Taek Sung Kim
Chonbuk National University
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Featured researches published by Taek Sung Kim.
Electronic Materials Letters | 2012
Kyu-Hwan Shim; Ha Yong Yang; Yeon-Ho Kil; Hyeon Deok Yang; Jong-Han Yang; Woong-Ki Hong; Sukill Kang; Tae Soo Jeong; Taek Sung Kim
The nanoscale dry etching of germanium was investigated by using inductively coupled CF4 plasma and electron-beam lithography. The optimal dose of PMMA as E-beam lithography resist was ∼200 mC/cm2. When ICP Power was 200W, CF4 gas flow rate was 40 sccm, and process pressure was 20 mTorr, it had a smooth surface and good etch rate. The etching selectivity of Ge wafer to PMMA resist was as low as ∼1.5. Various sub-100 nm dry-etching patterns have been obtained. SEM pictures showed good profile qualities with a smooth etching sidewall and ultrasmall etching features.
Electronic Materials Letters | 2012
Taek Sung Kim; Yeon-Ho Kil; Hyeon Deok Yang; Jong-Han Yang; Woong-Ki Hong; Sukill Kang; Tae Soo Jeong; Kyu-Hwan Shim
Si1−xGetx QDs structures were grown onto Si/Si0.8Ge0.2 layer using RPCVD system. Ge composition in Si1−xGetx QDs was determined as about 30% and 40%. Three peaks are observed in Raman spectrum, which are located at about 520, 410, and 295 cm−1, corresponding to the vibration of Si-Si, Si-Ge, and Ge-Ge phonons, respectively, and the Si1−xGetx QDs related peak was located at 490 cm−1. The PL spectrum that originates from the radiative recombinations came from the Si substrate, the Si0.8Ge0.2 layer and Si1−xGetx QDs. For Si1−xGetx QDs, the transition peaks related to the QDs region observed in the photocurrent spectrum were preliminarily assigned to electron-heavy hole (e-hh) and electron-light hole (e-lh) fundamental excitonic transitions.
Journal of Semiconductor Technology and Science | 2013
Yeon-Ho Kil; Jong-Han Yang; Sukil Kang; Tae Soo Jeong; Taek Sung Kim; Kyu-Hwan Shim
We investigate the effect of the ageing time and etching time on the etching rate of SiGe mixed etching solution, namely 1 vp HF (6%), 2 vp H₂O₂ (30%) and 3 vp CH₃COOH (99.8%). For this etching solution, we found that the etch rate of SiGe layer is saturated after the ageing time of 72 hours, and the selectivity of Si 0.8 Ge 0.2 layer and Si layer is 20:1 at ageing time of 72 hours. The collapse was appeared at the etching time of 9min with etching solution of after saturation ageing time.
Meeting Abstracts | 2010
Taek Sung Kim; Yeon-Ho Kil; Mi Im Shin; Tae Soo Jeong; Sukil Kang; Chel-Jong Choi; Kyu-Hwan Shim
We have investigated the of Si0.8Ge0.2/Si multi-layer structures grown directly onto Si (001) substrates using reduced pressure chemical vapor deposition (RPCVD) system. The Si substrates were cleaned through a normal cleaning procedure before the Si0.8Ge0.2/Si multi-layer growth. The growth of the Si0.8Ge0.2/Si multi-layer was then commenced by switching the SiH4 and GeH4 (1.5% diluted in H2) into reactor. The flow rates of SiH4 and GeH4 were changed from 10 to 100 sccm and from 40 to 300 sccm, respectively. The flow rate of H2 was fixed at 10slm. The growth temperatures were 600°C with a growth rate of 3.2nm/min for the Si0.8Ge0.2 layer and 600°C for the Si layer with a growth rate of 3.8nm/min. Finally, the layered structures were completed by depositing a 40 nm Si cap layer. Fig. 1 shows cross-sectional TEM image of Si0.8Ge0.2/Si multi-layer with Si layer thickness of 40 nm and Si0.8Ge0.2 layer thicknesses of 20, 40 and 60 nm, respectively. Fig. 2 shows the XRD patterns of the Si0.8Ge0.2/Si multi-layer and Ge/Si layer. The XRD peak position of the SiGe(004) plane shifts to the Ge(004) plane. This indicates that the Ge concentration in the SiGe layer is 20%. Fig. 3 shows Raman spectra of the Si0.8Ge0.2/Si multi layer taken in Raman setup at a temperature of 300 K. Strong substrate peak is observed in the Raman spectra at 520 cm, denoted as SiLO–TO which corresponds to the longitudinal optical–transverse optical (LO-TO) phonon. Three peaks corresponding to the vibration of Si-Si, SiGe, and Ge-Ge phonons are observed at about 510, 410, and 300 cm, respectively. Temperature dependence of photoluminescence spectra of Si0.8Ge0.2/Si multi-layer was measured from 4 to 300 K. Figure 4 shows photoluminescence spectrum for Si0.8Ge0.2/Si multi-layer at a temperature of 4 K. This spectrum originates from the radiative recombinations both from the Si substrate and the Si0.8Ge0.2/Si multi-layer. Peaks labeled as SiGe(NP) and SiGe(TO) correspond to the no-phonon (NP) and TO-phonon assisted transition from Si0.8Ge0.2/Si multi-layer. Band-edge emission (SiGe(NP)) was clearly observed from the Si0.8Ge0.2/Si multi-layer grown by using RPCVD. From the position (or energy) of these peaks, the Ge concentration at the apex of the Si1-xGex profile can be derived. A value of 0.20 was found for this sample. Figure 5 shows the photoluminescence spectra of temperature dependence. Fig. 6 shows the photocurrent spectrum of the Si0.8Ge0.2/Si multi-layer taken in photocurrent setup at a temperature of 10 K. The photocurrent spectrum was dominated by the QWs related transition that corresponding to the transitions of the electron-heavy hole sub-band (e-hh) and electron-light hole sub-band (e-lh).
Materials Science in Semiconductor Processing | 2014
Hyeon Deok Yang; Yeon-Ho Kil; Jong-Han Yang; Sukill Kang; Tae Soo Jeong; Chel-Jong Choi; Taek Sung Kim; Kyu-Hwan Shim
Materials Science in Semiconductor Processing | 2012
K-H. Shim; Y-H. Kil; Hyeon Deok Yang; B.K. Park; J-H. Yang; Sukill Kang; T. S. Jeong; Taek Sung Kim
Meeting Abstracts | 2013
Taek Sung Kim; Yeon-Ho Kil; Woong-Ki Hong; Hyeon Deok Yang; Sukill Kang; Tae Soo Jeong; Kyu-Hwan Shim
Materials Science in Semiconductor Processing | 2013
Yeon-Ho Kil; Hyeon Deok Yang; Jong-Han Yang; Ah Hyun Park; Sukill Kang; Tae Soo Jeong; Taek Sung Kim; Kyu-Hwan Shim
Materials Science in Semiconductor Processing | 2014
Hyeon Deok Yang; Yeon-Ho Kil; Jong-Han Yang; Sukill Kang; Tae Soo Jeong; Chel-Jong Choi; Taek Sung Kim; Kyu-Hwan Shim
Electronic Materials Letters | 2011
Sukill Kang; Yeon-Ho Kil; B. G. Park; Chel-Jong Choi; Taek Sung Kim; Tae Soo Jeong; Kyu-Hwan Shim