Before you can read a single line of the parent note, you need a toolbox. This page builds every symbol from absolute zero — plain words, then a picture, then why the topic needs it. Nothing here assumes you have seen the notation before.
Picture it: stand at one address x and count the marbles in a tiny box around you. That count (per volume) is n at that spot. Walk to a new x and the count may change.
Why the topic needs it: diffusion happens becausen is different in different places. If n were the same everywhere, nothing would spread. Notice the units: cm−3 means "per volume", which is exactly a crowdedness.
Here is the single most important symbol in the whole topic, so we build it slowly.
The d's mean "a tiny bit of":dn = a tiny change in crowding, dx = a tiny step in position. Their ratio is "change in crowding per tiny step". This is the idea of a derivative — see Fick's laws of diffusion where it becomes law.
Picture it: draw a doorway at some x. Stand there and count "marbles per second going right, minus marbles per second going left", divided by the doorway's area. That net count is the flux.
Why the topic needs it: flux is the bridge between carriers moving and electric current. First we find how many particles cross (F); later we multiply by charge to get amps.
Picture it: each marble carries a fixed "charge sticker". Multiply the flow of marbles by the sticker size and you get a flow of charge — an electric current.
Why the topic needs it: the parent's final formulas J=±qDdxdn get their q from exactly here, and the sign of q (minus for electrons, plus for holes) is why Jn and Jp end up with opposite signs.
Picture it: current I is total marbles-of-charge per second through the whole wire; J is that same flow but per tiny patch of the wire's face, so it does not depend on how fat the wire is.
Why the topic needs it: the boxed answers of the parent note are all J, not I, because J describes the material itself, independent of sample size.
Picture it: a pinball bouncing between bumpers — ℓ is the gap it flies, τ the time per hop.
Read the figure below: the purple curve is e−x/L. The mint dashed line marks x=L; follow it up to the curve and across (butter dotted line) and you land on the 1/e level — that is what "one diffusion length L" means: one factor of 1/e of decay. This is exactly the shape whose slope (its gradient dxdp) drives the diffusion current in a real diode.
Read it top-down: position and carriers define crowding n; the change in crowding is the gradient; gradient plus D gives flux; flux times charge gives current density; and the Einstein relation links D to drift's mobility. Every arrow is a symbol you now own.