Nanoscale three-terminal T-branch junctions operated in push–pull fashion commonly exhibit a nonzero voltage at the centre electrode. In principle, their sign corresponds to the conduction type of the semiconductor material. For example is for n-type conduction, independent of the origin of the effect which could be ballistic or diffusive mode control, hot-electron thermopower or, in Y-shaped junctions, ballistic charging. We report on orthogonal four-terminal junctions on high-mobility n-type GaAs/AlGaAs, with current-carrying branches of varying length at constant widths of 410 nm and 320 nm, respectively. When operated at low temperatures as three-terminal devices, we show that under sufficiently large gate voltage the result is This is particularly pronounced at short branches where the mode effect is weak. Up to a current we observe independent of the branch length, where Around the centre voltage exhibits a parabolic behaviour, where the curvature κ is independent of electron density in the range As temperature rises κ monotonically decreases, staying positive up to 77 K. The observation of the Gurzhi effect as a signature of the hydrodynamic transport regime suggests an explanation of the mechanism in terms of the electronic analogue of the Venturi effect.
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