an insulator, meaning it does not conduct electricity. Higher Temperature When the temperature rises, the material gains thermal energy. This energy can excite electrons, giving them enough energy to break free from their atoms. When an electron breaks free, it moves to the conduction band, where it can flow and conduct electricity. The absence of the electron in the atom creates a hole in the valence band, resulting in an equal number of electrons and holes. So far, we have seen the random movement of electrons and holes due to thermal energy. Let us examine what happens when an electric field is applied. Presence of Electric Field When an electric field is applied across a semiconductor material, it exerts a force on the charge carriers, thereby influencing their movement. Free electrons in the conduction band experience a force in a direction opposite to that of the electric field. These electrons move toward the positive terminal of the applied voltage. Holes in the valence band experience a force in the same direction as the electric field. As electrons from neighboring atoms move to fill these holes, they effectively move toward the negative terminal of the applied voltage, causing the holes to appear to move in the opposite direction. This collective motion constitutes an electric current within the semiconductor. In intrinsic semiconductors, the ability to conduct electricity depends on the number of charge carriers.
