19 results on '"S Baang"'
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2. New Trends in Wide Bandgap Semiconductors: Synthesis of Single Crystalline Silicon Carbide Layers by Low Pressure Chemical Vapor Deposition Technique on P-Type Silicon (100 and/or 111) and their Characterization
- Author
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M. Yasin, Adnan Ali, M. Asghar, A. Mehmood, Hasan, A.S. Gerges, Faisal Iqbal, S. Baang, and A. Raja
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Materials science ,Silicon ,Mechanical Engineering ,Analytical chemistry ,Wide-bandgap semiconductor ,Energy-dispersive X-ray spectroscopy ,chemistry.chemical_element ,Substrate (electronics) ,Chemical vapor deposition ,Carbide ,chemistry ,Mechanics of Materials ,General Materials Science ,Crystalline silicon ,Fourier transform infrared spectroscopy - Abstract
We report the growth of SiC layers on low cost p-type silicon (100 and/or 111) substrates maintained at constant temperature (1050 - 1350oC, ∆T=50oC) in a low pressure chemical vapor deposition reactor. Typical Fourier transform infrared spectrum showed a dominant peak at 800 cm-1 due to Si-C bond excitation. Large area x-ray diffraction spectra revealed single crystalline cubic structures of 3C-SiC(111) and 3C-SiC(200) on Si(111) and Si(100) substrates, respectively. Cross-sectional views exposed by scanning electron microscopy display upto 104 µm thick SiC layer. Energy dispersive spectroscopy of the layers demonstrated stiochiometric growth of SiC. Surface roughness and morphology of the films were also checked with the help of atomic force microscopy. Resistivity of the as-grown layers increases with increasing substrate temperature due to decrease of isolated intrinsic defects such as silicon and/or carbon vacanies having activation energy 0.59 ±0.02 eV.
- Published
- 2010
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3. Design and construction of the KSTAR tokamak
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G.S. Lee, M. Kwon, C.J. Doh, B.G. Hong, K. Kim, M.H. Cho, W. Namkung, C.S. Chang, Y.C. Kim, J.Y. Kim, H.G. Jhang, D.K. Lee, K.I. You, J.H. Han, M.C. Kyum, J.W. Choi, J. Hong, W.C. Kim, B.C. Kim, J.H. Choi, S.H. Seo, H.K. Na, H.G. Lee, S.G. Lee, S.J. Yoo, B.J. Lee, Y.S. Jung, J.G. Bak, H.L. Yang, S.Y. Cho, K.H. Im, N.I. Hur, I.K. Yoo, J.W. Sa, K.H. Hong, G.H. Kim, B.J. Yoo, H.C. Ri, Y.K. Oh, Y.S. Kim, C.H. Choi, D.L. Kim, Y.M. Park, K.W. Cho, T.H. Ha, S.M. Hwang, Y.J. Kim, S. Baang, S.I. Lee, H.Y. Chang, W. Choe, S.G. Jeong, S.S. Oh, H.J. Lee, B.H. Oh, B.H. Choi, C.K. Hwang, S.R. In, S.H. Jeong, I.S. Ko, Y.S. Bae, H.S. Kang, J.B. Kim, H.J. Ahn, D.S. Kim, J.H. Lee, Y.W. Lee, Y.S. Hwang, S.H. Hong, K.-H. Chung, D.-I. Choi, and KSTAR Team
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Nuclear and High Energy Physics ,Electric power system ,Tokamak ,law ,Nuclear engineering ,KSTAR ,Plasma shaping ,Divertor ,Water cooling ,Plasma diagnostics ,Superconducting magnet ,Condensed Matter Physics ,law.invention - Abstract
The extensive design effort for KSTAR has been focused on two major aspects of the KSTAR project mission - steady-state-operation capability and advanced tokamak physics. The steady state aspect of the mission is reflected in the choice of superconducting magnets, provision of actively cooled in-vessel components, and long pulse current drive and heating systems. The advanced tokamak aspect of the mission is incorporated in the design features associated with flexible plasma shaping, double null divertor and passive stabilizers, internal control coils and a comprehensive set of diagnostics. Substantial progress in engineering has been made on superconducting magnets, the vacuum vessel, plasma facing components and power supplies. The new KSTAR experimental facility with cryogenic system and deionized water cooling and main power systems has been designed, and the construction work is under way for completion in 2004.
