A simple method for the creation of Ohmic contact to 2-D electron gas (2DEG) in AlGaN/GaN high electron-mobility transistors (HEMTs) using Cr/Graphene layer is demonstrated. A weak temperature dependence of this Ohmic contact observed in the range 77 to 300 K precludes thermionic emission or trap-assisted hopping as possible carrier-transport mechanisms. It is suggested that the Cr/Graphene combination acts akin to a doped n-type semiconductor in contact with AlGaN/GaN heterostructure, and promotes carrier transport along percolating Al-lean paths through the AlGaN layer. This new use of graphene offers a simple and reliable method for making Ohmic contacts to AlGaN/GaN heterostructures, circumventing complex additional processing steps involving high temperatures. These results could have important implications for the fabrication and manufacturing of AlGaN/GaN-based microelectronic and optoelectronic devices/sensors of the future. under Ga-rich conditions 34 . The as-grown material was characterized using x-ray diffraction (XRD; BEDE D1, Durham, UK) -2 scans (Fig. 1a), and the thicknesses and composition of the layers were determined using routine dynamical XRD simulation. Atomic force microscopy (AFM; Veeco DI 3100, Plainview, NY) measurements reveal a smooth surface, with expected step-flow growth. The root mean square (RMS) roughness was estimated to be less than 0.5 nm over a surface area of 5×5 m 2 (Fig. 1a).Single-layer graphene was grown by CVD on high-purity polycrystalline Cu foils (Alfa Aesar, Ward Hill, MA) of 25 μm thickness using a process described elsewhere 35 . Cleaned Cu foil pieces (1×1 cm 2 ) were placed inside the CVD chamber consisting of a controlled-atmosphere quartz-tube furnace (Lindberg/Blue M, Asheville, NC), CH 4 +H 2 CVD was performed at 1000 ˚C.The polymethyl methacrylate (PMMA) method 32 was used to transfer the CVD graphene from the Cu foil onto the as-grown AlGaN/GaN substrate. The transferred graphene was characterized by Raman spectroscopy (InVia Raman Microscope, Renishaw, Gloucestershire, UK) using a 514 nm wavelength, 1 mW laser. Figure 1b shows representative Raman spectrum from the transferred graphene, with the signature D-band, G-band, and 2D-band peaks at 1350 cm -1 , 1580 cm -1 , and 2700 cm -1 , respectively. The approximate 2D:G peak height ratio of 2:1 is indicative of single-layer graphene. The lower intensity D-band peak in the spectrum indicates presence of a small amount of defects in the graphene.
4Metal/Graphene/AlGaN/GaN diodes (Fig. 2), and reference metal/AlGaN/GaN Schottky diodes without the graphene, were fabricated. In both types of diodes, an electron-beam evaporated Cr/Au/Ni metal stack (referred to as Cr) was used for contacts. In the case of the Cr/AlGaN/GaN Schottky diodes, the graphene layer was removed by O 2 plasma reactive ion etching (RIE) before metal evaporation. In both types of diodes, Ohmic contact to the 2DEG at the AlGaN/GaN interface was formed at the edge of the samples using pressed indium metal.Current density-voltage (I...