• 제목/요약/키워드: SiC-C films

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Ferroelectric Properties of PZT Thin Films by RF-Magnetron sputtering (RF 마그네트론 스퍼터링 법을 이용한 PZT 박막의 강유전 특성)

  • Park, Young;Joo, Pil-Yeoun;Yi, Ju-Sin;Song, Jun-Tae
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 한국전기전자재료학회 1999년도 춘계학술대회 논문집
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    • pp.341-344
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    • 1999
  • The effects of post annealing treatments of ferroelectrlclty in PZT(P $b_{1.05}$(Z $r_{0.52}$, $Ti_{0.48}$) $O_3$ thin film deposited on Pt/ $SiO_2$/Si substrate by RF-Magnetron sputtering methode was Investigated. Analyses by RTA(Rapid Thermal Annealing) treatments reveled that the crystallization process strongly depend on the healing temperature. The Perovskite structure with strong PZT (101) plan was obtained by RTA treatments at 75$0^{\circ}C$ With increasing RTA temperature of PZI thin films, the coercive field and remanent Polarization decreased, while saturation polarization( $P_{r}$) was decreased. P-E curves of Pt/PZT/Pt capacitor structures demonstrate typical hysteresiss loops. The measure values of $P_{r}$,. $E_{c}$ and dielectric constants by post annealed at 75$0^{\circ}C$ were 38 $\mu$C/$\textrm{cm}^2$ 35KV/cm and 974, respectively. Switching polarization versus fatigue characteristic showed 12% degradation up to 10$^{7}$ cycles.s.s.s.s.s.s.

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Ferroelectric properties of $Pb[(Zr,Sn)Ti]NbO_3$ Thin Films by Annealing (열처리에 따른 $Pb[(Zr,Sn)Ti]NbO_3$ 박막의 강유전 특성)

  • 최우창;최혁환;이명교;권태하
    • Proceedings of the IEEK Conference
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    • 대한전자공학회 2000년도 하계종합학술대회 논문집(2)
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    • pp.24-27
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    • 2000
  • Ferroelectric P $b_{0.99}$〔(Z $r_{0.6}$S $n_{0.4}$)$_{0.9}$ $Ti_{0.1}$$_{0.98}$N $b_{0.02}$ $O_3$(PNZST) thin films were deposited by a RF magnetron sputtering on (L $a_{0.5}$S $r_{0.5}$)Co $O_3$(LSCO)/Pt/Ti/ $SiO_2$/Si substrate using a PNZST target with excess PbO of 10 mole%. The thin films deposited at the substrate temperature of 500 $^{\circ}C$ were crystallized to a perovskite phase after rapid thermal annealing(RTA) The thin films annealed at 650 $^{\circ}C$ for 10 seconds in air exhibited the good crystal structures and ferroelectric properties. The remanent polarization and coercive field of the PNZST capacitor were about 20 $\mu$C/$\textrm{cm}^2$ and 50 kV/cm, respectively. The reduction of the polarization after 2.2$\times$10$^{9}$ switching cycles was less than 10 %.0 %.%.0 %.0 %.

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Preparation and structural properties of the Pb(Zr, Ti)${O}_{3}$ thin film by Sol-Gel method (Sol-Gel 법에 의한 Pb(Zr, Ti)${O}_{3}$ 박막의 제조 및 구조적 특성)

  • 이영준;정장호;이성갑;이영희
    • The Transactions of the Korean Institute of Electrical Engineers
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    • 제44권7호
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    • pp.914-918
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    • 1995
  • In this study, Pb(Zr$_{x}$ Ti$_{1-x}$ )O$_{3}$ (x=0.65, 0.52, 0.35) thin films were fabricated by Sol-Gel method. A stock solution with excess Pb 10[mol%] of Pb(Zr$_{x}$ Ti$_{1-x}$ )O$_{3}$ was made and spin-coated on the Pt/SiO$_{2}$/Si substrate at 4000[rpm] for 30[sec.]. Coated specimens were dried on the hot-plate at 400[.deg. C] for 10[min.]. Sintering temperature and time were 500~800[.deg. C] and 1~60[min.]. The coating process was repeated 6 times and the final thickness of the thin films were about 4800[A]. To investigate crystallization condition, PZT thin films were analyzed with sintering temperature, time and composition by the XRD. The microstructure of thin fulms were investigated by SEM. The ferroelectric perovskite phases precipitated under the sintering of 700[.deg. C] for 1 hours. In the PZT(52/48) composition, dielectric constant and dielectric loss were 2133, 2.2[%] at room temperature, respectively.ively.

