In a one-dimensional quantum point contact, the current carried by any single transverse mode is the product of two quantities: the velocity of the electrons, and their density.
These two quantities differ from one mode to the next. One state might carry a sparse population of electrons moving at high velocity, while another is densely packed but sluggish.
But their product is mode-independent. The variations in velocity exactly cancel the variations in density.
The result is that every single mode, regardless of its internal character, contributes exactly the same fixed quantum of conductance (2e^2/h) to the total. The geometry of the channel dictates the parts, but the multiplication erases the difference.
