high bias for APDs. Wide bandgap III-V GaN-based materials have attracted much attention owing to their continuously tunable energy bandgap from 0.7 to 6.2 eV, radiation durability, temperature stability, etc. [4,5] GaN-based photodetectors are urgently needed for military and civilian applications, such as plume detection, flame warning, chemical sensing, and solar astronomy. Many types of GaN-based photodetectors have been developed, such as p-i-n, Schottky barrier, and metalsemiconductor-metal structures. [6][7][8] However, the responsivity or sensitivity of GaN-based photodetectors is limited by the large dislocation densities in III-nitride materials (as high as 10 8 -10 10 cm −2 ) due to the lattice mismatch between the III-nitride material and foreign substrates. Especially for GaN-based APDs, which have very stringent requirements on crystalline quality, the large dislocation density hinders their further development.To improve the sensitivity of GaN-based photodetectors, surface plasmon resonant enhanced structures have been proposed via strong light coupling by localized surface plasmon resonance. [9,10] Graphene/GaN hybrid structures have also been proposed owing to the high light transmittance and easy Fermi level tunability of graphene. [11,12] However, such methods will only elevate the detection responsivity to tens of A W −1 , which is still not enough for weak photodetection. Due to the high quality and large surface-to-volume properties of the nanowires, GaN single nanowire-based photodetectors have been put forward with responsivities as high as 10 3 -10 7 A W −1 . [13][14][15] However, such photodetectors are not widely applicable because the complex fabrication process on a single nanowire is not suitable for mass production. Hence, obtaining nitride-based photodetectors with ultrahigh sensitivity remains a great challenge.In this work, a new type of photodetector based on a graphene/InGaN quantum dot (QD) hybrid structure is proposed, and this photodetector exhibits an ultrahigh responsivity over 10 9 A W −1 and an fW light detectivity at room temperature. For such structures, the gain, which originates from the recirculation of charge carriers in graphene during the lifetime of the photogenerated carriers, is denoted as [16][17][18][19] / lifetime transitwhere τ lifetime is the lifetime of the photogenerated carriers and τ transit is the carrier transit time in graphene between Highly sensitive photodetection is indispensable in applications, such as remote sensing, imaging, and smoke alarming. III-V nitrides are promising candidates for photodetectors due to their continuously tunable bandgap, radiation hardness, and temperature stability. However, the sensitivity of traditional III-V nitride-based photodetectors is limited by poor crystal quality which stems from lattice mismatch-induced point defects and dislocations. Recently, a new type of graphene-colloidal quantum dot (QD) hybrid phototransistor has been preferentially used to obtain high detection sensitivity, but III-V nitride-base...