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Preparing and Ferroelectric Properties of the Pb($Zr_{0.52}$$Ti_{0.48}$)$O_3$ Thin Film by Sol-Gel Method. (Sol-Gel법에 의한 Pb($Zr_{0.52}$$Ti_{0.48}$)$O_3$박막의 제조 및 강유전 특성)

  • 이영준;정장호;이성갑;이영희
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 한국전기전자재료학회 1994년도 추계학술대회 논문집
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    • pp.168-170
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    • 1994
  • Pb($Zr_{0.52}$$Ti_{0.48}$)$O_3$ ceramic thin films were fabricated from an alkoxide-based solution by Sol-Gel method. Pb($Zr_{0.52}$$Ti_{0.48}$)$O_3$ ceramic thin films were formed by spin coating method on Pt/$SiO_2$Si substrate at 4000ppm for 30 seconds. The coating process was repeated 6 times and then heat-treated at temperature between 500∼800[$^{\circ}C$] for 1 hour. The final thickness of the thin films were about 4800[A]. The ferroelectric perovskite phases precipitated under the heat-treated at 700[$^{\circ}C$] for 1 hour. Pb($Zr_{0.52}$$Ti_{0.48}$)$O_3$ thin films heat-treated at 700[$^{\circ}C$] for 1 hour showed good dielectric and ferroclectric properties.

Electrical and Optical Characteristics of ZnO:Al Films Prepared by rf Magnetron Sputtering for Thin Film Solar Cells Application (rf 마그네트론 스파터법에 의해 제조된 태양전지용 ZnO:Al 박막의 전기 광학적 특성)

  • Jeon, Sang-Won;Lee, Jeong-Chul;Park, Byung-Ok;Song, Jin-Soo;Yoon, Kyung-Hoon
    • Korean Journal of Materials Research
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    • 제16권1호
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    • pp.19-24
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    • 2006
  • ZnO:Al(AZO) films prepared by rf magnetron sputtering on glass substrate and textured by post-deposition chemical etching were applied as front contact and back reflectors for ${\mu}c$-Si:H thin film solar cells. For the front transparent electrode contact, AZO films were prepared at various working pressures and substrate temperature and then were chemically etched in diluted HCl(1%). The front AZO films deposited at low working pressure(1 mTorr) and low temperature ($240^{\circ}C$) exhibited uniform and high transmittance ($\geq$80%) and excellent electrical properties. The solar cells were optimized in terms of optical and electrical properties to demonstrate a high short-circuit current.

Dielectric Properties of the $Pb(Zr_{0.52}Ti_{0.48})O_3$ Thin Film by Sol-Gel Method. (Sol-Gel 법으로 제조한 $Pb(Zr_{0.52}Ti_{0.48})O_3$ 박막의 유전 특성)

  • Chung, Jang-Ho;Lee, Young-Jun;Lee, Sung-Gap;Lee, Young-Hie
    • Proceedings of the KIEE Conference
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    • 대한전기학회 1994년도 하계학술대회 논문집 C
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    • pp.1454-1456
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    • 1994
  • $Pb(Zr_{0.52}Ti_{0.48})O_3$ ceramic thin films were fabricated from an alkoxide-based solution by Sol-Gel method. $Pb(Zr_{0.52}Ti_{0.48})O_3$ ceramic thin films were formed by spin coating method on $Pt/SiO_2/Si$ substrate at 3000rpm for 30 seconds. The coating process was repeated 6 times and then heat-treated at temperature between 500 - $800[^{\circ}C]$ for 1 hour. The final thickness of the thin films were about 4800[A]. The 100% ferroelectric perovskite phases precipitated under the heat treated at $700[^{\circ}C]$ for 1 hour. $Pb(Zr_{0.52}Ti_{0.48})O_3$ thin films heat-treated at $700[^{\circ}C]$ for 1 hour showed good dielectric constant (812) property.

