Most of silicon carbide's superior intrinsic electrical properties have been known for
decades. At the genesis of the semiconductor electronics era, SiC was considered an early
transistor material candidate along with germanium and silicon. However, reproducible wafers
of reasonable consistency, size, quality, and availability are a prerequisite for commercial
mass-production of semiconductor electronics. Many semiconductor materials can be melted and
reproducibly recrystallized into large single-crystals with the aid of a seed crystal, such as
in the Czochralski method employed in the manufacture of almost all silicon wafers, enabling
reasonably large wafers to be mass-produced. However, because SiC sublimes instead of melting
at reasonably attainable pressures, SiC cannot be grown by conventional melt-growth
techniques. This prevented the realization of SiC crystals suitable for mass production until
the late 1980s. Prior to 1980, experimental SiC electronic devices were confined to small
(typically 1 cm), irregularly shaped SiC crystal platelets grown as a by-product of
the Acheson process for manufacturing industrial abrasives (e.g.,
sandpaper) [3] or by the Lely process [5]. In the Lely process, SiC
sublimed from polycrystalline SiC powder at temperatures near 2500C are randomly
condensed on the walls of a cavity forming small-hexagonally shaped platelets. While these
small, non-reproducible crystals permitted some basic SiC electronics research, they were
clearly not suitable for semiconductor mass production. As such, silicon became the dominant
semiconductor fueling the solid-state technology revolution, while interest in SiC-based
microelectronics was limited.