Ho-Gi Kim’s research while affiliated with Korea Advanced Institute of Science and Technology and other places

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Publications (184)


Effect of a Fullerene Derivative on the Performance of TiO2-Nanotube-Based Dye-Sensitized Solar Cells
  • Article

February 2012

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55 Reads

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12 Citations

Journal of Nanoscience and Nanotechnology

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Woong-Rae Kim

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Changduk Yang

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[...]

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Highly ordered TiO2 nanotube arrays were prepared by anodic oxidation of Ti foil in an application to dye-sensitized solar cells (DSCs). A fullerene derivative called PC61BM was used as a material for the surface modification of TiO2 nanotube arrays to improve the power conversion efficiency of DSCs Although open circuit voltages (Voc) were slightly decreased by PC61BM interlayer, short circuit current densities (Jsc) were increased and thus the power conversion efficiencies were improved. EIS (Electrochemical Impedance Spectroscopy) results showed superior properties for PC61BM-coated samples.


Highly sensitive SnO 2 hollow nanofiber-based NO 2 gas sensors

December 2011

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35 Reads

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95 Citations

Sensors and Actuators B Chemical

SnO2 hollow nanofibers (HNFs) with diameters of 300–500nm were fabricated via electrospinning of templating nanofibers and RF-sputtering of SnO2 thin overlayers (15–20nm thick and comparable grain size) followed by heat-treatment at 450°C. Gas sensors using these HNFs exhibited n-type gas sensing characteristics and an enhanced gas response to 2ppm NO2 (Rgas/Rair=81.4) as compared to that (Rgas/Rair=19.9) of planar SnO2 thin films. The enhanced response to NO2 is attributed to the greater accessible active area and the greater space charge modulation depth associated with the hollow thin walled structures.


Gas sensing properties of p-type hollow NiO hemispheres prepared by polymeric colloidal templating method

July 2011

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154 Reads

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132 Citations

Sensors and Actuators B Chemical

This work presents a simple and versatile route to produce macroporous p-type metal oxide thin films. Two-dimensional arrays of p-type NiO films with a hollow hemisphere structure were fabricated by colloidal templating and RF-sputtering followed by a subsequent heat treatment. The diameter and shell thickness of the NiO hemisphere were 800nm and 20nm, respectively. X-ray diffraction and high-resolution transmission electron microscopy analysis indicate that the pure NiO phase with grain size of 10nm was obtained at calcination temperatures that exceeded 450°C. Close-packed arrays of hollow NiO hemispheres were found to exhibit p-type gas sensing properties against (CO, H2, C3H8, CH4, NO2, and C2H5OH), leading to significantly enhanced responses to C2H5OH (Rgas/Rair=5.0 at 200ppm).


Surface modification effects of [Li,La]TiO3 on the electrochemical performance of Li[Ni0.35Co0.3Mn0.35]O2 cathode material for lithium–ion batteries

May 2011

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41 Reads

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6 Citations

Journal of Applied Electrochemistry

Surface modification of Li[Ni0.35Co0.3Mn0.35]O2 as a cathode material of lithium–ion batteries was carried out by hydrothermal treatment using lithium lanthanum titanate ([Li,La]TiO3). The modified surfaces were analyzed by morphology observation using transmission electron microscopy and by element investigation using X-ray photoelectron spectroscopy. It was thereupon found that the [Li,La]TiO3-coated layer formed by the surface modification played a definitive role in suppressing the solid electrolyte interface during repeated charge and discharge cycles. In addition, the thermal stability was enhanced by coated layer, resulting in an increase of the onset temperature to occur an exothermic reaction during thermal runaway. KeywordsSurface coating–Lithium lanthanum titanate–Cathode–Lithium–ion batteries


Effects of protecting layer [Li,La]TiO 3 on electrochemical properties of LiMn 2O 4 for lithium batteries