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- 2001
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4. The KSTAR project: An advanced steady state superconducting tokamak experiment
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G.S Lee, J Kim, S.M Hwang, C.S Chang, H.Y Chang, M.H Cho, B.H Choi, K Kim, K.W Cho, S Cho, K.K Choh, C.H Choi, J.H Choi, J.W Choi, I.S Choi, C.J Do, T.H Ha, J.H Han, J.S Hong, K.H Hong, N.I Hur, I.S Hwang, K.H Im, H.G Jhang, Y.S Jung, B.C Kim, D.L Kim, G.H Kim, H.S Kim, J.S Kim, J.Y Kim, W.C Kim, Y.S Kim, K.H Kwon, M.C Kyum, B.J Lee, D.K Lee, H.G Lee, J.M Lee, S.G Lee, H.G Na, Y.K Oh, J.H Park, H.C Ri, Y.S Ryoo, K.Y Song, H.L Yang, J.G Yang, B.J Yoo, S.J Yoo, N.S Yoon, S.B Yoon, G.H You, K.I You, W Choe, D.-I Choi, S.G Jeong, D.Y Lee, Y.S Bae, H.S Kang, G.N Kim, I.S Ko, W Namkung, J.S Oh, Y.D Bae, Y.S Cho, B.G Hong, G Hong, C.K Hwang, S.R In, M.H Ju, H.J Lee, B.H Oh, B.J Yoon, S Baang, H.J Choi, J Hwang, M.G Kim, Y.J Kim, S.I Lee, J Yee, C.S Yoon, K.-H Chung, S.H Hong, Y.S Hwang, S.H Kim, Y.H Kim, K.H Chung, J.Y Lim, D.W Ha, S.S Oh, K.S Ryu, Q.L Wang, T.K Ko, J Joo, S Suh, J.H Lee, Y.W Lee, H.S Shin, I.H Song, J Baek, I.Y Han, Y Koh, P.Y Park, C Ryu, J.J Cho, D.M Hwang, J.A Schmidt, H.K Park, G.H Neilson, W.T Reiersen, R.T Simmons, S Bernabei, F Dahlgren, L.R Grisham, S.C Jardin, C.E Kessel, J Manickam, S.S Medley, N Pomphrey, J.C Sinnis, T.G Brown, R.B White, K.M Young, J Schultz, P.W Wang, L Sevier, M.D Carter, P.M Ryan, D.W Swain, D.N Hill, W.M Nevins, and B.J Braams
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Physics ,Nuclear and High Energy Physics ,Tokamak ,Divertor ,Nuclear engineering ,Cyclotron ,Pulse duration ,Plasma ,Fusion power ,Condensed Matter Physics ,law.invention ,Nuclear magnetic resonance ,law ,Magnet ,KSTAR - Abstract
The Korea Superconducting Tokamak Advanced Research (KSTAR) project is the major effort of the national fusion programme of the Republic of Korea. Its aim is to develop a steady state capable advanced superconducting tokamak to establish a scientific and technological basis for an attractive fusion reactor. The major parameters of the tokamak are: major radius 1.8 m, minor radius 0.5 m, toroidal field 3.5 T and plasma current 2 MA, with a strongly shaped plasma cross-section and double null divertor. The initial pulse length provided by the poloidal magnet system is 20 s, but the pulse length can be increased to 300 s through non-inductive current drive. The plasma heating and current drive system consists of neutral beams, ion cyclotron waves, lower hybrid waves and electron cyclotron waves for flexible profile control in advanced tokamak operating modes. A comprehensive set of diagnostics is planned for plasma control, performance evaluation and physics understanding. The project has completed its conceptual design and moved to the engineering design and construction phase. The target date for the first plasma is 2002.
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- 2000
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5. Fundamental investigation of reflectometry as a density fluctuation diagnostic (invited)
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T. L. Rhodes, Neville C. Luhmann, S. Baang, W. A. Peebles, Calvin Domier, and A. E. Chou
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Physics ,Turbulence ,Wavenumber ,Experimental data ,Perturbation (astronomy) ,Spatial localization ,Plasma diagnostics ,Atomic physics ,Reflectometry ,Instrumentation ,Electromagnetic radiation ,Computational physics - Abstract
Reflectometry is currently used to monitor density fluctuations and turbulent correlation lengths in fusion plasmas. Various models have been used to interpret the experimental data and to determine the regimes of validity of the reflectometer fluctuation measurements. Heretofore, these models have not been validated by direct comparison with experiment. In this paper the first comparison between a controlled laboratory experiment and a one‐dimensional numerical model is presented. It is found that the model is unable to predict the observed high degree of spatial localization and dependence on perturbation wave number. The implications of these disagreements are discussed, together with suggestions for their resolution.
