HJHyeon-Seok Jeong

Hyeon-Seok Jeong

*This is an algorithmically generated author record based on publicly available information.

Current Organizations / Institutes

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Hyeon-Seok Jeong has a total of 21 co-authors. Here are the top co-authors by number of shared publications:


Latest Publications

  • Sub-50 nm Terahertz In0.8Ga0.2As Quantum-Well High-Electron-Mobility Transistors for 6G Applications

    by Wan-Soo Park, Hyeon-Bhin Jo, Hyo-Jin Kim, Su-Min Choi, Ji-Hoon Yoo, Hyeon-Seok Jeong, Sethu George, Ji-Min Baek, In-Geun Lee, Tae-Woo Kim, et al.

    We present a systematic study on the gate length ( ${L}_{{g}}\text {)}$ scaling behavior and the impact of the side-recess spacing ( ${L}_{\text {side}}\text {)}$ on dc and high-frequency characteristics of In0.8Ga0.2As quantum-well (QW) high-electron-mobility transistors (HEMTs) with ${L}_{{g}}$ from 10 $\mu $ m to 20 nm, for the purpose of understanding the scaling limit of maximum oscillation frequency ( ${f}_{\text {max}}\text {)}$ and thereby demonstrating terahertz devices. The fabricated In0.8Ga0.2As QW HEMTs with ${L}_{{g}} =20$ nm and ${L}_{\text {side}} =150$ nm exhibited values of drain-induced-barrier-lowering (DIBL) of 60 mV/V, current-gain cutoff frequency ( ${f}_{{T}}\text {)}$ of 0.75 THz, and ${f}_{\text {max}}$ of 1.1 THz, while the device with ${L}_{\text {side}} =50$ nm showed DIBL of 110 mV/V and ${f}_{{T}}$ / ${f}_{\text {max}}$ of 0.72/0.53 THz. It was central to strictly control short-channel effects (SCEs) from the perspective of DIBL to maximize the improvement of ${f}_{\text {max}}$ , as ${L}_{{g}}$ was scaled down deeply. In an effort to understand the ${L}_{{g}}$ scaling behavior of ${f}_{\text {max}}$ , we carried out the small-signal modeling for both types of devices and found that the increase of the intrinsic output conductance ( ${g}_{\text {oi}}\text {)}$ played a critical role in determining ${f}_{\text {max}}$ in short- ${L}_{{g}}$ HEMTs. On the contrary, the fabricated devices with ${L}_{\text {side}} =150$ nm exhibited a tight control of SCEs at ${L}_{{g}}$ of 20 nm. As a result, ${f}_{\text {max}}$ in those devices was boosted to 1.1 THz, and more importantly this high ${f}_{\text {max}}$ was maintained even as ${L}_{{g}}$ was scaled down to 20 nm. The results in this work represent the best balance of ${f}_{{T}}$ and ${f}_{\text {max}}$ in any transistor technology on any material system, displaying both ${f}_{{T}}$ and ${f}_{\text {max}}$ in excess of 700 GHz simultaneously.


  • Comprehensive modeling of the extrinsic transconductance for In Ga As/In Al As quantum-well high-electron-mobility transistors

    by Seung-Won Yun, Hyeon-Bhin Jo, Hyeon-Seok Jeong, Wan-Soo Park, Ji-Hoon Yoo, In-Geun Lee, Tae-Woo Kim, Takuya Tsutsumi, Hiroki Sugiyama, Hideaki Matsuzaki, et al.


  • Open Access

    Physics-Based Analytical Channel Charge Model of In x Ga1-x As/In0.52Al0.48As Quantum-Well Field-Effect Transistors From Subthreshold to Strong Inversion Regimes

    by Hyeon-Seok Jeong, Wan-Soo Park, Hyeon-Bhin Jo, In-Geun Lee, Tae-Woo Kim, Takuya Tsutsumi, Hiroki Sugiyama, Hideaki Matsuzaki, Sung-Ho Hahm, Jae-Hak Lee, et al.

    This paper presents a physics-based analytical channel charge model for indium-rich In x Ga 1-x As/In 0.52 Al 0.48 As quantum-well (QW) field-effect transistors (FETs) that is applicable from the subthreshold to strong inversion regimes. The model requires only seven physical/geometrical parameters, along with three transition coefficients. In the subthreshold regime, the conduction bands ( $E_{C}$ ) of all regions are flat with finite and symmetrical QW configurations. Since the Fermi–level ( $E_{F}$ ) is located far below $E_{C}$ , the two-dimensional electron-gas density ( $n_{2{-}DEG}$ ) should be minimal and can thus be approximated from Maxwell–Boltzmann statistics. In contrast, the applied gate bias lowers the $E_{C}$ of all structures in the inversion regime, yielding band-bending of an In 0.52 Al 0.48 As insulator and In x Ga 1-x As QW channel. The dependency of the energy separation between $E_{F}$ and $E_{C}$ on the surface of the In x Ga 1-x As QW channel upon $V_{GS}$ enables construction of the charge–voltage behaviors of In x Ga 1-x As/In 0.52 Al 0.48 As QW FETs. To develop a unified, continuous and differentiable areal channel charge density ( $Q_{ch}$ ) model that is valid from the subthreshold to strong inversion regimes, the previously proposed inversion-layer transition function is further revised with three transition coefficients of $\eta $ , $\alpha $ and $\beta $ in this work. To verify the proposed approach, the results of the proposed model are compared with those of not only the numerically calculated Qch from a one-dimensional (1D) Poisson–Schrödinger solver, but also the measured gate capacitance of a fabricated In 0.7 Ga 0.3 As QW metal-insulator-semiconductor FET with large gate length, yielding excellent agreement between the simulated and measured results.