Recent research into field-effect transistors (FETs) has often involved investigation of materials that could be used as alternatives to silicon, so that additional device functionalities that cannot be attained using silicone-based FETs can be realized. Transparent electronics, based on wide-bandgap semiconductors and flexible, large-area electronics consisting of organic semiconductors are currently subjects of intensive materials research. From a practical perspective, ZnO is a most attractive wide-bandgap semiconductor because of its low processing temperatures and low cost. Production of thinfilm transistors (TFTs) based on polycrystalline ZnO channels have been reported by several groups, [1±7] among whose works include the demonstration of a fully transparent device.[4] The field-effect mobilities (l FE ) reported in those studies, however, were quite low (0.01±7 cm 2 V ±1 s
±1). Recent simulation of a model of polycrystalline ZnO TFT [8] suggested that a double Schottky-like potential barrier would develop at grain boundaries and act as a charge valve in response to the gate bias. In this model, l FE was shown to increase supralinearly on increasing the gate bias, [9] and this has actually been observed in the devices. It is necessary to use a robust dielectric material for the gate, in order to lower the interface trap density. Such a material has not yet been established, but a CaHfO 3 buffer layer placed underneath the channel has been successfully used.[1] Considering these obstacles to realizing polycrystalline ZnO transistors with high mobility, it should be appropriate to investigate the field-effect characteristics of FETs that are made from single-crystalline ZnO films with well-defined dielectric gates. A grain-boundary-free channel should make it possible to achieve values of l FE that are comparable to those in the bulk crystal, and to realize intrinsic field-effect characteristics.Here we report on the simultaneously measured field-effect transfer characteristics and Hall-effect properties of a latticematched ZnO/ScAlMgO 4 (ZnO/SCAM) [10] heteroepitaxial interface, using an electric field applied through the SCAM substrate, which acted as the gate dielectric. We have previously reported that this particular heterostructure is outstanding in its ability to regulate the epitaxial processes in layer-by-layer growth, [11] and that excellent exciton-related optical properties can be realized in the ZnO epitaxial films formed. [12] We have successfully accumulated electrons with a density of up to~1 10 13 cm ±2 by reducing the SCAM thickness to 10 lm and applying a gate voltage of up to 1 kV (i.e., an electric field of up to 1 MV cm ±1 ). The dependence of the field-effect, Hall, and conductance mobilities on the gate voltage are discussed in order to evaluate the intrinsic field-effect transfer characteristics of the single-crystalline ZnO film, and to compare these properties with those observed in polycrystalline devices. The field-effect mobilities in the present devices can be as high as~70 c...