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- 1992
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6. Fluctuation measurements in the DIII‐D and TEXT tokamaks via collective scattering and reflectometry
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C. X. Yu, Neville C. Luhmann, K. H. Burrell, R. J. Groebner, Rolf Philipona, D. L. Brower, S. Baang, T. L. Rhodes, E. J. Doyle, H. Matsumoto, C. L. Rettig, W. A. Peebles, and T. Lehecka
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Physics ,Tokamak ,DIII-D ,Turbulence ,business.industry ,Scattering ,Phase (waves) ,law.invention ,Computational physics ,Optics ,Physics::Plasma Physics ,law ,Microturbulence ,Plasma diagnostics ,Reflectometry ,business ,Instrumentation - Abstract
Anomalous transport in fusion plasmas remains an enigma requiring explanation. A predictive capability is highly desirable if confinement enhancement regimes such as H mode or super shots are to be extrapolated to the next phase in development of the International Fusion program, epitomized, for example in ITER. Therefore, identification of the role that electrostatic turbulence plays in confinement is a critical issue requiring detailed experimental data capable of testing and challenging existing theoretical models. This article presents microturbulence measurements obtained on the DIII‐D and TEXT tokamaks utilizing heterodyne, far‐infrared collective scattering, and reflectometry techniques. The experimental systems are described on both machines and emphasis placed on results obtained during the L‐H transition, ELM activity, and saturated ohmic operation where ion temperature gradient driven (ITGD) turbulence is theoretically predicted to exist.
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- 1990
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7. Electron density measurement for microwave-induced atmospheric pressure plasmas using laser deflection method
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Wonho Choe, S. Baang, Junghee Kim, S.Y. Moon, and Seung Hun Lee
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Electron density ,Materials science ,Atmospheric pressure ,business.industry ,Physics::Optics ,Plasma ,Laser ,law.invention ,symbols.namesake ,Optics ,Stark effect ,Plasma torch ,law ,symbols ,Plasma diagnostics ,Atomic physics ,business ,Refractive index - Abstract
Summary form only given. A laser beam passing through plasma deflects due to a change in the line-integrated refractive index, which is attributed to an electron density gradient along the chord. By measuring the deflection angle of the laser beam, the electron density was obtained for an atmospheric pressure microwave-induced torch plasma generated in the ambient air. The diagnostic set-up, consisting of a low power He-Ne laser, a four channel segmented position-sensitive photodiode detector, and some relevant optical components, demands modest requirements of laser quality and optics alignments. The measured electron density was compared with that obtained by optical emission spectroscopy based on the measured Stark broadening width of the Balmer H-beta line emitted from the plasma. Both the multi channel deflection method and the optical emission method showed the same order of magnitude (~1015 cm-3) electron density values. Comparison of the detailed results will be presented.
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- 2007
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8. The KSTAR superconducting magnet system
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L. Myatt, P. Michel, W. Reiersen, H. Choi, J.H. Schultz, K. Kim, Alexey Radovinsky, Thomas Brown, S. Baang, and P.W. Wang
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Superconductivity ,Physics ,Thermonuclear fusion ,Tokamak ,Field (physics) ,Superconducting magnet ,Inductor ,Computer Science::Computers and Society ,Physics::Geophysics ,law.invention ,Nuclear physics ,chemistry.chemical_compound ,chemistry ,Physics::Plasma Physics ,law ,Condensed Matter::Superconductivity ,KSTAR ,Niobium-tin - Abstract
The Korean Superconducting Tokamak Advanced Research (KSTAR) at the Korea Basic Science Institute in Taejon will be the first Tokamak with an advanced all superconducting magnet system, including toroidal field (TF), poloidal field (PF),and field error correction (FEC) coils. The conductors are all cable-in-conduit (CICC) superconductors with a single conduit similar to those in the International Thermonuclear Experimental Reactor (ITER).
