농문 황

Prof. Dr. 농문 황

Seoul National University College of Engineering
orcid

Research Focus & Metrics

Academic Career Length

29Years (1998-Present)

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

Representative Publications

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1 September 2016 in Carbon
Verified
Journal Article
Closed access
JPJin-Woo Park
Jin-Woo Park
KKKun-Su Kim
Kun-Su Kim
농문 황농문 황
농문 황

24 October 2020 in Coatings
Verified
Journal Article
Open access
PDF file
SLSeungjun Lee
Seungjun Lee
JLJaehoo Lee
Jaehoo Lee
WKWoongsik Kim
Woongsik Kim
농문 황농문 황
농문 황
Dense yttrium oxyfluoride (YOF) coating was successfully deposited by suspension plasma spraying (SPS) with coaxial feeding. After deposition for 6 min at a plasma power of 105 kW, the thickness of the YOF coating was 55 ± 3.2 µm with a porosity of 0.15% ± 0.01% and the coating rate was ~9.2 µm/min. The crystalline structure of trigonal YOF was confirmed by X-ray diffractometry (XRD). The etching behavior of the YOF coating was studied using inductively coupled CHF3/Ar plasma in comparison with those of the Al2O3 bulk and Y2O3 coating. Crater-like erosion sites and cavities were formed on the whole surface of the Al2O3 bulk and Y2O3 coating. In contrast, the surface of the YOF coating showed no noticeable difference before and after exposure to the CHF3/Ar plasma. Such high resistance of the YOF coating to fluorocarbon plasma comes from the strongly fluorinated layer on the surface. The fluorination on the surface of materials was confirmed by X-ray photoelectron spectrum analysis (XPS). Depth profiles of the compositions of Al2O3, Y2O3, and YOF samples by XPS revealed that the fluorination layer of the YOF coating was much thicker than those of Al2O3 and Y2O3. These results indicate that if the inner wall of the semiconductor process chamber is coated by YOF using SPS, the generation of contamination particles would be minimized during the fluorocarbon plasma etching process.

1 August 2016 in Acta Materialia
Verified
Journal Article
Closed access
TNTae-Wook Na
Tae-Wook Na
HPHyung-Ki Park
Hyung-Ki Park
CPChang-Soo Park
Chang-Soo Park
JPJong-Tae Park
Jong-Tae Park
농문 황농문 황
농문 황

31 August 2009 in Carbon
Verified
Journal Article
Closed access
CKChan-Soo Kim
Chan-Soo Kim
YCYung-Bin Chung
Yung-Bin Chung
WYWoong-Kyu Youn
Woong-Kyu Youn
농문 황농문 황
농문 황

25 February 2019 in International Journal of Precision Engineering and Manufacturing-Green Technology
Verified
Journal Article
Closed access
PDF file
HJHye-Jin Jeong
Hye-Jin Jeong
JPJu-Won Park
Ju-Won Park
KJKyeong Jae Jeong
Kyeong Jae Jeong
농문 황농문 황
농문 황
Sung-Tae HongSung-Tae Hong
Sung-Tae Hong
HHHeung Nam Han
Heung Nam Han

2 January 2009 in Aerosol Science and Technology
Verified
Journal Article
Open access
CKChan-Soo Kim
Chan-Soo Kim
YCYung-Bin Chung
Yung-Bin Chung
WYWoong-Kyu Youn
Woong-Kyu Youn
농문 황농문 황
농문 황
We measured the size distribution of positively and negatively charged nanoparticles generated abundantly in the gas phase during the syntheses of ZnO nanowires by a carbothermal reduction process using a differential mobility analyzer. Under the conditions where these charged nanoparticles were not generated, no nanowires could be grown. The evolution of ZnO nanostructures on the substrate was studied with in-situ measurements of the size distribution of charged nanoparticles with varying reactor temperature and oxygen flow rate. The results suggest that the electrostatic energy arising from charged nanoparticles would play a critical role in the growth of ZnO nanowires.