• Title/Summary/Keyword: Si/O-doped

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Effects of Oxygen on the Properties of Mg-doped Zinc Tin Oxide Films Prepared by rf Magnetron Sputtering (rf 마그네트론 스퍼터링으로 증착한 Mg-doped Zinc Tin Oxide막의 특성에 미치는 산소의 영향)

  • Park, Ki Cheol;Ma, Tae Young
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.26 no.5
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    • pp.373-379
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    • 2013
  • Mg-doped zinc tin oxide (ZTO:Mg) thin films were prepared on glasses by rf magnetron sputtering. $O_2$ was introduced into the chamber during the sputtering. The optical properties of the films as a function of oxygen flow rate were studied. The crystal structure, elementary properties, and depth profiles of the films were investigated by X-ray diffraction (XRD), x-ray photoelectron spectroscopy (XPS), and secondary ion mass spectrometry (SIMS), respectively. Bottom-gate transparent thin film transistors were fabricated on $N^+$ Si wafers, and the variation of mobility, threshold voltage etc. with the oxygen flow rate were observed.

Property analysis of Hafnium doped Aluminum-Zinc-Oxide films (Hf의 도핑에 따른 Al-Zn-O 박막의 물성 분석)

  • Lee, Sang-Hyuk;Jun, Hyun-Sik;Park, Jin-Seok
    • Proceedings of the KIEE Conference
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    • 2015.07a
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    • pp.1149-1150
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    • 2015
  • In this study, hafnium was doped into aluminum zinc oxide (AZO) films were deposited on glass and Si substrates at room temperature via co-sputtering by varying the electric power applied to the Hf target. The properties of deposited Hf-doped AZO films, such as crystalline structure, optical transmittance, and band gap were analyzed using various methods such as X-ray diffraction (XRD) and UV/visible spectrophotometer. The experimental results confirmed that the abovementioned properties of Hf-AZO films strongly depended on the Hf sputtering power.

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Detection of Bio-chemical by Boron-doped Diamond Electrode (붕소가 도핑된 다이아몬드 전극을 이용한 생체화학물질의 검출)

  • Lee, Eun-Ju;Fujishima, A.;Park, Soo-Gil
    • Proceedings of the KIEE Conference
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    • 2002.11a
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    • pp.167-169
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    • 2002
  • Selective, highly stable determination of serotonin was achieved in cyclic voltammetric measurement carried out at electrochemically treated conductive boron-doped diamond electrode. Boron-doped diamond electrodes were prepared on single crystal Si wafers by microwave plasma chemical vapor deposition and $B_2O_3$ was dissolved in acetone/methanol(9:1) mixture solution so that the B/C weight ratio ca. $10^4ppm$. Serotonin is a kind of indoleamines, which secreted from adrenal marrow cells. The serious problem to detection of serotonin is the interference phenomena of electroactive constituent, including AA. In this study, electrochemical treatment of HDD was carried out to discriminate between serotonin and AA responses. Experimental results showed that the peak potential of AA oxidation shift to the positive direction and the oxidation peak of serotonin was unchanged.

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Synthesis and Formation Mechanism of Cobalt Doped Willemite Blue Pigments (Co-Doped Willemite 파란색 안료의 합성과 생성기구)

  • Hwang, Dong-Ha;Han, Kyong-Sop;Lee, Byung-Ha
    • Journal of the Korean Ceramic Society
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    • v.47 no.6
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    • pp.603-607
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    • 2010
  • Turquoise blue pigment of Vanadium-zircon blue (DCMA number 14-42-2), which was already commercialized, was stable to be reproduced but insufficient to give strong blue. However, it possible to obtain more intense blue by partially substituting cobalt ions into the willemite($Zn_2SiO_4$) lattice classified into DCMA number 7-10-2 for blue ceramic pigment. By the composition of willemite $Co_xZn_{2-x}SiO_4$(X=0.01, 0.03, 0.05, 0.07, 0.09 mole), this study used reagent grade zinc oxide, cobalt oxide and silicon dioxide as starting materials, carrying out the synthesis with solid reaction method by adding $H_3BO_3$ as a mineralizer. The firing temperature was between $1200^{\circ}C$ and $1400^{\circ}C$. The characteristics of synthesized pigment were analyzed by X-ray diffraction, Raman spectroscopy and SEM and the characteristics of color tones were analyzed by UV-Vis spectroscopy and CIE-$L^*a^*b^*$ measurement. As a result, the optimal composition was $Zn_{1.95}Co_{0.05}$ with 1wt% of $H_3BO_3$ as a mineralizer and firing condition was $1350^{\circ}C$/3 h. $L^*a^*b^*$ value was 29.25, 41.03, -59.93 for on glaze pigment and 37.03, 36.41, -60.03 for under glaze pigment.

