written 8.4 years ago by | • modified 8.4 years ago |
Mumbai university > FE > SEM 1 > Applied Physics 1
Marks: 5M
Year: May 2014,May 2015
written 8.4 years ago by | • modified 8.4 years ago |
Mumbai university > FE > SEM 1 > Applied Physics 1
Marks: 5M
Year: May 2014,May 2015
written 8.4 years ago by |
p–n junction is a junction formed by joining p-type and n-type semiconductors together in very close contact. The term junction refers to the boundary interface where the two regions of the semiconductor meet. If they were constructed of two separate pieces this would introduce a grain boundary, so p–n junctions are more often created in a single crystal of semiconductor by doping, for example by ion implantation, diffusion of dopants, or by epitaxy (growing a layer of crystal doped with one type of dopant on top of a layer of crystal doped with another type of dopant).
Formation of the Depletion Region-At the instant of the PN junction formation free electrons near the junction diffuse across the junction into the P region and combine with holes.
Filling a hole makes a negative ion and leaves behind a positive ion on the N side. These two layers of positive and negative charges form the depletion region, as the region near the junction is depleted of charge carriers. As electrons diffuse across the junction a point is reached where the negative charge repels any further diffusion of electrons. The depletion region now acts as a Barrier.
Barrier Potential. The electric field formed in the depletion region acts as a barrier. External energy must be applied to get the electrons to move across the barrier of the electric field. The potential difference required to move the electrons through the electric field is called the barrier potential. Barrier potential of a PN junction depends on the type of semiconductor material, amount of doping and temperature. This is approximately 0.7V for silicon and 0.3V for germanium.