Assuming the conventional divisions of the semiconductor into depleted and neutral regions, it is shown that for an abrupt p-n junction with nondegenerate carriers a relation exists between the open circuit photovoltage and the PN product at the junction

, which is valid for all signal levels. In the small-signal case this leads to the standard result. At intermediate levels a new relation
![V = KT/q (1 \\pm m) \\log _{e} ([(PN)_{0}]^{1/2}/n_{i})](/images/tex/15638.gif)
holds, the upper sign for p+-n junctions, the lower for n+-p junctions;

. At very high levels the photovoltage saturates to
![V = kT/q[\\log _{e}(M_{p}M_{n}/n_{i^{2}}) + m \\log _{e}(\\\\mu_{h}M_{p}/\\\\mu_{e}M_{N})]](/images/tex/15640.gif)
. Since M
pand M
Nare the doping levels in the p and n regions, the first term is the diffusion potential and the second term will be positive for p+-n junctions and negative for n+-p junctions. These results compare satisfactorily with the available experimental data.