Effect of Posphorus Dopants in the Thermal Oxidation of Tungsten Polycide Films (텅스텐 폴리사이드막의 열산화에서 인 불순물 효과)

  • 정회환;정관수
    • Journal of the Korean Vacuum Society
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    • v.4 no.3
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    • pp.293-300
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    • 1995
  • p-doped poly-Si/SiO2/Si 기판위에 저압 화학증착법(LPCVD)으로 증착한 텅스텐 실리사이드(WS2.7)막을$ 850^{\circ}C$에서 20분 동안 N2 분위기에서 열처리한 후에 건식 분위기에서 열산화하였다. 다결정 실리콘의 인도핑(doping)레벨에 따른 텅스텐 폴리사이드(WSi2.5/poly-Si)막의 산화 성장률과 텅스텐 폴리사이드막의 산화 메카니즘에 대하여 연구하였다. 텅스텐 폴리사이드막의 산화 성장률은 다결정 실리콘의 인(p) 도핑 레벨이 증가함에 따라 증가하였다. 텅스텐 폴리사이드막의 산화는 텅스텐 실리사이드층의 과잉(excess)Si가 초기 산화과정 동안 소모된 후에 다결정 실리콘층의 Si가 소모되었다. 산화막과 산화막을 식각(etching)한 후에 텅스텐 실리사이드막의 표면 거칠기는 다결정 실리?의 인 농도가 적을수록 평탄하였다.

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Photoluminescence properties of oxy-fluoride glass-ceramics of La2O3-CaF2-Al2O3-SiO2 system (La2O3-CaF2-Al2O3-SiO2 계 oxy-fluoride 결정화 유리의 광 발광 특성)

  • Ha, Taewan;Kang, Seunggu
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.31 no.2
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    • pp.84-88
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    • 2021
  • The change of the photoluminescence properties of La2O3-CaF2-Al2O3-SiO2 glass-ceramics doped with rare earth material, that is used as laser and optical sensors, was analyzed according to heat treatment temperature. The heat treatment conditions for fabricating glass-ceramics were obtained through non-isothermal thermal analysis, and X-ray diffraction analysis was performed to determine the degree of crystal growth and kinds of crystal phases generated according to the heat treatment temperature. Using Scherrer's equation, it was predicted that crystals with a size of 25~40 nm would be generated inside the glass-ceramics. Photoluminescence (PL) analysis showed that the specimens heat-treated at 660℃ to 670℃ for 1 hour had the highest PL intensity. Also, from the CIE color coordinate analysis, all glass-ceramics specimens emitted red-orange light regardless of the heat treatment condition.

Electrical and Chemical Properties of ultra thin RT-MOCVD Deposited Ti-doped $Ta_2O_5$

  • Lee, S. J.;H. F. Luan;A. Mao;T. S. Jeon;Lee, C. h.;Y. Senzaki;D. Roberts;D. L. Kwong
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.1 no.4
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    • pp.202-208
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    • 2001
  • In Recent results suggested that doping $Ta_2O_5$ with a small amount of $TiO_2$ using standard ceramic processing techniques can increase the dielectric constant of $Ta_2O_5$ significantly. In this paper, this concept is studied using RTCVD (Rapid Thermal Chemical Vapor Deposition). Ti-doped $Ta_2O_5$ films are deposited using $TaC_{12}H_{30}O_5N$, $C_8H_{24}N_4Ti$, and $O_2$ on both Si and $NH_3$-nitrided Si substrates. An $NH_3$-based interface layer at the Si surface is used to prevent interfacial oxidation during the CVD process and post deposition annealing is performed in $H_2/O_2$ ambient to improve film quality and reduce leakage current. A sputtered TiN layer is used as a diffusion barrier between the Al gate electrode and the $TaTi_xO_y$ dielectric. XPS analyses confirm the formation of a ($Ta_2O_5)_{1-x}(TiO_2)_x$ composite oxide. A high quality $TaTi_xO_y$ gate stack with EOT (Equivalent Oxide Thickness) of $7{\AA}$ and leakage current $Jg=O.5A/textrm{cm}^2$ @ Vg=-1.0V has been achieved. We have also succeeded in forming a $TaTi_x/O_y$ composite oxide by rapid thermal oxidation of the as-deposited CVD TaTi films. The electrical properties and Jg-EOT characteristics of these composite oxides are remarkably similar to that of RTCVD $Ta_2O_5, suggesting that the dielectric constant of $Ta_2O_5$ is not affected by the addition of $TiO_2$.

