2026-10-10
A crystal growth engineer runs two SiC growth runs in the same SiC crystal growth furnace. The temperature profile, the seed crystal, and the source powder are identical. The only difference is the chamber pressure. Run A is controlled at 5.0 kPa ± 0.1 kPa. Run B drifts between 4.5 kPa and 5.5 kPa. Run A produces a 4H-SiC crystal with a micropipe density of 0.5 cm⁻². Run B produces a crystal with a micropipe density of 8 cm⁻² and visible polytype inclusions. The pressure variation in Run B is only 20 percent, but it is enough to change the vapor transport rate and the supersaturation at the growth interface. This guide explains why pressure control is one of the most critical parameters in SiC crystal growth.
SiC crystal growth by the physical vapor transport (PVT) method relies on the sublimation of SiC source powder at high temperature (2,200°C to 2,500°C) and the transport of the vapor species to the seed crystal where they condense. The transport rate is driven by the partial pressure gradient between the source and the seed. The total chamber pressure determines the mean free path of the vapor species and the diffusivity of the gas mixture. At low pressure, the mean free path is long, and the transport is dominated by molecular diffusion. At high pressure, the mean free path is short, and the transport is dominated by convective flow. The table below shows the relationship between chamber pressure and transport rate for a typical SiC growth furnace.
| Chamber pressure (kPa) | Mean free path (mm) | Transport rate (g/hour) | Growth rate (mm/hour) | Typical defect density |
| 2.0 | 0.8 | 12 | 0.15 | Low |
| 5.0 | 0.3 | 28 | 0.35 | Low |
| 10.0 | 0.15 | 45 | 0.55 | Moderate |
| 20.0 | 0.08 | 60 | 0.70 | High |
| 50.0 | 0.03 | 75 | 0.80 | Very high |
The transport rate increases with pressure, but the defect density also increases. This is because higher pressure reduces the mean free path, which increases the probability of homogeneous nucleation in the gas phase. These nuclei deposit on the growing crystal as defects. The optimal pressure is the one that provides an acceptable growth rate with a low defect density. In our factory, we have found that a pressure of 4 to 6 kPa provides the best balance for 4H-SiC growth. WuYi TianYao New Material Tech.Co.,Ltd. has been developing SiC crystal growth furnace processes for over 8 years.
SiC has over 200 polytypes, but only 4H-SiC is used for power devices. The polytype that forms during growth depends on the temperature, the pressure, and the supersaturation at the growth interface. The 4H polytype is stable at high temperature and moderate pressure. The 6H polytype is stable at lower temperature and higher pressure. The 3C polytype is stable at low temperature and low pressure. Pressure fluctuations can cause the growth to switch from 4H to 6H or 3C, which creates polytype inclusions. These inclusions are electrically active and degrade device performance. The table below shows the polytype stability window for different pressures.
| Chamber pressure (kPa) | Dominant polytype | Polytype purity | Typical application |
| 1 – 3 | 3C-SiC | Low | Research only |
| 3 – 8 | 4H-SiC | High | Power devices |
| 8 – 15 | 4H + 6H mixture | Moderate | Not suitable for devices |
| 15 – 30 | 6H-SiC | High | LED substrates |
| > 30 | 3C + 6H mixture | Low | Not suitable |
The polytype purity is highest when the pressure is stable within ±0.2 kPa. A pressure fluctuation of ±1 kPa can cause the growth to switch polytypes. In our factory, we use a closed-loop pressure control system with a response time of less than 0.5 seconds. The pressure is measured by a capacitance manometer with an accuracy of ±0.05 percent of reading. WuYi TianYao New Material Tech.Co.,Ltd. integrates these pressure control systems into our SiC crystal growth furnace designs.
The pressure affects the thermal conductivity of the gas mixture in the furnace. At low pressure, the gas is rarefied, and the thermal conductivity is low. This reduces the heat transfer from the source to the seed and changes the temperature gradient. The temperature gradient determines the shape of the growth interface. A convex interface (toward the source) promotes the expansion of the crystal and the formation of defects. A flat or slightly concave interface promotes stable growth. The table below shows the effect of pressure on the temperature gradient and interface shape.
| Chamber pressure (kPa) | Thermal conductivity (W/mK) | Temperature gradient (°C/mm) | Interface shape | Defect tendency |
| 2.0 | 0.05 | 25 | Convex | High |
| 5.0 | 0.12 | 18 | Slightly convex | Low |
| 10.0 | 0.20 | 12 | Flat | Low |
| 20.0 | 0.35 | 8 | Concave | Moderate |
| 50.0 | 0.65 | 5 | Strongly concave | High (polycrystal) |
Process engineer's note: The pressure must be coordinated with the temperature profile and the seed position. A pressure that gives a flat interface at one temperature may give a convex interface at a different temperature. In our factory, we use a process model that couples the pressure, temperature, and geometry to predict the interface shape before the growth run. WuYi TianYao New Material Tech.Co.,Ltd. provides this modeling service to our customers.
Poor pressure control leads to four consequences. The first is polytype inclusions, which degrade the electrical properties. The second is micropipes, which are hollow defects that penetrate the crystal and cause device failure. The third is variable growth rate, which makes it difficult to produce crystals with uniform thickness. The fourth is source depletion, which limits the usable length of the crystal. The table below shows the defect density as a function of pressure stability.
| Pressure stability | Micropipe density (cm⁻²) | Polytype inclusions | Growth rate variation | Usable crystal length |
| ± 0.05 kPa | < 0.5 | None | < 5% | 20 – 25 mm |
| ± 0.2 kPa | 0.5 – 2 | Rare | 5 – 10% | 15 – 20 mm |
| ± 0.5 kPa | 2 – 8 | Occasional | 10 – 20% | 10 – 15 mm |
| ± 1.0 kPa | 8 – 20 | Frequent | 20 – 40% | 5 – 10 mm |
| > ± 1.0 kPa | > 20 | Severe | > 40% | < 5 mm |
The data shows that a pressure stability of ±0.05 kPa is required to achieve a micropipe density below 0.5 cm⁻². This is the level required for power device substrates. At ±0.5 kPa, the micropipe density increases to 2 to 8 cm⁻², which is not acceptable for high-performance devices. This is why the pressure control system is one of the most important components of a SiC crystal growth furnace. In our factory, we use a combination of a capacitance manometer, a butterfly valve, and a PID controller to achieve ±0.05 kPa stability. WuYi TianYao New Material Tech.Co.,Ltd. has validated this performance in production furnaces running 24/7.
Pressure control is one of the most critical parameters in SiC crystal growth. It determines the vapor transport rate, the polytype stability, the temperature gradient, and the defect density. A pressure stability of ±0.05 kPa is required to achieve micropipe densities below 0.5 cm⁻² for power device substrates. The pressure must be optimized for each furnace design and coordinated with the temperature profile. A closed-loop control system with a fast-response valve and a PID controller is essential for maintaining stability throughout the growth run. WuYi TianYao New Material Tech.Co.,Ltd. has been developing SiC crystal growth furnace processes for over 8 years and provides full process support for our customers.
WuYi TianYao New Material Tech.Co.,Ltd. designs and manufactures SiC crystal growth furnace systems with closed-loop pressure control, high-accuracy capacitance manometers, and fast-response butterfly valves. We provide process modeling, pressure optimization, and on-site commissioning support.