Hanearl Jung
Yonsei University
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Publication
Featured researches published by Hanearl Jung.
ACS Nano | 2013
Jeong Gyu Song; J. Park; W.S. Lee; Taejin Choi; Hanearl Jung; Chang Wan Lee; Sung Hwan Hwang; Jae Min Myoung; Jae Hoon Jung; Soo-Hyun Kim; Clement Lansalot-Matras; Hyungjun Kim
The synthesis of atomically thin transition-metal disulfides (MS2) with layer controllability and large-area uniformity is an essential requirement for their application in electronic and optical devices. In this work, we describe a process for the synthesis of WS2 nanosheets through the sulfurization of an atomic layer deposition (ALD) WO3 film with systematic layer controllability and wafer-level uniformity. The X-ray photoemission spectroscopy, Raman, and photoluminescence measurements exhibit that the ALD-based WS2 nanosheets have good stoichiometry, clear Raman shift, and bandgap dependence as a function of the number of layers. The electron mobility of the monolayer WS2 measured using a field-effect transistor (FET) with a high-k dielectric gate insulator is shown to be better than that of CVD-grown WS2, and the subthreshold swing is comparable to that of an exfoliated MoS2 FET device. Moreover, by utilizing the high conformality of the ALD process, we have developed a process for the fabrication of WS2 nanotubes.
Nature Communications | 2015
Jeong-Gyu Song; Gyeong Hee Ryu; Su Jeong Lee; Sangwan Sim; Chang Wan Lee; Taejin Choi; Hanearl Jung; Youngjun Kim; Zonghoon Lee; Jae Min Myoung; Christian Dussarrat; Clement Lansalot-Matras; J. Park; Hyunyong Choi; Hyungjun Kim
The effective synthesis of two-dimensional transition metal dichalcogenides alloy is essential for successful application in electronic and optical devices based on a tunable band gap. Here we show a synthesis process for Mo1−xWxS2 alloy using sulfurization of super-cycle atomic layer deposition Mo1−xWxOy. Various spectroscopic and microscopic results indicate that the synthesized Mo1−xWxS2 alloys have complete mixing of Mo and W atoms and tunable band gap by systematically controlled composition and layer number. Based on this, we synthesize a vertically composition-controlled (VCC) Mo1−xWxS2 multilayer using five continuous super-cycles with different cycle ratios for each super-cycle. Angle-resolved X-ray photoemission spectroscopy, Raman and ultraviolet–visible spectrophotometer results reveal that a VCC Mo1−xWxS2 multilayer has different vertical composition and broadband light absorption with strong interlayer coupling within a VCC Mo1−xWxS2 multilayer. Further, we demonstrate that a VCC Mo1−xWxS2 multilayer photodetector generates three to four times greater photocurrent than MoS2- and WS2-based devices, owing to the broadband light absorption.
ACS Applied Materials & Interfaces | 2013
Sanggeun Lee; Juree Hong; Ja Hoon Koo; Hyonik Lee; Seulah Lee; Taejin Choi; Hanearl Jung; Bon-Woong Koo; J. Park; Hyungjun Kim; Young-Woon Kim; Taeyoon Lee
We report the fabrication of graphene-encapsulated nanoballs with copper nanoparticle (Cu NP) cores whose size range from 40 nm to 1 μm using a solid carbon source of poly(methyl methacrylate) (PMMA). The Cu NPs were prone to agglomerate during the annealing process at high temperatures of 800 to 900 °C when gas carbon source such as methane was used for the growth of graphene. On the contrary, the morphologies of the Cu NPs were unchanged during the growth of graphene at the same temperature range when PMMA coating was used. The solid source of PMMA was first converted to amorphous carbon layers through a pyrolysis process at the temperature regime of 400 °C, which prevented the Cu NPs from agglomeration, and they were converted to few-layered graphene (FLG) at the elevated temperatures. Raman and transmission electron microscope analyses confirmed the synthesis of FLG with thickness of approximately 3 nm directly on the surface of the Cu NPs. X-ray diffraction and X-ray photoelectron spectroscopy analyses, along with electrical resistance measurement according to temperature changes showed that the FLG-encapsulated Cu NPs were highly resistant to oxidation even after exposure to severe oxidation conditions.