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Synthesis of Uniformly Doped Ge Nanowires with Carbon Sheath

  • Kim, Tae-Heon;;Choe, Sun-Hyeong;Seo, Yeong-Min;Lee, Jong-Cheol;Hwang, Dong-Hun;Kim, Dae-Won;Choe, Yun-Jeong;Hwang, Seong-U;Hwang, Dong-Mok
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.08a
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    • pp.289-289
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    • 2013
  • While there are plenty of studies on synthesizing semiconducting germanium nanowires (Ge NWs) by vapor-liquid-solid (VLS) process, it is difficult to inject dopants into them with uniform dopants distribution due to vapor-solid (VS) deposition. In particular, as precursors and dopants such as germane ($GeH_4$), phosphine ($PH_3$) or diborane ($B_2H_6$) incorporate through sidewall of nanowire, it is hard to obtain the structural and electrical uniformity of Ge NWs. Moreover, the drastic tapered structure of Ge NWs is observed when it is synthesized at high temperature over $400^{\circ}C$ because of excessive VS deposition. In 2006, Emanuel Tutuc et al. demonstrated Ge NW pn junction using p-type shell as depleted layer. However, it could not be prevented from undesirable VS deposition and it still kept the tapered structures of Ge NWs as a result. Herein, we adopt $C_2H_2$ gas in order to passivate Ge NWs with carbon sheath, which makes the entire Ge NWs uniform at even higher temperature over $450^{\circ}C$. We can also synthesize non-tapered and uniformly doped Ge NWs, restricting incorporation of excess germanium on the surface. The Ge NWs with carbon sheath are grown via VLS process on a $Si/SiO_2$ substrate coated 2 nm Au film. Thin Au film is thermally evaporated on a $Si/SiO_2$ substrate. The NW is grown flowing $GeH_4$, HCl, $C_2H_2$ and PH3 for n-type, $B_2H_6$ for p-type at a total pressure of 15 Torr and temperatures of $480{\sim}500^{\circ}C$. Scanning electron microscopy (SEM) reveals clear surface of the Ge NWs synthesized at $500^{\circ}C$. Raman spectroscopy peaked at about ~300 $cm^{-1}$ indicates it is comprised of single crystalline germanium in the core of Ge NWs and it is proved to be covered by thin amorphous carbon by two peaks of 1330 $cm^{-1}$ (D-band) and 1590 $cm^{-1}$ (G-band). Furthermore, the electrical performances of Ge NWs doped with boron and phosphorus are measured by field effect transistor (FET) and they shows typical curves of p-type and n-type FET. It is expected to have general potentials for development of logic devices and solar cells using p-type and n-type Ge NWs with carbon sheath.

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Electrical and Optical Properties of Ga-doped SnO2 Thin Films Via Pulsed Laser Deposition

  • Sung, Chang-Hoon;Kim, Geun-Woo;Seo, Yong-Jun;Heo, Si-Nae;Huh, Seok-Hwan;Chang, Ji-Ho;Koo, Bon-Heun
    • Journal of Surface Science and Engineering
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    • v.44 no.4
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    • pp.144-148
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    • 2011
  • $Ga_2O_3$ doped $SnO_2$ thin films were grown by using pulsed laser deposition (PLD) technique on glass substrate. The optical and electrical properties of these films were investigated for different doping concentrations, oxygen partial pressures, substrate temperatures, and film thickness. The films were deposited at different substrate temperatures (room temperature to $600^{\circ}C$). The best opto-electrical properties is shown by the film deposited at substrate temperature of $300^{\circ}C$ with oxygen partial pressure of 80 m Torr and the gallium concentration of 2 wt%. The as obtained lowest resistivity is $9.57{\times}10^{-3}\;{\Omega}cm$ with the average transmission of 80% in the visible region and an optical band gap (indirect allowed) of 4.26 eV.

Investigation of thermal annealing effects on the optical transparency and luminescent characteristics of Eu-doped Y2O3 thin films

  • Chung, Myun Hwa;Kim, Joo Han
    • Journal of Ceramic Processing Research
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    • v.20 no.4
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    • pp.431-435
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    • 2019
  • The thermal annealing effects on the optical transparency and luminescent characteristics of the Eu-doped Y2O3 thin films have been investigated. The as-deposited Y2O3:Eu films exhibited an optical band gap of 5.78 eV with a transparency of 89 % at a wavelength of 550 nm. As the annealing temperature increased from 1000 to 1300 ℃, the optical band gap and transparency of the films decreased from 5.77 to 4.91 eV and from 86.8 to 64.5 % at 550 nm, respectively. The crystalline quality of the films was improved with increasing annealing temperature. The annealed Y2O3:Eu films emitted a red-color photoluminescence (PL) with the highest emission peak near 612 nm. The PL intensity was increased with increasing annealing temperature to 1200 ℃, resulting from the improvement in the crystalline quality of the films. The PL intensity was decreased with further increasing temperature above 1200 ℃ due to the formation of Y2SiO5 phase by the reaction of the film with the quartz substrate.