• 제목/요약/키워드: Grain-v1

검색결과 546건 처리시간 0.033초

다공성 실리콘위에 증착된 Cu 박막의 구조적 물리적 특성 (Structuyal and physical properties of thin copper films deposited on porous silicon)

  • 홍광표;권덕렬;박현아;이종무
    • 한국진공학회지
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    • 제12권2호
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    • pp.123-129
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    • 2003
  • 다공질 실리콘(PS)기판 위에 rf-스퍼터링법으로 10~40 nm의 두께의 반 투과성 구리박막을 증착하였다. PS는 p형 (100) 실리콘 웨이퍼를 기판으로 50㎃/$\textrm{cm}^2$의 전류밀도를 사용하여 전해 에칭법으로 양극 산화하여 제작하였다. PS층과 Cu박막의 미세구조를 분석하기 위하여 SEM, AFM 그리고 XRD 분석을 시행하였다. AFM 분석결과 Cu 박막의 RMS roughness 값은 약 1.47nm로 Volmer-Weber 유형의 결정립 성장을 보였으며, 결정립의 성장은 (111) 배향성을 나타냈다. PS층의 PL 스펙트럼은 blue green 영역에서 관찰되었고, Cu 박막 증착 후 0.05eV의 blue shift가 나타났으며, 약간의 강도저하를 보였다. PS/Cu접합구조의 FTIR스펙트럼은 주 피크변화는 없으나 전반적인 강도의 감소를 보였다. I-V 특성곡선으로 본 PS/Cu 접합구조는 ideality factor가 2.77이고 barrier의 높이가 0.678eV인 Schottky 유형의 다이오드 특성을 보였다. PS/Cu 접합구조로 만든 다이오드 제조로 EL특성을 관찰할 수 있었다.

스퍼터링법으로 제작한 CIGS 박막의 후열처리에 따른 물성 평가 (Characteristic of the Sputtered CIGS Films in Relation to Heat Treatment Condition)

  • 정재헌;조상현;송풍근
    • 한국표면공학회지
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    • 제46권1호
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    • pp.16-21
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    • 2013
  • CIGS (Cu-In-Ga-Se) films were deposited on the Mo coated soda lime glass (Mo/SLG) by RF magnetron sputtering using a single sintered target with different chemical compositions. Heat treatment of the CIGS films were carried out under three different conditions, 1step ($350^{\circ}C$ for 2 hour and $550^{\circ}C$ for 2 hour) and 2step ($350^{\circ}C$ for 1 hour and $550^{\circ}C$ for 1 hour). In the case of CIGS films post-annealed on 2step method, grain size remarkably increased compared to other methods, indicating that chemical composition [Cu/(Ga+In) = 1] of CIGS films was same as CIGS target. After heat treatment by 2step method, band gap energy of the CIGS film deposited at RF 80 W showed 1.4 eV which is broadly similar to identical band gap energy (1.2 eV) of CIGS film prepared by evaporation method. Therefore, 2step heat treatment method could be expected to low temperature process.

Effects of Chamber Pressure on Dielectric Properties of Sputtered MgTiO3 Films for Multilayer Ceramic Capacitors

  • Park, Sang-Shik
    • 한국재료학회지
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    • 제20권7호
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    • pp.374-378
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    • 2010
  • $MgTiO_3$ thin films were prepared by r.f. magnetron sputtering in order to prepare miniaturized NPO type MLCCs. $MgTiO_3$ films showed a polycrystalline structure of ilmenite characterized by the appearance of (110) and (202) peaks. The intensity of the peaks decreased with an increase in the chamber pressure due to the decrease of crystallinity which resulted from the decrease of kinetic energy of the sputtered atoms. The films annealed at $600^{\circ}C$ for 60min. showed a fine grained microstructure without micro-cracks. The grain size and roughness of the $MgTiO_3$ films decreased with the increase of chamber pressure. The average surface roughness was 1.425~0.313 nm for $MgTiO_3$ films prepared at 10~70 mTorr. $MgTiO_3$ films showed a dielectric constant of 17~19.7 and a dissipation factor of 2.1~4.9% at 1MHz. The dielectric constant of the films is similar to that of bulk ceramics. The dielectric constant and the dissipation factor decreased with the increase of the chamber pressure due to the decrease of grain size and crystallinity. The leakage current density was $10^{-5}\sim10^{-7}A/cm^2$ at 200kV/cm and this value decreased with the increase of the chamber pressure. The small grain size and smooth surface microstructure of the films deposited at high chamber pressure resulted in a low leakage current density. $MgTiO_3$ films showed a near zero temperature coefficient and satisfied the specifications for NPO type materials. The dielectric properties of the $MgTiO_3$ thin films prepared by sputtering suggest the feasibility of their application for MLCCs.