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- 2002
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9. The KSTAR tokamak
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D.W. Swain, M.C. Kyum, M. Joo, J.C. Sinnis, Won Namkung, S. Baang, B.H. Choi, W. Reiersen, S.M. Hwang, Neil Pomphrey, J.Y. Lim, Kie-hyung Chung, S.R. In, W. M. Nevins, D.K. Lee, J.S. Hong, J.H. Schultz, B. Montgomery, D.L. Kim, C.H. Cho, Y.K. Oh, D.-I. Choi, G.H. You, L. Sevier, D.Y. Lee, K.H. Im, K.S. Kim, F. Dahlgren, Thomas Brown, Moo-Hyun Cho, R.T. Simmons, J. A. Schmidt, J. Manickam, Hyeon K. Park, S. Bernabei, L. R. Grisham, C.E. Kessel, Yong-Seok Hwang, Y.S. Cho, S.G. Lee, George H. Neilson, J.H. Park, W.C. Kim, H.Y. Chang, Kyekyoon Kim, P.W. Wang, Y.S. Jung, J.Y. Kim, B.J. Yoon, B.Y. Lee, K.-H. Chung, S. Cho, D. N. Hill, J.G. Yang, SeulChan Hong, J.H. Han, Jinchoon Kim, Stephen Jardin, N.I. Huh, B.G. Hong, Choong-Seock Chang, K. Young, G.S. Lee, and H.G. Jhang
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Physics ,Tokamak ,Toroid ,business.industry ,Nuclear engineering ,Divertor ,Electrical engineering ,Superconducting magnet ,law.invention ,Conceptual design ,law ,Plasma shaping ,Magnet ,KSTAR ,business - Abstract
The KSTAR (Korea Superconducting Tokamak Advanced Research) project is the major effort of the Korean National Fusion Program to design, construct, and operate a steady-state-capable superconducting tokamak. The project is led by Korea Basic Science Institute and shared by national laboratories, universities, and industry along with international collaboration. It is in the conceptual design phase and aims for the first plasma by mid 2002. The key design features of KSTAR are: major radius 1.8 m, minor radius 0.5 m, toroidal field 3.5 T, plasma current 2 MA, and flexible plasma shaping (elongation 2.0; triangularity 0.8; double-null poloidal divertor). Both the toroidal and the poloidal field magnets are superconducting coils. The device is configured to be initially capable of 20 s pulse operation and then to be upgraded for operation up to 300 s with non-inductive current drive. The auxiliary heating and current drive system consists of neutral beam, ICRF, lower hybrid, and ECRF. Deuterium operation is planned with a full radiation shielding.
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- 2002
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10. The results of performance tests of superconducting wires for KSTAR magnets
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S. Baek, H. Park, M. Kim, S. Baang, Q. Wang, Y. Chu, S. Lee, K. Kim, and Y. Chang
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Residual resistivity ,Materials science ,Fabrication ,Tokamak ,law ,Magnet ,KSTAR ,Nuclear engineering ,Eddy current ,Cryogenics ,Rod ,law.invention - Abstract
The Korean Superconducting Tokamak Advanced Research device consists of 16 TF coils and 14 PF coils. All TF and PF coils are superconducting. Among them, 16 TF coils and 10 PF coils are made from Nb3Sn and the other 4 coils (PF 6 and 7, up/down) are made from NbTi. It is estimated that total 27 tons of Nb3Sn and 11 tons of NbTi are required for the fabrication of KSTAR magnets. The superconducting 8 mm rods are supplied by Mitsubishi Electric Corporation (MELCO) and Intermagnetics General Corporation (IGC) and processed to the final chromium plated 0.78 mm diameter strands by Nexans Korea and KISWIRE. Currently, about 6 tons of Nb3Sn strands have been produced, and the performance tests for them have been carried out. The specimens for the strand performance tests are taken from the both ends of the strand lot. In this paper, we present the latest test results of the current carrying capacity of non-copper volume, hysteresis loss of non-copper volume and residual resistivity ratio using statistical analysis.
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- 2002
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11. Spatial resolution of microwave/millimeter‐wave reflectometry
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Neville C. Luhmann, W. A. Peebles, T. L. Rhodes, Calvin Domier, and S. Baang
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Physics ,business.industry ,Acoustic wave ,Electromagnetic radiation ,Optics ,Physics::Plasma Physics ,Extremely high frequency ,Wavenumber ,Plasma diagnostics ,business ,Reflectometry ,Instrumentation ,Image resolution ,Microwave - Abstract
Reflectometry is currently being used to investigate density fluctuations and turbulence in tokamak plasmas. However, there are unresolved questions about the spatial resolution and wave number sensitivity of this diagnostic method which impact the interpretation of the data. These questions are currently being addressed in a cylindrical, pulsed filament discharge plasma where ion acoustic waves (10–100 kHz) are launched toward the incident microwaves. Preliminary data supporting the spatially localized nature of reflectometry are presented. A computational model is also being developed to provide quantitative comparisons with experiment.
