Extended Data Fig. 3: Dependence of transmission thresholds and partitioning on average emission energy.
From: Two electrons interacting at a mesoscopic beam splitter
Additional schematic diagrams of electron partitioning equivalent to Fig. 2d, but with the statistical distribution centred at different values of 〈ϵ1〉, corresponding to features A, A\({}^{{\prime} }\), C and D in panels (a)-(d) respectively. The threshold functions \({\epsilon }_{1}^{* }({\epsilon }_{2})\) and \({\epsilon }_{2}^{* }({\epsilon }_{1})\) are the same as only the symmetric slice Δt = 0 of the statistical distribution with 〈Δt〉 = 0 is considered here. In panels (a)–(c) the partitioning domains are labelled by the indices nm of Pnm, whereas in (d) only the net contribution to the first order correlation signal s(1) is indicated, which assumes non-zero values only inside the two hatched areas ( + 1 and − 1, respectively).
