Jaephil Shim

Dr. Jaephil Shim


Research Focus & Metrics

Academic Career Length

5Years (2022-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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25 December 2022 in Micromachines
Verified
Journal Article
Open access
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SSSeung Heon Shin
Seung Heon Shin
JSJaephil Shim
Jaephil Shim
HJhyunchul jang
hyunchul jang
JJJae-Hyung Jang
Jae-Hyung Jang
In this work, we successfully demonstrated In0.53Ga0.47As/InAs/In0.53Ga0.47As composite channel metamorphic high electron mobility transistors (mHEMTs) on a GaAs substrate. The fabricated mHEMTs with a 100 nm gate length exhibited excellent DC and logic characteristics such as VT = −0.13 V, gm,max = 949 mS/mm, subthreshold swing (SS) = 84 mV/dec, drain-induced barrier lowering (DIBL) = 89 mV/V, and Ion/Ioff ratio = 9.8 × 103 at a drain-source voltage (VDS) = 0.5 V. In addition, the device exhibited excellent high-frequency characteristics, such as fT/fmax = 261/304 GHz for the measured result and well-matched modeled fT/fmax = 258/309 GHz at VDS = 0.5 V, which is less power consumption compared to other material systems. These high-frequency characteristics are a well-balanced demonstration of fT and fmax in the mHEMT structure on a GaAs substrate.

9 September 2023 in Materials
Verified
Journal Article
Open access
PDF file
KSKiyong Shin
Kiyong Shin
JSJu-Won Shin
Ju-Won Shin
WAWalid Amir
Walid Amir
SCSurajit Chakraborty
Surajit Chakraborty
JSJaephil Shim
Jaephil Shim
TKTae-Woo Kim
Tae-Woo Kim
Our investigation focused on assessing the influence of the metamorphic buffer in metamorphic high-electron-mobility transistors (MHEMT) that were grown on GaAs substrates. While an MHEMT exhibited elevated off-state current levels, its direct current (DC) and radio frequency (RF) traits were found to be comparable to those of InP-based lattice-matched high-electron-mobility transistors (LM-HEMTs). However, the Pulsed I–V measurement results confirmed the presence of the fast transient charging effect, leading to a more substantial degradation in drain current observed in MHEMT. In addition, through the low-frequency noise characteristics, it was confirmed that the dominant trapping location was located in the bulk site. The slope of the 1/f noise measurement indicated that the primary trapping site was in proximity to the bulk traps. The carrier-number-fluctuation (CNF) model was employed to extract the bulk trap density (Nt). For the LM-HEMTs, the value was at 3.27 × 1016 eV−1·cm−3, while for the MHEMT, it was 3.56 × 1017 eV−1·cm−3.