Tuning the exchange interaction by electric field in laterally coupled quantum dots

Abstract

The effect of external electric field on the exchange interaction has been studied by an exact diagonalization method for two electrons in laterally coupled quantum dots (QD's). We have performed a systematic study of several nanodevices that contain two gate-defined QD's with different shapes and sizes located between source and drain contacts. The confinement potential is modelled by two potential wells with a variable range and softness. In all the considered nanodevices, the overall dependence of exchange energy $J$ on electric field $F$ is similar, i.e., for low fields $J$ increases with increasing $F$, for intermediate fields $J$ reaches a maximum, and rapidly falls down to zero if $F$ exceeds a certain critical value. However, the $J(F)$ dependence shows characteristic properties that depend on the nanodevice geometry. We have found that the low- and intermediate-field behaviour can be accurately parametrized by linear function $J(F) = \αF + \β$, where $ alpha$ is independent of the nanodevice geometry and softness of the confinement potential. We have shown that the linear $J(F)$ dependence appears only if the tunnel coupling between the QD's is weak, i.e., the interdot separation is sufficiently large. The $J(F)$ dependence becomes non-linear for the strong interdot tunnel coupling. If the QD located near the contact, to which the higher voltage is applied, possesses the elliptic shape and is larger than the other QD, the $J(F)$ dependence shows a plateau in a broad electric-field regime. The linearity and rapid jumps of $J(F)$ as well as the existence of the plateau can be applied to tune the exchange interaction by changing the external electric field.