Chloe Leblanc1,Dinusha Herath Mudiyanselage2,Seunguk Song1,Huairuo Zhang3,4,Albert Davydov3,Houqiang Fu2,Deep Jariwala1
University of Pennsylvania1,Arizona State University2,National Institute of Standards and Technology3,Theiss Research, Inc.4
Chloe Leblanc1,Dinusha Herath Mudiyanselage2,Seunguk Song1,Huairuo Zhang3,4,Albert Davydov3,Houqiang Fu2,Deep Jariwala1
University of Pennsylvania1,Arizona State University2,National Institute of Standards and Technology3,Theiss Research, Inc.4
Monocyclic Gallium oxide β-Ga<sub>2</sub>O<sub>3</sub> is a promising candidate for high-power and high-temperature electronics and UV-range optoelectronic devices. Its advantageous properties include an ultra-wide bandgap, high critical electric field, and affordable bulk single crystal melt-growth techniques at the large production scale. However, single crystalline β-Ga<sub>2</sub>O<sub>3</sub> substrates are seldom explored, in part due to the uncertain effects of the semiconductor’s proven anisotropy. In this study, we fabricated 2D/3D β-Ga<sub>2</sub>O<sub>3</sub> vertical heterojunctions and comprehensively assessed the effect of the choice of 2D material, contact metal and substrate crystalline orientation on their performance. Three orientations of degenerately n-doped β-Ga<sub>2</sub>O<sub>3</sub> were considered: (001), (010) and (-201). Tungsten diselenide (WSe<sub>2</sub>), tungsten disulfide (WS<sub>2</sub>) and black phosphorus (BP) were chosen as 2D semiconductor materials for their popularity in high-performing optoelectronic devices, field-effect transistors (FETs) and light-emitting diodes (LEDs) among others. We compared Electron beam (E-beam) evaporated titanium (Ti), molybdenum trioxide (MoO<sub>3</sub>) and palladium (Pd) as candidates for electrical contacts, with thicknesses based on previous reports of low-resistance: Ti/Au (10/90nm), MoO<sub>3</sub>/Au (3/30nm), Pd/Au (30/70nm). The structure and properties of our fabricated devices were then evaluated using current-voltage (I-V) measurements at varying temperatures, atomic-force microscopy (AFM) techniques and technology computer-aided design (TCAD) simulations. Scanning transmission electron microscopy (STEM) cross-sectional images verified the clean interfaces of the heterostructures. We were able to realize high-performing diodes, whose ideality factors ranged from 1 to 3. Our findings suggest that heterojunction performance is optimized by the β-Ga<sub>2</sub>O<sub>3</sub> orientation (-201), combined with 2D WS<sub>2</sub> exfoliated layers and Ti metal contacts, and show record rectification ratios (> 10<sup>6</sup>) concurrently with ON current density (> 10<sup>3</sup> A/cm<sup>2</sup>) for application in power rectifiers. The lowest ideality factors along the (-201) orientation were 1.18 (BP & Ti/Au contacts), 1.22 (WS<sub>2</sub> & Ti/Au contacts) and 1.43 (WS<sub>2</sub> & Pd/Au contacts) in line with some of the best 2D/3D van der Waals heterojunction diodes reported in the past. The TCAD simulations were able to verify this, and accurately mimic the (-201) heterostructures’ behavior. At large biases and before the junctions reach saturation, the exponential current density increase matches the strongly rectifying property of ideal diodes. In such a linear regime, the devices are driven by the diffusion current across the internal 2D/3D potential barrier. Moreover, the reverse and low forward bias regions present current densities that are both very low (<10<sup>-10</sup> A/µm<sup>2</sup>) and independent of the applied voltage. Our findings demonstrate a facile fabrication of strongly rectifying and high ON current density Ga<sub>2</sub>O<sub>3</sub>-based heterojunction diodes and enables this material’s potential for new avenues in solid state devices.