Apr 25, 2024
9:15am - 9:45am
Room 345, Level 3, Summit
Ahmad Islam1,Ashok Dheenan2,Weisong Wang3,Kevin Leedy1,Kyle Liddy1,Daniel Dryden1,Guru Subramanyam4,Aaron Arehart2,Siddharth Rajan2,Kelson Chabak1,Andrew Green1
Air Force Research Laboratory1,The Ohio State University2,Wright State University3,University of Dayton4
Ahmad Islam1,Ashok Dheenan2,Weisong Wang3,Kevin Leedy1,Kyle Liddy1,Daniel Dryden1,Guru Subramanyam4,Aaron Arehart2,Siddharth Rajan2,Kelson Chabak1,Andrew Green1
Air Force Research Laboratory1,The Ohio State University2,Wright State University3,University of Dayton4
Dielectric integration is always challenging for any semiconductor material when used in a metal-oxide-semiconductor (MOS) configuration. SiO<sub>2</sub> offers the best oxide interface on Si, mainly because the SiO<sub>2</sub>/Si interface was carefully engineered by the pioneering works of Atalla et al. Interfacial defect engineering is currently being investigated for wide-bandgap semiconductor such as SiC. Such defect engineering solutions are, however, missing for other oxide/semiconductor interfaces involving wide or ultra-wide bandgap semiconducting materials.<br/><br/>The newest semiconductor β-Ga<sub>2</sub>O<sub>3</sub> can be grown from melt, has a high critical electric field, a low switching loss that can be obtained at a high breakdown voltage, and an efficient high frequency performance. β-Ga<sub>2</sub>O<sub>3</sub> has therefore already demonstrated promises for power switching applications with drive current > 100A and high temperature electronics with operating temperature T >500 <sup>o</sup>C. The dielectric/semiconductor interface of β-Ga<sub>2</sub>O<sub>3</sub> however has large interface defect density (N<sub>IT</sub>) mainly due to the deposition of dielectrics after many process steps in a device fabrication process. A dielectric-early process flow is preferred for reducing N<sub>IT</sub>; to enable this process, dielectrics will have to withstand all the remaining semiconductor process steps, some of which (such as dopant activation anneal) involves >900 <sup>o</sup>C process temperature. Such high T processes induce poly-crystallization (resulting in electrical and mass transport through the grain boundaries) in most dielectrics formed using atomic layer deposition (ALD) – a deposition process that is routinely used for all semiconductor device processes.<br/>Till 2020, most of the MOS devices made on β-Ga<sub>2</sub>O<sub>3</sub> substrates exhibited N<sub>IT</sub> > 10<sup>12</sup> cm<sup>-2</sup> and, therefore, devices exhibited large hysteresis and frequency dispersion during the capacitance-voltage (C-V) and current-voltage (I-V) characteristics. Using conventional crystalline semiconductor wisdom, crystallization of dielectrics via high T annealing were considered for defect reduction (and hence hysteresis and dispersion reduction); this however had limited success as the resultant poly-crystalline suffered from grain boundary conduction and materials diffusion. Therefore, dielectrics with low N<sub>IT</sub> and good thermal stability still remained elusive for establishing electronic-grade semiconductor process flow for β-Ga<sub>2</sub>O<sub>3</sub> devices.<br/>In this work, we will highlight the general challenge for integrating dielectrics on β-Ga<sub>2</sub>O<sub>3</sub>, address the associated requirements for obtaining high-quality dielectric with low N<sub>IT</sub>, and in particular discuss the integration of Al<sub>2</sub>O<sub>3</sub> and SiO<sub>2</sub> dielectrics on (010) β-Ga<sub>2</sub>O<sub>3</sub> substrates. We will discuss the role of surface roughness, surface cleanliness (using piranha treatment), surface defective layer removal (using buffered HF), and post-deposition annealing on interface defect density. We will also compare the thermal stability and interface quality of SiO<sub>2</sub> and Al<sub>2</sub>O<sub>3</sub> dielectrics formed on β-Ga<sub>2</sub>O<sub>3</sub>. We will explain how interfacial crystallization of monolayer Al<sub>2</sub>O<sub>3</sub> (during a low temp ALD deposition at 250 <sup>o</sup>C) enabled formation of high-quality interfaces at the Al<sub>2</sub>O<sub>3</sub>/β-Ga<sub>2</sub>O<sub>3</sub> interface – therefore, showed the lowest interface defect density. This is mainly because the crystal structures of γ-Al<sub>2</sub>O<sub>3</sub> and β-Ga<sub>2</sub>O<sub>3</sub> resembles each other and hence promotes the formation of monolayer γ-Al<sub>2</sub>O<sub>3</sub> at the Al<sub>2</sub>O<sub>3</sub>/β-Ga<sub>2</sub>O<sub>3</sub> interface even at 250 <sup>o</sup>C deposition temperature.<br/>All these considerations have enabled us to envision pathways towards electronic-grade integration of dielectrics on β-Ga<sub>2</sub>O<sub>3</sub> substrates needed to attain high breakdown voltage in power electronics applications and also to attain low frequency dispersion and high operating frequency in radio frequency applications.