Double-groove step buffer gate 4H-SiC metal semiconductor field effect transistor and modeling simulation method
A technology of metal semiconductors and field effect transistors, applied in semiconductor devices, transistors, special data processing applications, etc., can solve the problems of current density decrease and limit power density, etc., achieve power density improvement, increase saturation current density, and optimize electric field lines distribution effect
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Embodiment 1
[0064] like figure 1 and figure 2 As shown, the schematic diagrams of the prior art (hereinafter referred to as SBG MESFET) and the present invention (hereinafter referred to as SBG-MRMESFET) are respectively. These two structures are composed of 4H-SiC semi-insulating substrate layer, P-type buffer layer, N-type channel layer, two heavily doped N-type cap layers and between the gate and N-type channel from bottom to top. The ladder buffer gate layer composition. The only difference between these two structures is that two grooves are introduced on top of the P-type buffer layer of the SBG-MR MESFET, i.e. the first groove is under the gate and the second groove is between the field plate and drain below the pole. The depth and length of the two grooves are the same, 0.15 μm and 1 μm, respectively. The length of the small pillar between the two grooves (L ch ) is 0.2 μm. For comparison, the parameter values used in the simulations are equal and listed in Table 1.
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Embodiment 2
[0087] In the present invention, the output characteristics of the SBG-MR 4H-SiC MESFET and the SBG4H-SiC MESFET will be simulated under the same structural parameters for comparison.
[0088] image 3 shows the V gs = 0V and V ds = Saturation drain current curve under the condition of 40V. It can be seen that the maximum saturated drain current density of the SBG4H-SiC MESFET is 0.0016A / μm, while that of the SBG-MR 4H-SiC MESFET is 0.0022A / μm, which is 37.5% higher than that of the SBG structure.
[0089] Figure 4(a) and Figure 4(b) depict the internal electron flow profiles of these two structures, and the current density of the SBG-MR structure marked in Figure 4(b) is significantly higher than that of the SBG structure in Figure 4(a) density. The reason for these differences is that the two grooves introduced by the p-buffer layer of the SBG-MR structure provide a wider channel, that is, a larger total channel cross-section. This means that the resistance of the SBG-M...
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