March 2011

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20 Reads

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28 Citations

Journal of Alloys and Compounds

A sample of LiMn2O4 spinel oxide was surface-modified with lithium lanthanum titanate ([Li,La]TiO3), which was developed as a lithium ionic conductor, by means of hydrothermal processing and subsequent heat treatment at 400°C. The surface coating layers were analyzed by morphology observation using a transmission electron microscopy. Energy-dispersive spectrometry and X-ray photoelectron spectroscopy were used for element investigation. The surface modification effects on rate capability during cycling and capacity retention for the LiMn2O4 spinel oxide were confirmed. Then Mn dissolution during storage at elevated temperatures of the pristine, coated sample was characterized. The Mn dissolution characterization was based on the idea that Mn dissolution is one of the most significant reasons for capacity loss for LiMn2O4 spinel oxide, and this phenomenon is especially severe at elevated temperatures. Our experimental results indicate that the surface-modified sample shows much a better initial capacity and rate capability compared with the pristine sample. The [Li,La]TiO3 coating effectively enhances the structural stability of LiMn2O4 at elevated temperatures, most likely because the [Li,La]TiO3-modifying layers play a definitive role in suppressing Mn dissolution in the electrolyte during storage.


Fabrication of dye-sensitized solar cells by transplanting highly ordered TiO2 nanotube arrays

January 2011

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52 Reads

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131 Citations

Solar Energy Materials and Solar Cells

Highly ordered TiO2 nanotube arrays fabricated by anodization are very attractive to dye-sensitized solar cells (DSCs) due to their superior charge percolation and slower charge recombination. However, the efficiency of TiO2-nanotube-based DSCs is 6.89%, which is still lower than that of TiO2-nanoparticle-based DSCs. We have suggested the transplanting the highly ordered TiO2 nanotube arrays to FTO glass to improve the performance of TiO2-nanotube-based DSCs. DSCs based on transplanted TiO2 nanotube arrays and TiO2 nanoparticles were fabricated by same process and materials to exclude the unexpected factors. In TiO2 thickness of ca. 15 μm, the efficiency of 2.91% in front-side illuminated DSCs based on TiO2 nanotube arrays was higher than those in back-side illuminated DSCs based on TiO2 nanotube arrays and in front-side illuminated DSCs based on TiO2 nanoparticle. Front-side illuminated DSCs based on TiO2 nanotube arrays having various thicknesses were successfully fabricated. The efficiency in DSCs having 20.0 μm thick TiO2 nanotube arrays was improved to 5.36% by TiCl4 treatment.


Characterization on Bandedge Electronic Structure of MgO Added Bi1.5Zn1.0Nb1.5O7 Gate Dielectrics for ZnO-Thin Film Transistors

January 2011

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8 Reads

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2 Citations

Electrochemical and Solid State Letters

Significantly reduced leakage current characteristics of the Bi1.5Zn1.0Nb1.5O7 (BZN) gate dielectric for producing high-performance ZnO-thin film transistors (TFTs) were achieved by an addition of MgO (30 atom %). The overall TFT parameters using MgO-BZN gate insulator against those that used pure BZN dielectric were enhanced remarkably. The diphasic MgO-BZN composite oxide structure was confirmed by an analysis of the spectroscopically detected bandedge electronic structures. The bandgap energy of MgO-BZN was identical to that of BZN at similar to 3.3 eV, but the Fermi energy level was shifted to 1.2 eV from 0.6 eV for BZN against the valence bandedge.


Reparation and Characterization of BST Thin Films with Hybrid Bottom Electrodes

January 2011

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4 Reads

Materials Research Society symposia proceedings. Materials Research Society

Thin platinum layer was used for the modification of the interface state between (Ba,Sr)TiO3 (BST) thin films and RuO2 bottom electrodes. Pt/RuO2 hybrid bottom electrodes were fabricated with various platinum deposition temperatures by a conventional dc magnetron sputtering method. Although the surface morphology and XRD patterns of BST thin films were not changed, the electrical properties of BST films deposited on Pt/RuO2 hybrid electrodes were improved compared to the films on RuO2 electrodes. Dielectric constant (εr) and leakage current density of BST thin films on Pt/RuO2 hybrid electrodes prepared at the platinum deposition temperature of 400°C were 498 and 8.6 × 10−8 A/cm2 at 1.5V, respectively.