Preparation and Properties of Y2O3-Doped ZrO2 Films on Etched Al Foil by Sol-Gel Process

  • Chen, Fei;Park, Sang-Shik
    • 한국재료학회지
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    • 제25권2호
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    • pp.107-112
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    • 2015
  • The oxide films formed on etched aluminum foils play an important role as dielectric layers in aluminum electrolytic capacitors. $Y_2O_3$-doped $ZrO_2$ (YZ) films were coated on the etched aluminum foils by sol-gel dip coating, and the electrical properties of YZ-coated Al foils were characterized. YZ films annealed at $450^{\circ}C$ were crystallized into a cubic phase, and as the $Y_2O_3$ doping content increased, the unit cell of $ZrO_2$ expanded and the grain size decreased. The etch pits of Al foils were filled by YZ sol when it dried at atmospheric pressure after repeating for several times, but this step could essentially be avoided when being dried in a vacuum. YZ-coated foils indicated that the specific capacitance and dissipation factor were $2-2.5{\mu}F/cm^2$ and 2-4 at 1 kHz, respectively, and the leakage current and withstanding voltage of films approximately 200 nm thick were $5{\times}10^{-4}A$ at 21 V and 22 V, respectively. After being anodized at 500 V, the foils exhibited a specific capacitance and dissipation factor of $0.6-0.7{\mu}F/cm^2$ and 0.1-0.2, respectively, at 1 kHz, while the leakage current and withstanding voltage were $2{\times}10^{-4}-3{\times}10^{-5}A$ at 400 V and 420-450 V, respectively. This suggests that YZ film is a promising dielectric that can be used in high voltage Al electrolytic capacitors.

Interfacial Energetics of All Oxide Transparent Photodiodes

  • Yadav, Pankaj;Kim, Hong-sik;Patel, Malkeshkumar;Kim, Joondong
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2016년도 제50회 동계 정기학술대회 초록집
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    • pp.390.1-390.1
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    • 2016
  • The present work explains the interfacial energetics of all oxide transparent photodiodes. The optical, structural and morphological of copper oxides were systematically analyse by UV-Visible spectrometer, X-Ray diffraction, Raman spectroscopy, Scanning electron microscopy (SEM) and Atomic force microscopy measurements (AFM). The UV-Visible result exhibits optical bandgap of Cu2O and CuO as 2.2 and 2.05 eV respectively. SEM and AFM result shows a uniform grain size distribution in Cu2O and CuO thin films with the average grain size of 45 and 40 nm respectively. The results of Current-Voltage and Kelvin probe force microscope characteristics describe the electrical responses of the Cu2O/ZnO and CuO/ZnO heterojunctions photodiodes. The obtained electrical response depicts the approximately same knee voltages with a measurable difference in the absolute value of net terminal current. More over the present study realizes the all oxide transparent photodiode with zero bias photocurrent. The presented results lay the template for fabricating and analysing the self-bias all oxide transparent photodetector.

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AISI E 52100 강(鋼)의 기계적(機械的) 성질(性質)에 미치는 탄화물(炭化物) 크기의 영향(影響) (The Effect of Carbide Size on the Mechanical Properties of AISI E 52100 Steel)

  • 최기윤;김봉완;남태운;이병권
    • 열처리공학회지
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    • 제3권4호
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    • pp.10-22
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    • 1990
  • A study has been investigated on the effect of mechanical properties (tension strength, rotary bending fatigue strength, wear resistance, hardness) according to the carbide particle size variation by the treatment of 1) quenching tempering, and 2) quenching, subzero treatment and tempering. The material used in this investigation was a typical bearing steel, high C high Cr, AISI E 52100. The result obtained in this study were as follows : (1) Finer the carbide particle size increasing the hardness and retained austenite in same quenching condition. (2) Finer the carbide particle size reduced the tension and rotary bending fatigue which were resulted from austenite grain growth and carbide precipitation on grain boundry that induced by carbide refine heat treatment. (3) Finer the carbide particel size increasing the wear resistance which were resulted by uniform distribution of carbide and increased hardness induced by microstructural uniform hardenability of matrix. (4) When the carbide particles were refinded, subzero treatment is effective only wear resistance and hardness.

