MOSFET Structure and Threshold: Voltage Opens a Channel
Raise the gate voltage to wake the channel
On top is the gate, and the thin band beneath it is the insulating oxide. Raise the gate voltage Vgs. Below a threshold Vth there is nothing at the surface, but above it electrons gather at the surface to form a golden channel linking source and drain.
An insulated gate, field not current
The gate of a MOSFET rests on a thin oxide insulating layer. Because the insulator blocks it, essentially no current flows into the gate. This is the very opposite of the BJT, which needed a base current to work. The gate works by its electric field instead of current. Since almost no current enters, the input impedance is very large and it barely burdens the signal source.
Cross the threshold and a channel forms
The body under the gate is p-type, so there are almost no electrons at its surface. Put a positive voltage on the gate and its field pushes holes away and pulls electrons, the minority carriers, toward the surface. At low voltage too few are drawn, but past a threshold enough electrons gather at the surface to form a thin n-type layer, an inversion layer. This layer becomes the channel linking the n-type source and drain on either side, and only then does a path for current open.
Threshold voltage Vth and overdrive
The gate voltage at which the channel just begins to form is the threshold voltage Vth. Its value is set by the oxide thickness, the doping, and the materials. The more Vgs exceeds Vth, that is, the larger the overdrive Vgs - Vth, the more electrons are drawn in, the thicker the channel, and the more current it can carry. This switch, opening and closing a channel with voltage alone through an insulated gate that draws almost no current, is why MOSFETs underpin digital chips and power conversion.
Back to the first screen
When the gate voltage was below threshold, the surface was empty and source and drain were disconnected. The moment you raised the voltage past the threshold, electrons were drawn to the surface and a golden channel linked the two n-type regions. What opened that path was not a current into the gate but the gate’s electric field acting across the insulator. The threshold is the boundary where the channel just appears, and the overdrive raised above it thickens the channel. This switch, opening and closing a flow with voltage alone without drinking a drop of current, is the starting point of the MOSFET.
What comes next
You crossed the threshold and opened the channel. But how much actually flows once the channel exists also depends on the drain voltage. The next unit raises the drain voltage and sees how the behavior splits: a linear region where the channel acts like a resistor, and a saturation region where the channel end pinches and the current stops rising.