photoejected hot carriers excited through photon absorption in metal structures and extracted via internal photoemission [1,2] with the intriguing prospect of direct below-bandgap photodetection at room temperature (RT). However, the collection efficiency of photoejected hot carriers at metal-semiconductor (MS) interface [3] or metal-insulator-metal (MIM) junctions [4] is severely hindered by (i) the fast internal relaxation process, (ii) momentum mismatch, and (iii) the lack of effective lighttrapping mechanisms. To date, plasmonic modes in metals have been widely utilized to enhance photoemission of hot electrons since they can concentrate photon energy in a deep subwavelength region, where extensive amounts of hot electrons can be generated. [5][6][7] Therefore, the working wavelength can be tuned by simply adjusting the frequency of metal plasmonic resonance rather than the bandgap of materials. Hot carriers can be generated in a femtosecond timescale via the Laudau damping of plasmonic modes [8] and they are lifted from electronic states below the Fermi level with appropriate energy hυ. However, they lose their energy very fast, as a consequence, only a small portion of them is able to escape from the MS or MIM interface. Despite the presence of Photodetectors exploiting photoejected hot electrons have the potential to achieve ultrahigh sensitivity and broadband detection capabilities, which are controlled by the structure of the device rather than the bandgap of the employed materials. However, the achievement of photodetectors of long-wavelength photons with both high responsivity and bandwidth is still challenging. Here, a novel class of high-gain photodetectors based on the manipulation of intrinsic hot carriers by exploiting the electromagnetic engineering of a graphene-based active channel is presented. Light field is focused in a split-finger gated structure to create a potential gradient in the channel, which is able to trap and detrap the charges laterally transferred from low resistive Au-graphene interface, finally leading to a high photoconductive gain. Correspondingly, the device activity can be easily switched from photovoltaic to photoconductive, depending on the photoinduced hot-carrier distribution, just by controlling the electric field. The device shows tunable sensitivity, higher energy efficiency, and photoconductive gain. In particular, the responsivity (0.6-6.0 kV W −1 ) and the noise-equivalent power (less than 0.1 nW Hz −0.5 at room temperature) are significantly improved even at low-energy terahertz band with respect to state-of-the-art devices based on extrinsically coupled hot carriers operating in the near infrared.