Abstract

We demonstrate that three conductance features, 0.5 and $0.7{G}_{0}$ plateaus and a dip at $0.5{G}_{0}$, observed in quantum point contacts (QPCs) can be consistently explained by the Rashba interaction in the nonuniform electric field created by the side gates along the transport direction. A quantity $\ensuremath{\gamma}$ is defined which depends on the extent of this nonuniformity and the electron density. A short QPC tends to have a small $\ensuremath{\gamma}$. Only when $\ensuremath{\gamma}$ is large will the Rashba interaction produce a potential well deep enough to localize the electron. This provides the bound state that forms the Kondo resonance with the tunneling electrons. We propose to compare the medium/long QPC to small/large quantum dots, which are governed by the Kondo physics and the Coulomb blockade, respectively. The relation between 0.7 anomaly and the side-gate voltage, length of QPC, and temperature can all be determined to agree qualitatively with the experiments.

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