7 results on '"Kim, Hong Seung"'
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2. Effects of Mg incorporation by co-sputtering into the ZnO channel layer of thin-film transistors
- Author
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Lee, Jong Hoon, Kim, Chang Hoi, Kim, Hong Seung, Jang, Nak Woon, Yun, Young, Do, Lee Mi, and Baek, Kyu Ha
- Published
- 2013
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3. A Study of the Growth of Single-Phase Mg0.5Zn0.5O Films for UV LED
- Author
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Kim, Hong Seung, Kim, Chang Hoi, and Yue, Lili
- Subjects
ZnO ,MgO ,UV LED ,ZnMgO - Abstract
Single-phase, high band gap energy Zn0.5Mg0.5O films were grown under oxygen pressure, using pulse laser deposition with a Zn0.5Mg0.5O target. Structural characterization studies revealed that the crystal structures of the ZnX-1MgXO films could be controlled via changes in the oxygen pressure. TEM analysis showed that the thickness of the deposited Zn1-xMgxO thin films was 50–75 nm. As the oxygen pressure increased, we found that one axis of the crystals did not show a very significant increase in the crystallization compared with that observed at low oxygen pressure. The X-ray diffraction peak intensity for the hexagonal-ZnMgO (002) plane increased relative to that for the cubic-ZnMgO (111) plane. The corresponding c-axis of the h-ZnMgO lattice constant increased from 5.141 to 5.148 Å, and the a-axis of the c-ZnMgO lattice constant decreased from 4.255 to 4.250 Å. EDX analysis showed that the Mg content in the mixed-phase ZnMgO films decreased significantly, from 54.25 to 46.96 at.%. As the oxygen pressure was increased from 100 to 150 mTorr, the absorption edge red-shifted from 3.96 to 3.81 eV; however, a film grown at the highest oxygen pressure tested here (200 mTorr)., {"references":["V. Srikantand D.R. Clarke, \"On the optical band gap of Zinc oxide,\"J. Appl. Phys. Vol. 83, pp. 5447-5451, 1998.","P. Bhattacharya, R.R. Das, and R.S. Katiyar, \"Fabrication of stable wide-band-gap ZnO/MgO multilayer thin films,\"Appl. Phys. Lett. Vol. 83, pp. 2010-2012, 2003.","M.H. Liang, Y.T. Ho, W.L. Wang, C.Y. Peng, and L. Chang, \"Growth of ZnMgO/ZnO films on r-plane sapphires by pulsed laser deposition,'J. Crystal Growth Vol. 310, pp.1847-1852, 2008.","I. Takeuchi, W. Yang, K.S. Chang, M.A. Aronova, T. Venkatesan, R.D. Vispute, and L.A. Bendersky,\"Monolithic multichannel ultraviolet detector arrays and continuous phase evolution in MgZnOcompositin spreads,\" J. Appl. Phys. Vol. 94, pp. 7336-7340, 2003.","Y. Chen, H.J. Ko, S.K. Hong, and T. Yao, \"Layer by layer growth of ZnOepilayer on Al2O3(0001) by using a MgO buffer layer,\"Appl. Phys. Lett. Vol. 76, pp.559-561, 2000.","A. Ohtomo, M. Kawasaki, T. Koida, K. Masubuchi, H. Koinuma, Y. Sakurai, Y. Yoshida, T. Yasuda, and Y. Segawa,\"MgZnO as a II-V wideband gap semiconductor alloy,\" Appl. Phys. Lett. Vol. 72 pp. 2466-2468, 1998.","C.Y. Liu, H.Y. Xu, L. Wang, X.H. Li, and Y.C. Liu, \"Pulse laser deposition of high Mg-content MgZnO films: Effects of substrate and oxygen pressure,\"J. Appl. Phys. Vol. 106, pp. 073518-1-073518-4, 2009.","Z.G. Ju, C.X. Shan, D.Y. Jiang, J.Y. Zhang, B. Yao, D.X. Zhao, D.Z. Shen, and X.W. Fan, \"MgZnO based photodetectors covering the whole solar-blind spectrum range,\"Appl. Phys. Lett. Vol. 93, pp. 173505-1-173505-3, 2008.","B.P. Zhang, N.T. Binh, K. Wakatsuki, C.Y. Liu, Y. Segawa, and N. Usami, \"Growth of ZnO/ZnMgO quantum wells on sapphire substrates and observation of the two-dimensional confinement effect,\" Appl. Phys. Lett. Vol. 86, pp. 032105-1-032105-3, 2005.