Graphene-based photodetectors have attracted strong interest for their exceptional physical properties, which include an ultrafast response 1-3 across a broad spectrum 4 , a strong electronelectron interaction 5 and photocarrier multiplication [6][7][8] . However, the weak optical absorption of graphene 2,3 limits its photoresponsivity. To address this, graphene has been integrated into nanocavities 9 , microcavities 10 and plasmon resonators 11,12 , but these approaches restrict photodetection to narrow bands. Hybrid graphene-quantum dot architectures can greatly improve responsivity 13 , but at the cost of response speed. Here, we demonstrate a waveguide-integrated graphene photodetector that simultaneously exhibits high responsivity, high speed and broad spectral bandwidth. Using a metal-doped graphene junction coupled evanescently to the waveguide, the detector achieves a photoresponsivity exceeding 0.1 A W 21 together with a nearly uniform response between 1,450 and 1,590 nm. Under zero-bias operation, we demonstrate response rates exceeding 20 GHz and an instrumentation-limited 12 Gbit s 21 optical data link.Graphene demonstrates ultrafast carrier dynamics for both electrons and holes, and it has been shown that a weak internal electric field allows high-speed and efficient photocarrier separation 2,3,14 . Moreover, graphene's two-dimensional nature appears to enable the generation of multiple electron-hole pairs for every highenergy photon excitation 6-8 . This carrier multiplication process is equivalent to inherent gain in graphene photodetection, which exists even without external bias, unlike traditional avalanche detection 15 . Despite these attractive features, the low optical absorption in graphene results in low photoresponsivity in vertical-incidence photodetector designs.Recently it has been revealed that coupling graphene to a bus waveguide can enhance light absorption over a broadband spectrum 16,17 . Here, we show that, by integrating a graphene photodetector onto a silicon-on-insulator (SOI) bus waveguide, it is possible to greatly enhance graphene absorption and the corresponding photodetection efficiency without sacrificing the high speed and broad spectral bandwidth. In our device, presented in Fig. 1a, a silicon waveguide is backfilled with SiO 2 and then planarized to provide a smooth surface for the deposition of graphene. A thin SiO 2 layer ( 10 nm) deposited on the planarized chip electrically isolates the graphene layer from the underlying silicon structures. The optical waveguide mode couples to the graphene layer through the evanescent field, leading to optical absorption and the generation of photocarriers. Two metal electrodes located on opposite sides of the waveguide collect the photocurrent. One of these electrodes is positioned 100 nm from the edge of the waveguide to create a lateral metal-doped junction that overlaps with the waveguide mode. The junction is close enough to the waveguide to efficiently separate the photoexcited electron-hole pairs at zero bias, but the meta...