For a forward biased PN junction, we assume the hole and electron currents are constant inside the depletion region when there is no generation or recombination in the depletion region (shown from the figure off of Neaman's book). If we only consider the holes, their concentration profile inside the depletion region and the P side can be determined determined from the quasi-fermi level for holes $E_{Fp}$: $$p(x)= n_{i}e^\frac{(E_{i}-E_{F_{p}})}{KT}$$
However, using $J_{p$} = e\mu_{p}p(x)E_{bi}(x)-eD_{p}\frac{dp(x)}{dx}$ where $E_{bi}(x)$ is the built in electric field which is known, I dont get a constant hole current inside the depletion region as the book claims? why is this the case? Is there something I am missing that is taking place inside the depletion region ?