\n[10]\tJ. Z, Chen, C-H. Li, and I-C. Cheng, \"Phase transition of room temperature RF-sputtered ZnO/MgZnO multilayer thin films after thermal annealing,\"Thin Solid Films Vol.520, pp.1918-1923, 2012.\n[11]\tZ. Vashaei, T. Minegishi, H. Suzuki, T. Hanada, M.W. Cho, T. Yao, and A. Setiawan,\"Structure variation of cubic and hexagonal MgZnO layer grown on MgO(111)/c-sapphire,\"J. Appl. Phys. Vol. 98, pp. 054911-1-054911-4, 2005.\n[12]\tX. Chen and J. Kang,\"The structural properties of wurtzite and rocksalt MgZnO,\"Semicond. Sci. Technol.Vol. 23, pp. 025008, 2008.\n[13]\tA. Kaushal and D. Kaur,\"Effect of Mg content on the structural, electrical and optical properties of ZnMgO nanocomposite thin films,\"Solar Energy Materials & Solar Cells Vol. 93 pp. 193-198, 2009."]}
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- 2014
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4. Characterization of magnesium oxide gate insulators grown using RF sputtering for ZnO thin-film transistors.
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Lee, Jong Hoon, Kim, Hong Seung, Kim, Sang Hyun, Jang, Nak Won, and Yun, Young
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MAGNESIUM oxide , *ELECTRIC insulators & insulation , *RADIOFREQUENCY sputtering , *THIN films , *CRYSTAL growth , *FIELD-effect transistors - Abstract
Abstract: A ZnO thin-film transistor (TFT) with an MgO insulator was fabricated on a silicon (100) substrate using a radiofrequency magnetron sputtering system. The MgO insulator was deposited using the same deposition system; the total pressure during the deposition process was maintained at 5 mTorr, and the oxygen percentage of O2/(Ar + O2) was set at 30%, 50%, or 70%. The process temperature was maintained at below 300 °C. The dielectric constant of the MgO thin layer was approximately 11.35 with an oxygen percentage of 70%. This ZnO TFT displayed enhanced transistor properties, with a field-effect mobility of 0.0235 cm2 V−1 s−1, an I ON/I OFF ratio of ∼105, and an SS value of 1.18 V decade−1; these properties were superior to those measured for the MgO insulators synthesized using oxygen percentages of 30% and 50%. [Copyright &y& Elsevier]
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- 2014
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5. The effects of thermal annealing in NH3 -ambient on the p-type ZnO films
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Jung, Eun Soo, Kim, Hong Seung, Cho, Hyung Koun, and Kim, Jin Hyeok
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PHOTOLUMINESCENCE , *MASS spectrometry , *SPECTRUM analysis , *PARTICLES (Nuclear physics) - Abstract
Abstract: Thermal annealing in NH3-ambient was carried out to form p-type ZnO films. The properties were examined by X-ray diffraction (XRD), Hall-effect measurement, photoluminescence (PL), and secondary ion mass spectrometry (SIMS). Electron concentrations in ZnO films were in the range of 1015–1017/cm3 with thermal annealing in NH3-ambient. The activation thermal annealing process was needed at 800 ∘C under N2-ambient to obtain p-type ZnO. The electrical properties of the p-type ZnO showed a hole concentration of 1.06×1016/cm3, a mobility of 15.8 cm2/V s, and a resistivity of 40.18 Ω cm. The N-doped ZnO films showed a strong photoluminescence peak at 3.306 eV at 13 K, which is closely related to neutral acceptor bound excitons of the p-type ZnO. The incorporation of nitrogen was confirmed in the SIMS spectra. [Copyright &y& Elsevier]
- Published
- 2007
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6. A study of electrical enhancement of polycrystalline MgZnO/ZnO bi-layer thin film transistors dependence on the thickness of ZnO layer.
