The mobility of a one-dimensional electron gas can be changed markedly
by moving the electron path from the high-mobility channel toward the
low-mobility focused ion-beam-implanted regions. This can be done sim
ply by applying different biases to the two adjacent in-plane gates. W
hen the bias voltage on one gate is fixed, we increase the other gate
potential and force the current path close to the ion-implanted region
. In this way the mobility rather than the density of the carriers is
controlled, which is the key feature of the velocity modulation transi
stors with inherently fast response.