Abstract <p>This work presents a stepwise structural optimization of N-polar GaN HEMTs on SiC, in which each design iteration addresses the limitations of the previous structure and moves toward a higher-performance device. Starting from an experimental baseline (<i>g</i><sub>m</sub> = 270 mS/mm,&#xa0; <i>f</i><sub>T</sub> = 18 GHz,&#xa0; <i>f</i><sub>max</sub> = 44 GHz, <i>I</i><sub>Dmax</sub> = 0.812 A/mm), Device A (Arcuate-Ended Field Plate) mitigates peak edge fields and increases <i>g</i><sub>m</sub> to 316.44 mS/mm,&#xa0; <i>f</i><sub>T</sub> to 95.68 GHz, and&#xa0; <i>f</i><sub>max</sub> to 170.01 GHz while raising <i>I</i><sub>Dmax</sub> to 1.05 A/mm and yielding BV&#xa0;=&#xa0;240 V. However, Device A still suffers from substantial gate leakage and residual dynamic collapse. Device B (HfO<sub>2</sub> MIS gate with partial HfO<sub>2</sub> passivation) directly resolves Device A’s leakage and interface issues: <i>C</i><sub>gs</sub>/<i>C</i><sub>gd</sub> reduce to 0.36/0.08 pF/mm, <i>g</i><sub>m</sub> rises to 380.32 mS/mm, <i>f</i><sub>T</sub>/<i>f</i><sub>max</sub> improve to 135.19/251.07 GHz, <i>I</i><sub>Dmax</sub> increases to 1.28 A/mm, BV = 300 V, and gate leakage at <i>V</i><sub>GS</sub> = 2 V falls to = 5 × 10<sup>–8</sup> A/mm. Finally, Device C (recessed corrugated channel with a dual-dielectric HfO<sub>2</sub>/HfZrO<sub><i>x</i></sub> (HZO) gate stack) overcomes Device B’s remaining trade-offs, further lowering <i>C</i><sub>gs</sub>/<i>C</i><sub>gd</sub> to 0.30/0.06 pF/mm, boosting <i>g</i><sub>m</sub> to 460.91 mS/mm and&#xa0; <i>f</i><sub>T</sub>/<i>f</i><sub>max</sub> to 183.14/360.03 GHz, achieving <i>I</i><sub>Dmax</sub>= 1.50 A/mm, BV = 380 V, and ultra-low gate leakage (4.4 × 10<sup>–9</sup> A/mm). The results demonstrate that progressive field–gate co-engineering, field-plate shaping, high-<i>k</i> MIS integration, and ferroelectric gating provide a practical pathway to suppress leakage and trapping while significantly improving DC and RF performance for N-polar GaN HEMTs.</p>

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Sequential Gate and Field Plate Optimization in N-Polar GaN HEMTs for High Breakdown Voltage and RF Efficiency

  • B. Mohan,
  • J. Charles Pravin,
  • P. Harikrishnan

摘要

Abstract

This work presents a stepwise structural optimization of N-polar GaN HEMTs on SiC, in which each design iteration addresses the limitations of the previous structure and moves toward a higher-performance device. Starting from an experimental baseline (gm = 270 mS/mm,  fT = 18 GHz,  fmax = 44 GHz, IDmax = 0.812 A/mm), Device A (Arcuate-Ended Field Plate) mitigates peak edge fields and increases gm to 316.44 mS/mm,  fT to 95.68 GHz, and  fmax to 170.01 GHz while raising IDmax to 1.05 A/mm and yielding BV = 240 V. However, Device A still suffers from substantial gate leakage and residual dynamic collapse. Device B (HfO2 MIS gate with partial HfO2 passivation) directly resolves Device A’s leakage and interface issues: Cgs/Cgd reduce to 0.36/0.08 pF/mm, gm rises to 380.32 mS/mm, fT/fmax improve to 135.19/251.07 GHz, IDmax increases to 1.28 A/mm, BV = 300 V, and gate leakage at VGS = 2 V falls to = 5 × 10–8 A/mm. Finally, Device C (recessed corrugated channel with a dual-dielectric HfO2/HfZrOx (HZO) gate stack) overcomes Device B’s remaining trade-offs, further lowering Cgs/Cgd to 0.30/0.06 pF/mm, boosting gm to 460.91 mS/mm and  fT/fmax to 183.14/360.03 GHz, achieving IDmax= 1.50 A/mm, BV = 380 V, and ultra-low gate leakage (4.4 × 10–9 A/mm). The results demonstrate that progressive field–gate co-engineering, field-plate shaping, high-k MIS integration, and ferroelectric gating provide a practical pathway to suppress leakage and trapping while significantly improving DC and RF performance for N-polar GaN HEMTs.