“…Wide-band-gap semiconductors, such as GaN, SiC, and diamond, have attracted significant attention for their potential to surpass the limitations of silicon-based technologies. , Due to a combination of extraordinary electronic properties such as high breakdown voltage (>20 MV/cm), high carrier mobilities (4500 cm 2 /(V·s) for electrons and 3800 cm 2 /(V·s) for holes), and high carrier saturation velocities (2.7 × 10 7 cm/s for electrons and 1.1 × 10 7 cm/s for holes), diamond has been long hailed as the ideal material for building the next generation of high-power and high-frequency electronics with performance unattainable by other competing wide-bandgap semiconductors . Although diamond, similar to most wide-band-gap semiconductors, is inherently difficult to be doped due to deep doping levels, the discovery and understanding of the p-type surface conductivity on hydrogen-terminated diamond (H-diamond) induced by either atmospheric acceptors and solid-state surface acceptors − through the so-called surface transfer doping process , have paved the way for making surface-conducting diamond a promising platform to develop diamond-based electronics and spintronics technologies. , The emergence of p-type surface conductivity of H-diamond is particularly attractive for fabricating metal-oxide-semiconductor field-effect transistors (MOSFETs), a basic electronic element at the core of next-generation diamond-based integrated circuits . Indeed, high-performance diamond MOSFETs, formed by exploiting the surface-conducting channel of H-diamond, have been widely reported .…”