Step 1: Understanding the Concept:
In a pure semiconductor the electron and hole concentrations are equal, \(n_e = n_h = n_i\).
Doping changes one of them a lot. Even so, the product \(n_e n_h\) stays equal to \(n_i^2\) at the same temperature. This is the law of mass action.
Step 2: Part (a): Type of semiconductor:
The hole concentration rises from \(3 \times 10^8\) to \(6 \times 10^{10}\ \text{m}^{-3}\).
Holes are now the majority carriers. So the semiconductor is p-type. It was doped with a trivalent impurity such as boron or aluminium.
Step 3: Part (b): New electron concentration:
Use the law of mass action: \(n_e n_h = n_i^2\).
\[ n_e = \frac{n_i^2}{n_h} = \frac{(3 \times 10^8)^2}{6 \times 10^{10}} \]
\[ n_e = \frac{9 \times 10^{16}}{6 \times 10^{10}} = 1.5 \times 10^{6}\ \text{m}^{-3} \]
The electron concentration falls a lot, because the extra holes recombine with electrons.
Step 4: Part (c): Energy gap and band diagram:
The energy gap \(E_g\) of the semiconductor stays almost the same on doping. The gap is a property of the host crystal.
Doping only adds a new energy level for the impurity.
Energy band diagram of a p-type semiconductor (described in words):
1. Draw the conduction band at the top, with its lowest edge marked \(E_c\).
2. Draw the valence band at the bottom, with its top edge marked \(E_v\). The gap between them is \(E_g\).
3. Draw a thin dashed line \(E_A\), the acceptor level, just above \(E_v\). The gap between \(E_A\) and \(E_v\) is very small (about 0.01 to 0.05 eV).
4. Show electrons from the valence band jumping up to the acceptor level. They leave holes in the valence band.
Final Answer:
(a) The semiconductor is p-type. (b) The new electron concentration is \(1.5 \times 10^{6}\) m\(^{-3}\). (c) The energy gap stays almost unchanged, and an acceptor level appears just above the valence band.
\[ \boxed{n_e = 1.5 \times 10^{6}\ \text{m}^{-3}} \]