| 摘要 |
A high-resistivity silicon carbide single crystal is disclosed that includes at least one compensated dopant having an electronic energy level far enough from an edge of the silicon carbide bandgap to avoid conductive behavior, while far enough from mid-gap towards the band edge to create a greater band offset than do mid-level states when the substrate is in contact with a doped silicon carbide epitaxial layer and when the net amount of the dopant present in the crystal is sufficient to pin the Fermi level at the dopant's electronic energy level. The silicon carbide crystal has a resistivity of at least 5000 ohms-centimeters at room temperature. |