Facile synthesis and electrochemical properties of RuO2 nanofibers with ionically conducting hydrous layer

October 2010

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34 Reads

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62 Citations

Journal of Materials Chemistry

The facile synthesis, by electrospinning of highly conductive RuO2 fiber mats as the conducting core of electrochemical capacitors, is reported. Electrospun RuO2 fiber mats, calcined at 400 °C, exhibited highly porous morphologies composed of crystalline RuO2 nano-particles with an average particle size of 10 nm. The highly conducting (σ = 288 S cm−1) fiber mats were used as the basis of a hybrid electrochemical capacitor in which the fiber mats served as the conducting core for electrochemically deposited hydrate RuO2·nH2O overlayers. These electrochemical capacitors exhibited superior characteristics: a high specific capacitance of 886.9 F g−1 (based on the mass of the hydrous RuO2 coating layer) at scan rate of 10 mV s−1 and high rate capability with a capacity loss of only 30% from 10 to 2000 mV s−1. This is attributed to the superior electron transport pathways provided by the fiber mat core to the upper ionically conducting hydrous RuO2 coating layer.


Figure 1 shows current-transient curves obtained during anodic oxidation of Ti foil. Figure 1(a) gives the current-time behavior when the anodization voltage increases from 0 V to 60 V at the ramping speed of 1 V/s. In the early stage of voltage ramping, the current, which flows from Ti anode to Pt cathode, abruptly decreases due to the formation of thin TiO 2 layer on Ti foil. However, after ~4 seconds, the current increases in proportion to the ramping time. It seems that the as-formed TiO 2 layer on Ti foil is not thick enough to block the current flow thus the current is proportional to the ramping voltage. A current-transient curve obtained at a constant voltage of 60 V during anodizing process can be shown in Fig. 1(b). At the beginning the current increases to some extent because etching of thin TiO 2 layer on Ti foil by F ions exposes Ti metal. However, the exposed surface of Ti metal is readily converted to thin TiO 2 layer thus the current decreases according to the anodizing time. TiO 2 nanotube structures start to be formed from the moment at which the current decreases. Directional etching of TiO 2 and Ti by F-ions induced by an applied voltage makes possible to fabricate highly ordered TiO 2 nanotube arrays. Figure 2 shows FESEM images of TiO 2 nanotube arrays obtained by anodic oxidation of Ti foil in 0.3 wt·% NH 4 F contained ethylene glycol solution. Figures 2(a)-(c) give the cross-section images obtained by anodization at a constant voltage of 60 V for 20, 30, and 40 minutes, respectively. The thickness of TiO 2 nanotube arrays increased from 18 µm for 20 minutes anodization to 30.8 µm for 40 minutes anodization. In ethylene glycol solution, the movement of F-ions is slow thus the etching speed for the surface of TiO 2 nanotube arrays is lower than that in aqueous solution [15, 19, 20]. Longer nanotube arrays up to 1,000 µm can be obtained by controlling NH 4 F concentration, anodizing time, anodizing voltage, etc. [20]. The bottom and cross-section images of TiO 2 nanotube arrays can be shown in Fig. 2(d). TiO 2 nanotube arrays were close-packed together and the bottom of each TiO 2 nanotube was blocked. The diameter, wall thickness, pore size of each TiO 2 nanotube were ~120 nm, ~40 nm, ~40 nm, respectively. Figure 3 shows FETEM images of annealed TiO 2 nanotube arrays. Figure 3(a) is the magnified image of part A in the inset figure and Fig. 3(b) gives the magnified image of part B in Fig. 3(a). There are several crystal fringes in Fig. 3(a) and each fringe has a different orientation. From these results, we can know that the annealed TiO 2 nanotube arrays have a polycrystalline structure 
Characterizations of Highly Ordered TiO 2 Nanotube Arrays Obtained by Anodic Oxidation
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  • Full-text available

June 2010

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108 Reads

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25 Citations

Transactions on Electrical and Electronic Materials

This paper provides the properties of TiO_2 nanotube arrays which are fabricated by anodic oxidation of Ti metal. Highly ordered TiO_2 nanotube arrays could be obtained by anodic oxidation of Ti foil in 0.3\;wt{\cdot}%NH_4F contained ethylene glycol solution at 30^{\circ}C. The length, pore size, wall thickness, tube diameter etc. of TiO_2 nanotube arrays were analyzed by field emission scanning electron microscopy. Their crystal properties were studied by field emission transmission electron microscopy and X-ray photoelectron spectroscopy.

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Citations (69)


... The energy management methods try to explain how energy is distributed between batteries and fuel cells following some rules and criteria determined and specified by the vehicle's system as shown in [10]- [13]. They can optimize the fuel cell capacities and consumption depending on energy demands as described in [14], [15]. ...

