Fig. 5: Extracted \({{{{\mathcal{T}}}}}_{C}\) in the double-source and single-source situations.
From: Fractional-statistics-induced entanglement from Andreev-like tunneling
This figure shows difference between the measured \({{{{\mathcal{T}}}}}_{C}\) for the single-source and double-source settings, which likely results from the effect of bias voltages on the overall electrostatic landscape of the setup. a Values of \({{{{\mathcal{T}}}}}_{C}\), for the double-source (black dots) and the single-source cases with IA0 finite (solid green squares). b The same double-source transmission \({{{{\mathcal{T}}}}}_{C}\) (black dots) is compared to that of the single-source case with IB0 finite (empty green squares). Corresponding values of \({{{{\mathcal{T}}}}}_{A}\) and \({{{{\mathcal{T}}}}}_{B}\) (arranging approximately between 0.02 and 0.08) are provided by the Supplementary Fig. S7.
