Note that the property of an oxide semiconductor is not uniquely determined by an atomic ratio. Even with the same atomic ratio, the property of an oxide semiconductor might be different depending on a formation condition. For example, in the case where the oxide semiconductor is deposited with a sputtering apparatus, a film having an atomic ratio deviated from the atomic ratio of a target is formed. In particular, [Zn] in the film might be smaller than [Zn] in the target depending on the substrate temperature in deposition. Thus, the illustrated regions each represent an atomic ratio with which an oxide semiconductor tends to have specific characteristics, and boundaries of the regions A to C are not clear.
Next, the case where the oxide semiconductor is used for a transistor is described.
Note that when the oxide semiconductor is used for a transistor, carrier scattering or the like at a grain boundary can be reduced; thus, the transistor can have high field-effect mobility. In addition, the transistor can have high reliability.
An oxide semiconductor with low carrier density is preferably used for the transistor. In order to reduce the carrier density of the oxide semiconductor film, the impurity concentration in the oxide semiconductor film is reduced so that the density of defect states can be reduced. In this specification and the like, a state with a low impurity concentration and a low density of defect states is referred to as a highly purified intrinsic or substantially highly purified intrinsic state. For example, an oxide semiconductor whose carrier density is lower than 8×1011/cm3, preferably lower than 1×1011/cm3, further preferably lower than 1×1010/cm3, and higher than or equal to 1×10?9/cm3 is used.