- Author
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Lee, Jong Hoon, Jang, Nak Woon, Yun, Young, Kim, Chang Yeon, Lee, Ji Hyun, Kim, Jin-Gyu, and Kim, Hong Seung
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MAGNESIUM compounds , *POLYCRYSTALS , *ELECTRIC properties of metals , *THIN film transistors , *ZINC oxide , *MAGNETRON sputtering - Abstract
A polycrystalline MgZnO/ZnO bi-layer was deposited by using a RF co-magnetron sputtering method and the MgZnO/ZnO bi-layer TFTs were fabricated on the thermally oxidized silicon substrate. The performances with varying the thickness of ZnO layer were investigated. In this result, the MgZnO/ZnO bi-layer TFTs which the content of Mg is about 2.5 at % have shown the enhancement characteristics of high mobility (6.77–7.56 cm 2 V −1 s −1 ) and low sub-threshold swing (0.57–0.69 V decade −1 ) compare of the ZnO single layer TFT ( μ FE = 5.38 cm 2 V −1 s −1 ; S.S. = 0.86 V decade −1 ). Moreover, in the results of the positive bias stress, the ΔV on shift (4.8 V) of MgZnO/ZnO bi-layer is the 2 V lower than ZnO single layer TFT (ΔV on = 6.1 V). It reveals that the stability of the MgZnO/ZnO bi-layer TFT enhanced compared to that of the ZnO single layer TFT. [ABSTRACT FROM AUTHOR]
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- 2015
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7. The effect of Mg0.1Zn0.9O layer thickness on optical band gap of ZnO/Mg0.1Zn0.9O nano-scale multilayer thin films prepared by pulsed laser deposition method
- Author
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Cho, Ja Young, Shin, Seung Wook, Kwon, Ye Bin, Lee, Hyun-Ki, Sim, Kyu Ung, Kim, Hong Seung, Moon, Jong-Ha, and Kim, Jin Hyeok
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THICKNESS measurement , *MULTILAYERED thin films , *PULSED laser deposition , *ZINC oxide , *CRYSTAL growth , *SUPERLATTICES , *ULTRAVIOLET detectors , *ENERGY bands , *TEMPERATURE effect , *MAGNESIUM compounds - Abstract
Abstract: Epitaxial ZnO/Mg0.1Zn0.9O (MZO) nano-scale multilayer thin films were prepared on Al2O3 (0001) substrates by pulsed laser deposition. The ZnO/MZO multilayer thin films were grown by stacking alternate layers of ZnO and Mg0.1Zn0.9O with a laser fluence, repetition rate, substrate temperature and oxygen partial pressure of 3J/cm2, 5Hz, 600°C and 3.8×10−7 Pa, respectively. The thickness of an individual ZnO layer was maintained at 3nm, whereas that of the MZO layers was varied from 3nm to 15nm. Cross-sectional transmission electron microscopy revealed alternating layers of bright and dark contrast, indicating the formation of a ZnO/MZO multilayer. X-ray diffraction results showed that multilayer thin films were epitaxially grown as a hexagonal wurzite phase with orientation relationship of . The 2θ value of the (0002) peak of the ZnO/MZO multilayer thin films increased from 34.30° to 34.71°, indicating that Mg is replaced with Zn in the hexagonal lattice in the MZO of ZnO/MZO multilayer. UV–visible spectroscopy showed a systematic increase in the band gap of the ZnO/MZO multilayer thin films from 3.34eV to 3.70eV with increasing MZO layer thickness, which suggests that the band gap energy of a ZnO/MZO multilayer thin film can be controlled by varying the thickness of each constituent layer. [Copyright &y& Elsevier]
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- 2011
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