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- 1990
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12. Plasma diagnostic reflectometry
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B. B. Afeyan, Neville C. Luhmann, John C. Garrison, Calvin Domier, Bruce I. Cohen, T. B. Kaiser, A.E. Chou, and S. Baang
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Engineering ,business.industry ,Nuclear engineering ,Iter tokamak ,Reflectometry ,National laboratory ,business ,Simulation - Abstract
Theoretical and experimental studies of plasma diagnostic reflectometry have been undertaken as a collaborative research project between the Lawrence Livermore National Laboratory (LLNL) and the University of California Department of Applied Science Plasma Diagnostics Group under the auspices of the Laboratory Directed Research and Development Program at LLNL. Theoretical analyses have explored the basic principles of reflectometry to understand its limitations, to address specific gaps in the understanding of reflectometry measurements in laboratory experiments, and to explore extensions of reflectometry such as ultra-short-pulse reflectometry. The theory has supported basic laboratory reflectometry experiments where reflectometry measurements can be corroborated by independent diagnostic measurements.
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- 1996
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13. Fluctuation measurements in the DIII‐D and TEXT tokamaks via collective scattering and reflectometry (abstract)
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W. A. Peebles, S. Baang, D. L. Brower, K. Burrell, E. J. Doyle, R. J. Groebner, T. Lehecka, N. C. Luhmann, H. Matsumoto, R. Philipona, C. Rettig, T. L. Rhodes, and C. X. Yu
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Instrumentation - Published
- 1990
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14. Analyzing Acceptor-like State Distribution of Solution-Processed Indium-Zinc-Oxide Semiconductor Depending on the In Concentration.
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Kim D, Lee H, Yun Y, Park J, Zhang X, Bae JH, and Baang S
- Abstract
Understanding the density of state (DOS) distribution in solution-processed indium-zinc-oxide (IZO) thin-film transistors (TFTs) is crucial for addressing electrical instability. This paper presents quantitative calculations of the acceptor-like state distribution of solution-processed IZO TFTs using thermal energy analysis. To extract the acceptor-like state distribution, the electrical characteristics of IZO TFTs with various In molarity ratios were analyzed with respect to temperature. An Arrhenius plot was used to determine electrical parameters such as the activation energy, flat band energy, and flat band voltage. Two calculation methods, the simplified charge approximation and the Meyer-Neldel (MN) rule-based carrier-surface potential field-effect analysis, were proposed to estimate the acceptor-like state distribution. The simplified charge approximation established the modeling of acceptor-like states using the charge-voltage relationship. The MN rule-based field-effect analysis validated the DOS distribution through the carrier-surface potential relationship. In addition, this study introduces practical and effective approaches for determining the DOS distribution of solution-processed IZO semiconductors based on the In molarity ratio. The profiles of the acceptor-like state distribution provide insights into the electrical behavior depending on the doping concentration of the solution-processed IZO semiconductors.
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- 2023
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15. Investigation on Atomic Bonding Structure of Solution-Processed Indium-Zinc-Oxide Semiconductors According to Doped Indium Content and Its Effects on the Transistor Performance.
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Kim D, Lee H, Kim B, Baang S, Ejderha K, Bae JH, and Park J
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The atomic composition ratio of solution-processed oxide semiconductors is crucial in controlling the electrical performance of thin-film transistors (TFTs) because the crystallinity and defects of the random network structure of oxide semiconductors change critically with respect to the atomic composition ratio. Herein, the relationship between the film properties of nitrate precursor-based indium-zinc-oxide (IZO) semiconductors and electrical performance of solution-processed IZO TFTs with respect to the In molar ratio was investigated. The thickness, morphological characteristics, crystallinity, and depth profile of the IZO semiconductor film were measured to analyze the correlation between the structural properties of IZO film and electrical performances of the IZO TFT. In addition, the stoichiometric and electrical properties of the IZO semiconductor films were analyzed using film density, atomic composition profile, and Hall effect measurements. Based on the structural and stoichiometric results for the IZO semiconductor, the doping effect of the IZO film with respect to the In molar ratio was theoretically explained. The atomic bonding structure by the In doping in solution-processed IZO semiconductor and resulting increase in free carriers are discussed through a simple bonding model and band gap formation energy.
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- 2022
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16. Atomic Structure Evaluation of Solution-Processed a -IZO Films and Electrical Behavior of a -IZO TFTs.