Reference:

Evaluation of energy management system of a hybrid energy source in EV
Power Control Strategy for Fuel Cell Hybrid Electric Vehicles
  • Citing Conference Paper
  • March 2003

SAE Technical Papers

... In Refs. [29,57,58,68,69], the authors have presented algorithms based on least squares (LS) for various battery state estimations, such as SoC and SoH. Least square estimation-based methods consider input data and model states and parameters as deterministic signals. ...

Available Power and Energy Prediction Using a Simplified Circuit Model of HEV Li-ion Battery
  • Citing Article
  • April 2010

SAE Technical Papers

... Table 1 presents the determined pH(I) values. When pH is below the pH(I), the photocatalyst surface is positively charged and reversely, when pH is over the pH(I) value, the photocatalyst surface is negatively charged [82,83]. The pH(I) values of the prepared photocatalysts were found to range from 3.6 to 6.4. ...

Surface passivation of highly ordered TiO2 nanotube arrays and application to dye-sensitized solar cells using the concept of isoelectric point

Journal of the Ceramic Society of Japan

... However, pure SnO 2 nanomaterials have problems such as a long response/recovery time, high operating temperature, and poor selectivity [16,17]. Therefore, in recent years, a large number of scholars have adopted various methods to improve these problems, such as material microstructure design, precious metal composites, heterojunction generation, and doping modification [18][19][20][21][22]. Scholars have modified it by adding graphene. ...

Facile Synthesis of Pt-Functionalized SnO2 Hollow Hemispheres and Their Gas Sensing Properties
  • Citing Article
  • January 2010

... 4) In LiMn 2 O 4 nanosized systems, synthetic procedures are generally complex, cost affected, and difficult to scale up. A number of soft chemistry techniques such as sol-gel, 19) solutionphase, 20) combustion, 21) and templating methods 22) have been explored to prepare LiMn 2 O 4 . Moreover, electrochemical performances of the electrode materials are closely associated with the preparation methods. ...

Combustion Synthesis of LiMn2LiMn_2O4O_4with Citric Acid and the Effect of Post-heat Treatment
  • Citing Article
  • January 2001

Journal of the Korean Ceramic Society

... No antimony was detected. It is quite probable that the antimony source and especially the Sb itself acts as a surfactant as already has been reported for the CVD growth of germanium [28]. The in situ deposition of germanium in an antimony atmosphere prior to the growth of Ge-Sb-Te promotes the growth of flat layers by improving the coverage of the substrate. ...

Ge film growth in the presence of Sb by metal organic chemical vapor deposition
  • Citing Article
  • October 2007

... Basically, the peak intensity ratio of (003)/(104) indicates the degree of cationic dimensional order [25] and when I 003 / I 104 < 1.2 cation mixing would prevent lithiation and delithiation process [33]. In addition, c/a lattice parameter ratio refers to the layered structure [34]. ...

High-rate, high capacity ZrO2 coated Li[Li1/6Mn1/2Co1/6Ni1/6]O2 for lithium secondary batteries
  • Citing Article
  • October 2008

Journal of Applied Electrochemistry

... al. [20] After the thermal treatment, the formation of RuO 2 with rutile phase was observed to be the same as that of commercial RuO 2 . [21] The key difference of TÀ Ru/CP was the broadening of the peaks, which gives evidence on the formation of much smaller crystallite sizes. The average crystallite size estimated by Scherrer equation [D = 0.94 · λ/βcos(2θ), where λ = 0.154 nm for Cu K α radiation of X-ray and β = full width at half maximum (FWHM) at 2θ] was approximately 11 nm. ...

Facile synthesis and electrochemical properties of RuO2 nanofibers with ionically conducting hydrous layer
  • Citing Article
  • October 2010

Journal of Materials Chemistry

... It could be attributed to the larger atomic radius difference between Zn and In, which results in the poor crystallinity (Fig. 2) and interrupts smooth movement of carriers [21]. This also creates compressive or tensile deformation, which leads to the decrease in the resistivity and mobility because of the increased effective mass of electron [24]. The following equation is a way to explain above. ...

Structural and Electrical Properties of Indium Doped ZnO Thin Film on 6H-SiC Substrate by RF Magnetron Sputtering
  • Citing Article
  • June 2010

Integrated Ferroelectrics