In all-oxide ferroelectric (FE) / superconductor (S) bilayers, due to the low carrier concentration of oxides compared to transition metals, the FE interfacial polarization charges induce an accumulation (or depletion) of charge carriers in the S. This leads either to an enhancement or a depression of its critical temperature depending on FE polarization direction. Here we exploit this effect at a local scale to define planar weaklinks in high-temperature superconducting wires. This is realized in BiFeO 3 (FE)/YBa 2 Cu 3 O 7-x (S) bilayers in which the remnant FE domain structure is "written" at will by locally applying voltage pulses with a conductive-tip atomic force microscope. In this fashion, the FE domain pattern defines a spatial modulation of superconductivity. This allows us to "write" a device whose electrical transport shows different temperature regimes and magnetic field matching effects that are characteristic of Josephson coupled weak-links. This illustrates the potential of the ferroelectric approach for the realization of high-temperature superconducting devices. Josephson applications were early realized using low critical temperature (T C ) superconductors. However, the advent of high T C superconductivity prompted efforts to createJosephson devices using high-T C cuprates [6] capable of operating above liquid-nitrogen temperature. A versatile approach, developed during the last decade, exploits a nanoscale spatial modulation of T C in a superconducting film [7,8]. This is accomplished by controllably introducing structural disorder (mostly oxygen interstitials and vacancies) on a local scale, via masked ion irradiation or focused ion beams. That type of disorder locally depresses T C , which allows "patterning" the superconducting properties of the film [9,10]. Both S/N/S weak-links [7,8] and S/I/S tunnel junctions [11] can be defined in this way. Besides yielding very reproducible Josephson characteristics [12], the key advantage of this approach is that the planar geometry allows for very large junction arrays [13], thus opening the door to a variety of superconductor electronics applications [14] .In this paper we investigate a different approach to define planar weak-links in cuprate superconducting films. The idea is to create a nanoscale spatial modulation of T C by electrostatic doping [15] through ferroelectric field-effect [16][17][18]. This is achieved in ferroelectric (FE)/superconductor (S) bilayers in which we combine a FE (BiFeO 3 ) whose polarization has a strong out-of-plane component [19] and a high-T C superconductor (YBa 2 Cu 3 O 7-x ). In this FE/S structure, if the FE polarization points away from the interface, holes are accumulated in the S to screen the negative polarization charges, which enhances T C [red curve in Fig. 1(a)]. Conversely, if the FE points towards the interface, a hole depletion is induced, which leads to a depressed T C [blue curve in Fig. 1(a)]. Switching between those two remnant states is achieved by momentarily applying a gate voltage to reverse t...