2.1.9 · D1Band Theory & Carrier Physics

Foundations — Diffusion current and concentration gradient

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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.


The cast of characters (built in order)

1. A carrier — the thing that moves

Picture it: think of coloured marbles rolling around inside a shoebox. Each marble is a carrier.

Why the topic needs it: diffusion current is made of carriers moving. If nothing carries charge, there is no current to talk about.


2. Position — where along a line we are

Picture it: a ruler laid flat. Every point on it has one number, .

Why the topic needs it: carriers move from one place to another, so we need a way to say "here" versus "there". is that address.


3. Concentration (and ) — how crowded it is here

Picture it: stand at one address and count the marbles in a tiny box around you. That count (per volume) is at that spot. Walk to a new and the count may change.

Why the topic needs it: diffusion happens because is different in different places. If were the same everywhere, nothing would spread. Notice the units: means "per volume", which is exactly a crowdedness.


4. The concentration gradient — the STEEPNESS of the crowding

Here is the single most important symbol in the whole topic, so we build it slowly.

The 's mean "a tiny bit of": = a tiny change in crowding, = 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.


5. Flux — how many carriers cross a line each second

Picture it: draw a doorway at some . 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 (); later we multiply by charge to get amps.


6. Charge — how we turn a particle count into current

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 get their from exactly here, and the sign of (minus for electrons, plus for holes) is why and end up with opposite signs.


7. Current and current density — charge flow, total vs per-area

Picture it: current is total marbles-of-charge per second through the whole wire; 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 , not , because describes the material itself, independent of sample size.


8. The diffusion coefficient — how eager the spreading is

Picture it: honey versus water. Drop dye in both — it spreads fast in water (large ), slowly in honey (small ). Same idea for carriers in silicon.

Why the topic needs it: is the proportionality knob in Fick's law . Without it we'd know the direction of flow but not the rate.


9. Supporting cast (used in the derivation and examples)

Picture it: a pinball bouncing between bumpers — is the gap it flies, the time per hop.

Read the figure below: the purple curve is . The mint dashed line marks ; follow it up to the curve and across (butter dotted line) and you land on the level — that is what "one diffusion length " means: one factor of of decay. This is exactly the shape whose slope (its gradient ) drives the diffusion current in a real diode.


How the foundations feed the topic

Position x

Concentration n

Carrier

Gradient dn dx

Flux F

Diffusion coefficient D

Mean free path and speed

Charge q

Current density J

Diffusion current

Mobility mu

Einstein relation

Thermal voltage VT

Read it top-down: position and carriers define crowding ; the change in crowding is the gradient; gradient plus gives flux; flux times charge gives current density; and the Einstein relation links to drift's mobility. Every arrow is a symbol you now own.


Equipment checklist

Hide the right side and test yourself. If you can answer all, you are ready for the parent note.

What does measure and in what units?
Position along a line, in cm.
What does measure and in what units?
Carrier crowding — carriers per volume, .
In plain words, what is ?
The slope/steepness of the crowding graph — how fast changes per tiny step in ; units .
Why does diffusion depend on the slope, not on itself?
An even crowd, however dense, doesn't spread; only a lopsided (sloped) one does.
If falls as rises, what is the sign of ?
Negative — and that's the normal case, not an error.
What is flux and its units?
Net carriers crossing a line per second per area (rightward positive); units .
What is the difference between current and current density ?
is total charge per second (amperes) through the whole cross-section; is current per unit area ().
How do you turn flux into current density ?
Multiply by the carrier's charge: .
What is and its sign for each carrier?
C; electrons , holes .
What does the diffusion coefficient tell you, in units?
How fast carriers spread, in .
What is built from?
Mean free path over collision time, .
What are and ?
= Boltzmann constant ; = absolute temperature in kelvin (room temp ).
What equation links and mobility ?
The Einstein relation, .
What is at 300 K?
About V ( mV).
What does mean in ?
The diffusion length — the distance over which the profile decays by a factor .