Transistors switch a semiconductor conductive state (or on-state) and an insulator state (or off-state) by means of a third additional terminal known as gate [1]- [3]. An external bias between their two flow electrodes is always required for channel carriers to move, and this bias represents an undesirable yet unavoidable energy consumption. Harvesting the photon energy, a photovoltaic junction would already act as a self-powered current source, but incipient photovoltaic switches do not have a stable low energy consumption state [4]- [10]. Here, we report a new photo-ferroelectric transistor device concept based on a ferroelectric oxide (FEoxide)/organic semiconductor heterojunction, where an insulating FE-oxide (Pb(ZrxTi1-x)O3) acts as a reversibly polarizable electron transport media of the organic bulk heterojunction (P3HT:PCBM) photogenerated carriers. Therefore we demonstrate two terminal (i.e. gate-less), low-cost (metal-oxide solutionprocessed), self-powered and non-volatile phototransistors that switch between bi-stable on and off states and with a low energy consumption in the off state.A phototransistor, photo-switch or photo-FET [11]-[13] can be defined as a three-terminal device whose output can be simultaneously and independently controlled by light or voltage [14]. Ideally, the phototransistor concept should be integrated into a vertical (sandwich-like) two-terminal device for larger density of miniaturization [15] while keeping a normally-off state for better dissipation efficiency and easier control [16]. A reliable, cleanroom-less, low cost two-terminal phototransistor would represent a paradigm shift for the next generation of sustainable embodiments such as photodetectors, smart windows, flexible detector systems and optical memories [17]. Nevertheless, such a device is unconventional and challenging since a photovoltaic semiconductor Schottky or p-n junction does not switch as internal fields and chemical potentials are not bi-stable [16]. There are however several photo-switchable mechanisms that can result in diverse types of photovoltaic responses; these include ferroelectric photovoltaics [4]-[6], light-induced ionic drift in halide perovskites [7], [8], photovoltaic resistive switching [9] and the photochromic effect [10]. Among the photovoltaic mechanisms enabling switching responses, ferroelectric oxides (FE-oxide) possess useful features in their switchable properties (a changeable direction of current and voltage by polarization switching) and in their anomalous photovoltaic effect that can generate photovoltages much bigger than the band-gap [18] [19]. Nevertheless, their inherently low photocurrents (in the range of nA-µA/cm 2 ) have resulted in poor overall photovoltaic efficiency [19]-[20]. A way to improve the photovoltaic current of FEoxide solar cells is through the combination with organic [31]-[34] or inorganic light absorbers [21]-[27].It has been theoretically [28] and experimentally demonstrated [29], [30] that ferroelectrics bend their electronic band structure and offs...