Applied Physics Letters | 2012
Hyemin Kang; J. Park; Taejin Choi; Hanearl Jung; Kwang Hoon Lee; Seongil Im; Hyungjun Kim
Core-shell p-n junction diode was fabricated using the atomic layer deposition (ALD) of ZnO on p-Si nanowire (NW) array prepared by electroless etching method. I-V measurements have shown that the carrier concentrations in ALD ZnO for both of the core-shell and planar diodes are effectively controlled by nitrogen doping to a proper level to form rectifying junction. Responsivity of the core-shell device was about 0.98 A/W at 660 nm, which is significantly improved compared to planar device. The superior sensitivity of core-shell structure is attributed to the effective carrier separation and collection originating from the characteristic of core-shell NWs full depletion.
Scientific Reports | 2016
Youngjun Kim; Jeong Gyu Song; Yong Ju Park; Gyeong Hee Ryu; Su Jeong Lee; Jin Sung Kim; Pyo Jin Jeon; Chang Wan Lee; Whang Je Woo; Taejin Choi; Hanearl Jung; Han Bo Ram Lee; Jae Min Myoung; Seongil Im; Zonghoon Lee; Jong Hyun Ahn; J. Park; Hyungjun Kim
This work reports the self-limiting synthesis of an atomically thin, two dimensional transition metal dichalcogenides (2D TMDCs) in the form of MoS2. The layer controllability and large area uniformity essential for electronic and optical device applications is achieved through atomic layer deposition in what is named self-limiting layer synthesis (SLS); a process in which the number of layers is determined by temperature rather than process cycles due to the chemically inactive nature of 2D MoS2. Through spectroscopic and microscopic investigation it is demonstrated that SLS is capable of producing MoS2 with a wafer-scale (~10 cm) layer-number uniformity of more than 90%, which when used as the active layer in a top-gated field-effect transistor, produces an on/off ratio as high as 108. This process is also shown to be applicable to WSe2, with a PN diode fabricated from a MoS2/WSe2 heterostructure exhibiting gate-tunable rectifying characteristics.
ACS Applied Materials & Interfaces | 2014
Hanearl Jung; J. Park; Il Kwon Oh; Taejin Choi; Sanggeun Lee; Juree Hong; Taeyoon Lee; Soo-Hyun Kim; Hyungjun Kim
Without introducing defects in the monolayer of carbon lattice, the deposition of high-κ dielectric material is a significant challenge because of the difficulty of high-quality oxide nucleation on graphene. Previous investigations of the deposition of high-κ dielectrics on graphene have often reported significant degradation of the electrical properties of graphene. In this study, we report a new way to integrate high-κ dielectrics with graphene by transferring a high-κ dielectric nanosheet onto graphene. Al2O3 film was deposited on a sacrificial layer using an atomic layer deposition process and the Al2O3 nanosheet was fabricated by removing the sacrificial layer. Top-gated graphene field-effect transistors were fabricated and characterized using the Al2O3 nanosheet as a gate dielectric. The top-gated graphene was demonstrated to have a field-effect mobility up to 2200 cm(2)/(V s). This method provides a new method for high-performance graphene devices with broad potential impacts reaching from high-frequency high-speed circuits to flexible electronics.
RSC Advances | 2015
Yun Cheol Kim; Su Jeong Lee; Hanearl Jung; Bo Eun Park; Hyungjun Kim; Woong Lee; Jae Min Myoung
Structural optimization of the indium zinc oxide (IZO)–Ag–IZO oxide–metal–oxide (OMO) transparent flexible electrode structure was carried out in terms of the thickness of the Ag layer based on the Haacke figure of merit. While showing sufficient sheet resistance and visible transmittance, the optimized OMO structure also exhibited good resistance to fracture under repeated bending which resulted in very small change in sheet resistance over the 10 000 cycles of repeated bending. Low sheet resistance was found to be beneficial to lowering the contact resistances at the source and drain electrodes when the OMO structure was applied to a model thin film transistor (TFT) as revealed in the improved device performances. Device application potential of the OMO structure was demonstrated in a fully transparent TFT formed on a glass substrate in which the source, drain, and back gate electrodes were all formed using the OMO structure.
