SiC Drift Region Carrier Tuning via Particle Beam Defects
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Solution Overview
Problem
Conventional silicon carbide semiconductor devices face challenges in controlling the variation of majority carrier concentration in the n−-type drift region, leading to inconsistencies in ON resistance and breakdown voltage, especially under high temperature conditions.
Innovation Solution
The silicon carbide semiconductor device incorporates a method where a particle beam is irradiated to introduce point defects in the n−-type drift region, adjusting the effective majority carrier concentration to be lower than the impurity concentration, thereby reducing variation and optimizing device performance.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Manufacturing precision
If epitaxial growth is performed at high temperature (about 1600 degrees C) to form the n−-type drift region, then the drift region can be formed with appropriate doping, but the majority carrier concentration varies significantly (±15% from target value between chips)
Solution Approach 1:
The patent applies parameter changes by introducing point defects through particle beam irradiation to modify the electrical characteristics of the drift region. The irradiation dose is controlled to create a specific density of point defects that compensate for the high-temperature epitaxial growth variations, thereby adjusting the majority carrier concentration to match target values across different chips.
Solution Approach 2:
The patent replaces the purely thermal process (epitaxial growth at 1600°C) with a combined approach involving particle beam irradiation. This substitution introduces a new mechanism (radiation-induced point defects) to control carrier concentration, complementing the thermal growth process and achieving better precision than temperature control alone.
2Ease of manufacture
If high temperature epitaxial growth is used to form the drift region, then the doping process can be completed, but the ON resistance and breakdown voltage show significant variation
Solution Approach 1:
The patent changes the physical state of the drift region by introducing point defects through particle beam irradiation. This creates a new parameter (defect density) that can be independently controlled to adjust electrical characteristics, thereby achieving precise control of ON resistance and breakdown voltage despite variations in the epitaxial growth process.
3Strength
If the majority carrier concentration is reduced to optimize breakdown voltage, then voltage withstanding capability improves, but ON resistance increases
Solution Approach 1:
The patent applies local quality by creating point defects specifically in the drift region through particle beam irradiation. These localized defects provide compensation that allows independent optimization of breakdown voltage and ON resistance, decoupling the trade-off that would otherwise require uniform changes in doping concentration across the entire drift region.
Applied Scientific Principles
This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.
Function Achieved in This Case
This approach effectively reduces the variation of the effective majority carrier concentration in the n−-type drift region, stabilizing the ON resistance and breakdown voltage, and enhancing the device's performance under high temperature conditions.
Implementation Method 1
a particle beam is irradiated to introduce point defects in the n−-type drift region, adjusting the effective majority carrier concentration to be lower than the impurity concentration
Data Source
AI summary
At any timing after formation of gate electrodes, particle beam irradiation is performed to a semiconductor wafer having an n−-type drift region constituted by an n−-type epitaxial layer and having an n-type impurity concentration that is higher than a target majority carrier concentration (design value) of the n−-type drift region. Point defects of a defect density corresponding to an irradiation dose of the particle beam are generated in the n−-type drift region by the particle beam irradiation, whereby an effective majority carrier concentration of the n−-type drift region is adjusted and reduced with respect to the n-type impurity concentration of the n−-type drift region, to approach the design value. After formation of the n−-type epitaxial layer, the n-type impurity concentration of the n−-type drift region may be measured, or the n−-type epitaxial layer may be formed to have an n-type impurity concentration higher than the design value.


