Diamond is a wide bandgap semiconductor (bandgap 5.5 eV). However, due to impurity doping, it becomes a p-type or n-type semiconductor. The minimum resistivity of the p-type semiconductor is less than 10-3 Ωcm, which is equivalent to that of silicon (Si). When the diamond surface is terminated with hydrogen (H) or Si atoms, the subsurface becomes a p-type accumulation layer or inversion layer, forming a two-dimensional Hall gas (2DHG) that can be used as a channel for field effect transistors (FETs). As a p-channel FET (p-FET), its performance is now approaching that of other wide bandgap semiconductor n-channel FETs. This review describes the metal contact and 2DHG formation on the H-terminated diamond surface from a surface dipole perspective. Recent advances in 2DHG FETs have been discussed, especially in current densities of > 1A / mm and high frequency performance. Finally, we propose two types of complementary high-voltage circuits that combine diamond p-FETs and other wide bandgap semiconductor n-FETs.