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Kim D, Lee H, Kim B, Zhang X, Bae JH, Choi JS, and Baang S
- Abstract
Understanding the chemical reaction pathway of the metal-salt precursor is essential for modifying the properties of solution-processed metal-oxide thin films and further improving their electrical performance. In this study, we focused on the structural growth of solution-processed amorphous indium-zinc-oxide ( a -IZO) films and the electrical behavior of a -IZO thin-film transistors (TFT). To this end, solution-processed a -IZO films were prepared with respect to the Zn molar ratio, and their structural characteristics were analyzed. For the structural characteristic analysis of the a -IZO film, the cross-section, morphology, crystallinity, and atomic composition characteristics were used as the measurement results. Furthermore, the chemical reaction pathway of the nitrate precursor-based IZO solution was evaluated for the growth process of the a -IZO film structure. These interpretations of the growth process and chemical reaction pathway of the a -IZO film were assumed to be due to the thermal decomposition of the IZO solution and the structural rearrangement after annealing. Finally, based on the structural/chemical results, the electrical performance of the fabricated a -IZO TFT depending on the Zn concentration was evaluated, and the electrical behavior was discussed in relation to the structural characteristics.
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- 2022
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17. Semitransparent Thin-Film Dual-Metal Anode for Red-Phosphorescent Organic Light-Emitting Diodes.
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Zhang X, Lee HW, Lee H, Baang S, and Park J
- Abstract
Semitransparent dual-metal electrodes comprising several thin layers of metals, such as Ni, Ag, Cu, and Al, were developed for designing flexible red-phosphorescent organic light-emitting diodes (OLEDs). The said diodes were fabricated by first depositing a Ni layer on four glass and polyethylene terephthalate (PET) substrates each to facilitate adhesion with glass and a flexible PET substrate. Subsequently, a conductive layer of Ni, Ag, Cu, and Al was stacked atop the first Ni layer on the four glass and PET substrates each, respectively. The proof of principles has been employed to demonstrate the performance potential via optical, physical, and electrical analyses of dual-as well as single-metal layers prior to device realization. In addition, their electrical and optical characteristics were compared against those of In-Sn-oxide-based OLEDs to demonstrate their potential with regard to application flexibility.
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- 2021
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18. Illumination Effect on Electrical Characteristics of Poly(3-hexylthiophene-2,5-diyl) Thin-Film Transistors.
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Shin H, Park J, Baang S, and Choi JS
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We investigate the electrical characteristics of solution-processed poly(3-hexylthiophene-2,5-diyl) (P3HT) thin-film transistors (TFTs) under monochromatic illumination conditions at different wavelengths of 700, 655, 515, and 315 nm. The TFT characteristics measured under light illumination at the wavelengths of 700 and 655 nm were comparable to those measured in the dark state. In addition, light illumination at a wavelength of 515 nm, of which photon energy (~2.4 eV) is higher than the band gap energy of P3HT (~1.7 eV), had a little effect on the electrical characteristics of P3HT TFTs. On the other hand, the TFT performance was notably changed by light illumination at a wavelength of 315 nm. These results indicate that the photon energy, which cause the characteristic degradation in the solution-processed P3HT TFTs, is much higher than the band gap energy of P3HT. Consequently, the illumination-induced variation in the TFT performance can be understood through a broad distribution of energetic states in the solution-processed P3HT semiconductor.
- Published
- 2020
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19. Signal modeling with random scatterers for confocal microwave imaging.
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Baang S, Lee YU, Park CY, and Dae Kim J
- Abstract
Microwave breast tumor detection uses the electrical property contrast between normal tissues and malignancies to detect the latter in an early development stage. However, previous works on the microwave imaging uses 2-D or more complicated models of the breast and electromagnetic wave propagation. We present a computationally efficient and physically instructive electromagnetic wave channel modeling for confocal microwave imaging system for the breast tumor detection. The proposed model covers all of the factors that have been examined in the previous 2-D model, such as the radial spreading, path loss, partial reflection and transmission of the backscattered electromagnetic wave from the tumor cell. The characteristics of the reconstructed images of the tumor using the proposed 1-D model are compared with them of the previous 2-D FDTD method. Previous 2-D model of the cancerous breast utilizes the MRI-derived discretized cell model to simulate the realistic perturbation, but there has been no consideration on the system noise that can be detrimental to the reconstruction of the tumor. The effect of the system noise level to the reconstruction algorithm will be addressed as well.
- Published
- 2005
- Full Text
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