Fig. 2: Black phosphorus (BP) photo-tunneling transistor.
From: Ultra-weak infrared light detection based on steep-slope phototransistors

a Schematic of device structure, showing BP channel, graphene contacts (with source and drain electrodes Vs and Vd), bottom gate (Vbg), and two partial top gates (Vtg1 and Vtg2) as well as the dielectric layer of hexagonal Boron Nitride (hBN). b Scanning electron microscopy (SEM) photograph (with false color) of a representative device in (a), the colored dashed line indicate different layers of the device: yellow for bottom hBN and white for top hBN, while the solide white line indicates the bottom gate, the scale bar is 10 \({{\rm{\mu }}}{{\rm{m}}}\). c, d illustrate the schematic band-diagram profiles for the principal operation of different photo-transistors. Specifically, they depict the dark (dashed blue line) and light-illuminated (red line) cases in a photo-tunneling transistor and a conventional field-effect transistor (FET), respectively. With a band-to-band tunneling (thermionic) charge injection mechanism, the device has a steep (smooth) Sub-threshold Swing (SS) and response (does not respond) to weak light, Id represents the source-drain current, Ef denotes the fermi level and Ev indicates the valence band energy of the BP channel. e Room-temperature transfer curves of the device in (b) at different modes. Without top gate (Vtg), the device is an ambipolar FET (black curve). With Vtg1 = 6 V (Vtg2 = −6 V), the device is configured as p-type (n-type) tunneling-transistor Vds = 0.1 V. f, g are enlarged transfer curves for tunneling transistor mode. The dashed triangles show subthreshold slopes of SS = 60 mV/dec for comparison.