20.04.2013 Views

Banha University

Banha University

Banha University

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

negatively charged acceptor ions. If we assume there are no external connections<br />

to the semiconductor, then this diffusion process cannot continue indefinitely. The<br />

density gradient produces a "diffusion force" that acts on the majority carriers.<br />

These diffusion forces, acting on the electrons and holes at the edges of the space<br />

charge region. The net positive and negative ion charges in the n and p regions<br />

induce an electric field in the region near the junction, in the direction from the<br />

positive to the negative charge, or from the n to the p region. The electric field in<br />

the junction region produces another force on the electrons and holes which is in<br />

the opposite direction to the diffusion force for each type of particle. In thermal<br />

equilibrium, the diffusion force and the E-field force exactly balance each other.<br />

The net positively and negatively charged regions are referred to as the space<br />

charge region. Essentially all electrons and holes are swept out of the space charge<br />

region by the electric field. Since the space charge region is depleted of any mobile<br />

charge, this region is also referred to as the depletion region.<br />

The Fermi energy level is constant throughout the entire system. The conduction<br />

and valance band energies must bend as we go through the space charge region.<br />

(ii) The electric field:<br />

The charge density ρ(x) = - eNa - xp ≤ x ≤ 0<br />

= e Nd 0 ≤ x ≤ xn

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!