Abstract

We measure a strong enhancement of the nonlinear differential conductance ($g=dI/dV$), the amplitude of which exceeds the universal quantum conductance ($2{e}^{2}/h$), under finite bias voltage in quantum point contacts (QPCs). By developing a spin-based model in the low-electron-density limit, we demonstrate that this resonance is an intrinsic nonequilibrium phenomenon that arises from many-body induced modifications to the QPC potential. A comparison with the linear conductance ($G=I/V$) shows that this phenomenon is driven by many-body dynamics within a single one-dimensional sub-band.

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