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Breakdown Voltage Enhancement in ScAlN/GaN High-Electron-Mobility Transistors by High-<i>k</i> Bismuth Zinc Niobate Oxide

Junao Cheng, Mohammad Wahidur Rahman, Andy Xie, Hao Xue, Shahadat H. Sohel, Edward Beam, Cathy Lee, Hao Yang, Caiyu Wang, Yu Cao, Siddharth Rajan, Wu Lu

2021IEEE Transactions on Electron Devices41 citationsDOI

Abstract

ScAlN/GaN dielectric superjunction high-electron-mobility transistors (HEMTs) with high- k passivation layer Bi <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">1.5</sub> Zn <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">1.0</sub> Nb <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">1.5</sub> O <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">7</sub> (BZN) are demonstrated for enhancement of breakdown voltage. The BZN thin film deposited by RF magnetron sputtering has a dielectric constant of 192 after postdeposition annealing at 400 °C for 10 min. The HEMT with L <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">g</sub> = 200 nm and L <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">sd</sub> = 2.0 μm has a maximum current density of 1.98 A/mm, a maximum transconductance of 0.52 S/mm, and a threshold voltage of V <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">th</sub> = -3 V. With the use of SiN/BZN/SiN sandwiched passivation layer, the average value of breakdown voltage is improved from 68.9 to 121.5 V, due to the reduction of the peak electrical field between the gate and the drain. The device has a cutoff frequency ( f <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">T</sub> ) and maximum oscillation frequency ( f <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">max</sub> ) of 59 and 69 GHz, respectively. Overall, the devices exhibit a significantly higher breakdown voltage with essentially the same f <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">T</sub> and f <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">max</sub> values. Pulse measurements suggest that SiN/BZN/SiN has a similar passivation effect in comparison with devices passivated by a SiN-only layer. This work demonstrates that high current and high breakdown voltage can be achieved simultaneously on semiconductor heterostructures with a high sheet charge density by integration of high- k dielectrics.

Topics & Concepts

TransconductancePassivationHigh-electron-mobility transistorDielectricBreakdown voltageMaterials scienceAnalytical Chemistry (journal)TransistorOptoelectronicsElectrical engineeringPhysicsVoltageChemistryLayer (electronics)NanotechnologyOrganic chemistryEngineeringGaN-based semiconductor devices and materialsGa2O3 and related materialsAcoustic Wave Resonator Technologies
Breakdown Voltage Enhancement in ScAlN/GaN High-Electron-Mobility Transistors by High-<i>k</i> Bismuth Zinc Niobate Oxide | Litcius