Chapter/Index: Introduction | A | B | C | D | E | F | G | H | I | J | K | L | M | N | O | P | Q | R | S | T | U | V | W | X | Y | Z | Appendix
| Silicon carbide (SiC) has a critical breakdown field that is an order of magnitude higher than that of silicon (Si), along with a bandgap and thermal conductivity approximately three times greater. These properties collectively enable SiC to offer roughly three times the cooling efficiency. Among the various polytypes of SiC (silicon carbide) structures, 6H-SiC and 4H-SiC are the most commonly used, particularly for device manufacturing, due to their ability to form large wafers and their commercial availability. For high-power, high-temperature, and high-frequency device applications, 4H-SiC is the preferred and widely used material because of its superior electron mobility, [1, 2] wider bandgap, higher critical electric field, [3] and lower ionization energy of dopants, [4] as well as the availability of single crystalline wafers. Additionally, unlike 6H-SiC, [5] 4H-SiC does not exhibit anisotropic electron mobility, which has contributed to its focused development and broader availability. Table 1524a. Comparison of the key properties of Silicon (Si), Silicon Carbide (SiC), and Gallium Nitride (GaN).
Table 1524a. Comparison of material parameters of polytypes of SiC and Si.
[1] Palmour, J.; Singh, R.; Glass, R.; Kordina, O.; Carter, C. Silicon carbide for power devices. In Proceedings of the 9th International
Symposium on Power Semiconductor Devices and IC’s, Weimar, Germany, 26–29 May 1997; pp. 25–32.
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