Superconducting field-effect transitor (SuFET) and Josephson field-effect transistor (JoFET) technologies take advantage of electric-field-induced control of charge-carrier concentration to modulate the channel superconducting properties. Despite the fact that the field-effect is believed to be ineffective for superconducting metals, recent experiments showed electric-field-dependent modulation of the critical current ( I C ) in a fully metallic transistor. However, the grounding mechanism of this phenomenon is not completely understood. Here, we show the experimental realization of Ti-based Dayem bridge field-effect transistors (DB–FETs) able to control the I C of the superconducting channel. Our easy fabrication process for DB–FETs show symmetric full suppression of I C for applied critical gate voltages as low as V G C ≃ ±8 V at temperatures reaching about the 85% of the record critical temperature, T C ≃ 550 mK, for titanium. The gate-independent T C and normal-state resistance ( R N ) coupled with the increase of resistance in the superconducting state ( R S ) for gate voltages close to the critical value ( V G C ) suggest the creation of field-effect induced metallic puddles in the superconducting sea. Our devices show extremely high values of transconductance (| g m MAX | ≃ 15 μA/V at V G ≃ ±6.5 V) and variations of Josephson kinetic inductance ( L K ) with V G of 2 orders of magnitude. Therefore, the DB–FET appears as an ideal candidate for the realization of superconducting electronics, superconducting qubits, and tunable interferometers as well as photon detectors.
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Paolucci et al. (2018) studied this question.
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