Acceptors
Acceptors

Figure 2: Hole orbiting the acceptor impurity at T = 0K.

By analogy, the incomplete covalent bond in the vicinity of an acceptor impurity in silicon at low temperatures is treated as a positive charge orbiting the negatively charged impurity atom. Its orbit radius is

Equation 6

and its ionisatioon energy becomes

Equation 7

It so happens that in silicon, so that acceptor and donor ionisation energies are approximately equal, , and we are again justified in assuming that all acceptors impurities in silicon are ionised at room temperature; po = NA- = NA.

Note, however, for a III - V semiconductor such as GaAs,Equation 8 so Equation 9.
Also,Equation 10,so Equation 11;specifically,Equation 12 , and Equation 13.

leftarrow