Applied Physics Letters | 2016
Ki Seok Kim; Il Kwon Oh; Hanearl Jung; Hyungjun Kim; Geun Young Yeom; Kyong Nam Kim
The polymer residue generated during the graphene transfer process to the substrate tends to cause problems (e.g., a decrease in electron mobility, unwanted doping, and non-uniform deposition of the dielectric material). In this study, by using a controllable low-energy Ar+ ion beam, we cleaned the polymer residue without damaging the graphene network. HfO2 grown by atomic layer deposition on graphene cleaned using an Ar+ ion beam showed a dense uniform structure, whereas that grown on the transferred graphene (before Ar+ ion cleaning) showed a non-uniform structure. A graphene–HfO2–metal capacitor fabricated by growing 20-nm thick HfO2 on graphene exhibited a very low leakage current (<10−11 A/cm2) for Ar+ ion-cleaned graphene, whereas a similar capacitor grown using the transferred graphene showed high leakage current.
RSC Advances | 2014
Yongwon Chung; Sanggeun Lee; Chandreswar Mahata; Jungmok Seo; Seung Min Lim; Min Su Jeong; Hanearl Jung; Young-Chang Joo; Young Bae Park; Hyungjun Kim; Taeyoon Lee
In this work, we have demonstrated chemically coupled (3-aminopropyl)trimethoxysilane (APTMS) and 3-mercaptopropionic acid (MPA) self-assembled monolayers (SAMs) to enhance the diffusion barrier properties against copper (Cu) as well as the adhesion properties towards SiO2 and Cu electrode. The coupled-SAM (C-SAM) can attach to both Cu and SiO2 strongly which is expected to enhance both the diffusion barrier and adhesion properties. A carbodiimide-mediated amidation process was used to link NH2 terminated APTMS to COOH terminated MPA. The resulting C-SAM shows a low root-mean-square roughness of 0.44 nm and a thickness of 2 nm. Time-dependent dielectric breakdown (TDDB) tests are used to evaluate APTMS and C-SAM for their ability to block Cu ion diffusion. The average time-to-failure (TTF) is enhanced over 4 times after the MPA attachment, and is even comparable to TaN barriers. Capacitance–voltage (C–V) measurements are also conducted to monitor Cu ion diffusion. Negligible change in the flatband voltage and C–V curve is observed during the constant voltage stress C–V measurement. Enhancement of the adhesion properties are measured using four-point bending tests and shows that the C-SAM has a 33% enhancement in the adhesion properties between SiO2 and Cu compared to APTMS. The C-SAM shows potential as an ultra-thin Cu diffusion barrier which also has good adhesion properties.
ACS Applied Materials & Interfaces | 2018
Hanearl Jung; Woo-Hee Kim; Bo-Eun Park; Whang Je Woo; Il-Kwon Oh; Su Jeong Lee; Yun Cheol Kim; Jae Min Myoung; Satoko Gatineau; Christian Dussarrat; Hyungjun Kim
We report the effect of Y2O3 passivation by atomic layer deposition (ALD) using various oxidants, such as H2O, O2 plasma, and O3, on In-Ga-Zn-O thin-film transistors (IGZO TFTs). A large negative shift in the threshold voltage (Vth) was observed in the case of the TFT subjected to the H2O-ALD Y2O3 process; this shift was caused by a donor effect of negatively charged chemisorbed H2O molecules. In addition, degradation of the IGZO TFT device performance after the O2 plasma-ALD Y2O3 process (field-effect mobility (μ) = 8.7 cm2/(V·s), subthreshold swing (SS) = 0.77 V/dec, and Vth = 3.7 V) was observed, which was attributed to plasma damage on the IGZO surface adversely affecting the stability of the TFT under light illumination. In contrast, the O3-ALD Y2O3 process led to enhanced device stability under light illumination (ΔVth = -1 V after 3 h of illumination) by passivating the subgap defect states in the IGZO surface region. In addition, TFTs with a thicker IGZO film (55 nm, which was the optimum thickness under the current investigation) showed more stable device performance than TFTs with a thinner IGZO film (30 nm) (ΔVth = -0.4 V after 3 h of light illumination) by triggering the recombination of holes diffusing from the IGZO surface to the insulator-channel interface. Therefore, we envisioned that the O3-ALD Y2O3 passivation layer suggested in this paper can improve the photostability of TFTs under light illumination.