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CoO 첨가량에 따른 $Pr_{6}O_{11}$계 ZnO 바리스터의 전기적 특성 (Electrical Properties of $Pr_{6}O_{11}$-Based ZnO Varistors with CoO Content)

  • 김향숙;류정선;남춘우
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2001년도 하계학술대회 논문집
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    • pp.419-422
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    • 2001
  • The electrical properties of Pr$_{6}$O$_{11}$-based ZnO varistors composed of ZnO-Pr$_{6}$O$_{11}$-CoO-Cr$_2$O$_3$-Dy$_2$O$_3$- based ceramics were investigated with CoO content in the range of 0.5~5.0 mol%. As CoO content is increased, the average grain size and the density were increased in the range of 9.86~27.22 $\mu$m and in the range of 5.25-5.55 g/cm$^3$, respectively. The varistor voltage was decreased in the range of 235.32~86.01 V/mm due to the increase of average grain size with CoO content. The varistors doped with CoO in the rage of 1.0~2.0 mol% exhibited a high nonlinearity, in which is above 55 in the nonlinear exponent and below 1.5 $\mu$A in the leakage current. Increasing CoO content further greatly decreased the nonlinearity.ity.ity.

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(Sr$_{1-x}.Ca_x)$TiO$_3$세라믹의 Ca변화량얘 따른 전기적인 특성 (Electrical Properies with Ca Contents of the (Sr$_{1-x}.Ca_x)$TiO$_3$Ceramic)

  • 김진사;정일형;신철기;김충혁;최운식;이준웅
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 1997년도 춘계학술대회 논문집
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    • pp.318-322
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    • 1997
  • The (Sr$_{l-x}$.Ca$_{x}$)TiO$_3$(0.05$\leq$x$\leq$0.2) ceramics were fabricated to form semiconducting ceramics by sintering at about 1350[$^{\circ}C$] in a reducing atmosphere($N_2$gas). After being fired in a reducing atmosphere, metal oxides, CuO, was painted on the both surface of the specimens to diffuse to the grain boundary. They were annealed at 1100[$^{\circ}C$] for 2 hours and cooled to room temperature. The grain boundary was composed of the continuous insulating layers. The capacitance changes slowly and almost linearly in the temperature region of -30~+85[$^{\circ}C$]. The capacitance characteristics appears a stable value within $\pm$10[%]. The conduction mechanism of the specimens observed in the temperature range of 25~125[$^{\circ}C$], and is divined into three regions haying different mechanism as the current increased: the region I below 230[V/cm] shows the ohmic conduction. The region II can be explained by the Poole-Frenkel emission theory, and the region III is dominated by the tunneling effect.ect.

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$(Sr_{0.50}Pb_{0.25}Ba_{0.25})TiO_3$세라믹의 유전특성에 관한 연구 (A study on the dielectric properties of the $(Sr_{0.50}Pb_{0.25}Ba_{0.25})TiO_3$ ceramics)

  • 김세일;정장호;이성갑;배선기;이영희
    • E2M - 전기 전자와 첨단 소재
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    • 제8권3호
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    • pp.267-271
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    • 1995
  • The electrical properties of (S $r_{0.50}$P $b_{0.25}$B $a_{0.25}$)Ti $O_{3}$ ceramics were studied. Specimens were prepared by the conventional mixed oxide method, and fired between 1300[.deg. C] - 1375[.deg. C], for 2[hr.]. The electrical and structural preperties of specimens were investigated with sintering temperature. Increasing the sintering temperature from 1300[.deg. C] to 1375[.deg. C], average grain size was increased from 2.61[.mu.m] to 4.53[.mu.m]. (S $r_{0.50}$P $b_{0.25}$B $a_{0.25}$)Ti $O_{3}$ specimen sintered at 1350[.deg. C] for two hours showed good dielectric constant(2147) and dielectric loss(1.7[%]) properties at 1[khz]. Sintered density and breakdown field strength were the highest value of 5.75[g/c $m^{3}$], 20[kV/cm], respectively. Dielectric properties with applied voltage were independent of the sintering temperature.temperature.

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Single Grained PZT Array Fabricated by Physical Etching of Pt Bottom Electrode

  • Park, Eung-Chul;Lee, Jang-Sik;Kim, Kwang-Ho;Park, Jung-Ho;Lee, Byung-Il
    • The Korean Journal of Ceramics
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    • 제6권1호
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    • pp.74-77
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    • 2000
  • Ta-doped PZT thin films prepared by reactive co-sputtering method could be transformed into single grained perovskite structure utilizing physical etching of Pt bottom electrode. It is found that PZT perovskite phase on damaged (111) Pt electrode by IMD was more easily crystallized than random oriented Pt electrode and less crystallized than (111) Pt electrode. This shows that amorphized Pt electrode surface by IMD process has an effect on crystallization of PZT perovskite phase. 40$\mu\textrm{m}\times40\mu\textrm{m}$ square shape single grain PZT array could be obtained utilizing the difference of incubation time for nucleation of rosettes between ion damaged Pt and (111) oriented Pt electrode. Single grained PZT thin films show low leakage current density of $1\times10^{-7}$ A/$\textrm{cm}^2$ and high break down field of 440kV/cm. The loss of remanent polarization after $10^{11}$ cycles was less than 15% of initial value.

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