edented impact on the electronic industry and on solid-state research in particular. [2] Usually, they are fabricated by connecting two p-n junction diodes in a back-to-back configuration and work as a critical component in some high-speed computers, modem communication, and power systems. [3] A typical BJT consists of emitter (E), base (B), and collector (C) regions. By replacing the middle contact (B) with a light beam, one can achieve photocurrent gain, which is called floating-base bipolar phototransistor. In such device, the asformed bipolar transistor is operated in a common-emitter mode with the base floated and collector negatively biased, presenting ultrasensitive photoelectric response to weak light intensity due to its additional internal gain to amplify the weak photo-induced current [4][5][6][7] and achieving a well-rounded performance in terms of gain, bandwidth, responsivity, quantum efficiency, and dark current noise. [8,9] In bulk semiconductors, p-n junctions are formed by carefully incorporating substitutional impurities. [10] Such techniques, nonetheless, are difficult to implement in nanostructured semiconductors. Besides, nanostructured semiconductor BJT devices are usually constructed by multiple transfer processes, which is both cumbersome and inefficient. [4,11] Because of its intrinsic lack of defects and grain boundaries, organic semiconductor crystal exhibits high transport efficiency and long exciton diffusion length and lifetime, which has drawn ever-increasing attention for photoelectric device applications, such as organic field effect transistors (OFETs), organic light-emitting diodes (OLEDs), and organic photovoltaic cells (OPVs). [12][13][14][15] However, the low drift velocity of carriers and high density of localized states have hindered the application of organic semiconductors in optoelectronics. [16,17] These shortcomings have been addressed through significant efforts, including coupling organic active crystals with other sensitive materials to form heterojunction. Perovskites containing methylammonium lead halide (MAPbX 3 , MA = CH 3 NH 3 + , X = Cl, Br, I) exhibit an ultra-ideal photoelectric response because of their direct bandgap, large absorption coefficient, and long lifetime of photocarriers, rendering them outstanding candidates as efficient phototransistor materials. [18,19] Besides, organic semiconductor crystals usually show a narrow, single-band response Bipolar junction transistor (BJT) has had an unprecedented impact on the electronic industry and helped to usher in the digital revolution prominently. However, the critical part of BJT, p-n junction, is formed by carefully incorporating substitutional impurities in traditional bulk semiconductors and it is difficult to implement in nanostructured device. In this work, a floating-base BJT device is demonstrated by growing C8-BTBT/MAPbBr 3 /C8-BTBT PNP heterostructure in liquid phase. Growth of two semiconductor microwires into a crisscross heterojunction is achieved through template-guided printing and antisol...