Mode-selected heat flow through a one-dimensional waveguide network

TL;DR

This study investigates heat flow in a 1D electron waveguide network in a GaAs/AlGaAs heterostructure at 4.2 K, showing mode-dependent heat transport and negligible electron-phonon interaction.

Contribution

It demonstrates mode-controlled heat flow in a 1D electron waveguide network, revealing deviations from previous single-conductor observations and negligible electron-phonon coupling.

Findings

Heat flow proportional to square of heating current

No temperature increase without electron transmission

Mode control affects heat flow independently of subband population

Abstract

Cross-correlated measurements of thermal noise are performed to determine the electron temperature in nanopatterned channels of a GaAs/AlGaAs heterostructure at 4.2 K. Two-dimensional (2D) electron reservoirs are connected via an extended one-dimensional (1D) electron waveguide network. Hot electrons are produced using a current $I_{\text{h}}$ in a source 2D reservoir, are transmitted through the ballistic 1D waveguide and relax in a drain 2D reservoir. We find that the electron temperature increase ${\Delta}T_{\text{e}}$ in the drain is proportional to the square of the heating current $I_{\text{h}}$, as expected from Joule's law. No temperature increase is observed in the drain when the 1D waveguide does not transmit electrons. Therefore, we conclude that electron-phonon interaction is negligible for heat transport between 2D reservoirs at temperatures below 4.2 K. Furthermore, mode control of the 1D electron waveguide by application of a top-gate voltage reveals that ${\Delta}T_{\text{e}}$ is not proportional to the number of populated subbands $N$, as previously observed in single 1D conductors. This can be explained with the splitting of the heat flow in the 1D waveguide network.