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Structural and Dielectric Properties of PZT(20/80)/PZT(80/20) Heterolayered Thin Films Prepared by Sol-Gel Method. (Sol-Gel법으로 제작한 PZT(20/80)/PZT(80/20) 이종층 박막의 구조 및 유전특성)

  • Shim, Kwang-Taek;Chung, Jang-Ho;Lee, Young-Hie;Park, In-Gil;Lee, Sung-Gap
    • Proceedings of the KIEE Conference
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    • 대한전기학회 1996년도 추계학술대회 논문집 학회본부
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    • pp.245-247
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    • 1996
  • The ferroelectric $Pb(Zr_xTi_{1-x})O_3$ (20/80, 80/20) heterolayered thin films were fabricated from an alkoxide-based by Sol-Gel method. The PZT(20/80) and PZT(80/20) stock solution were made and spin-coated on the Pt/Ti/$SiO_2$/Si substrate by turns. Each layers were baked to remove the organic materials at 300[$^{\circ}C$] for 30[min]. and sintered at 650[$^{\circ}C$] for 1[hr]. This procedure was repeated 5 times. At this time the thickness of thin films were about 4000[$\AA$]. Relative dielectric constant and remanent polarization of the PZT heterolayered thin films were 1200, 27.10 [${\mu}C/cm^2$], respectively.

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Characteristics of Silicon Oxide Thin Films Prepared by Atomic Layer Deposition Using Alternating Exposures of SiH2Cl2 and O3 (SiH2Cl2 와 O3을 이용한 원자층 증착법에 의해 제조된 실리콘 산화막의 특성)

  • Lee Won-Jun;Lee Joo-Hyeon;Han Chang-Hee;Kim Un-Jung;Lee Youn-Seung;Rha Sa-Kyun
    • Korean Journal of Materials Research
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    • 제14권2호
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    • pp.90-93
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    • 2004
  • Silicon dioxide thin films were deposited on p-type Si (100) substrates by atomic layer deposition (ALD) method using alternating exposures of $SiH_2$$Cl_2$ and $O_3$ at $300^{\circ}C$. $O_3$ was generated by corona discharge inside the delivery line of $O_2$. The oxide film was deposited mainly from $O_3$ not from $O_2$, because the deposited film was not observed without corona discharge under the same process conditions. The growth rate of the deposited films increased linearly with increasing the exposures of $SiH_2$$Cl_2$ and $O_3$ simultaneously, and was saturated at approximately 0.35 nm/cycle with the reactant exposures over $3.6 ${\times}$ 10^{9}$ /L. At a fixed $SiH_2$$Cl_2$ exposure of $1.2 ${\times}$ 10^{9}$L, growth rate increased with $O_3$ exposure and was saturated at approximately 0.28 nm/cycle with $O_3$ exposures over$ 2.4 ${\times}$ 10^{9}$ L. The composition of the deposited film also varied with the exposure of $O_3$. The [O]/[Si] ratio gradually increased up to 2 with increasing the exposure of $O_3$. Finally, the characteristics of ALD films were compared with those of the silicon oxide films deposited by conventional chemical vapor deposition (CVD) methods. The silicon oxide film prepared by ALD at $300^{\circ}C$ showed better stoichiometry and wet etch rate than those of the silicon oxide films deposited by low-pressure CVD (LPCVD) and atmospheric-pressure CVD (APCVD) at the deposition temperatures ranging from 400 to $800^{\circ}C$.

Properties of Yttrium Manganates with MFS Structure Fabricated on Various Substates (MFS 구조로 적층된 Yttrium Manganates의 기판 변화에 따른 특성 연구)

  • 강승구
    • Journal of the Korean Ceramic Society
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    • 제40권2호
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    • pp.206-211
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    • 2003
  • Effects of substrates and buffer layer upon the formation of crystalline phases and ferroelectricity of $YMnO_3$ thin films were investigated. The hexagonal $YMnO_3$ was easily formed on Si(100) while the mixed phases, hexagonal and orthorhombic $YMnO_3$, on $Pt(111)/TiO_2/SiO_2/Si$ substrate. When the $Y_2O_3$ buffer layer of 70 nm thick was inserted between the substrates and the $YMnO_3,$ the c-axis oriented hexagonal single phase formed on both substrates, Si(100) and $Pt(111)/TiO_2/SiO_2/Si$. The leakage current density of the hexagonal $YMnO_3$ thin films was lower than that consisting of mixed phases, hexagonal and orthorhombic. Furthermore the hexagonal $YMnO_3$ with c-axis preferred orientation showed the lowest leakage current density. The remnant polarization from a P-E hysteresis curve for the $YMnO_3$ formed on Si(100) was 0.14 without buffer layer and $0.24_{mu}C/cm^2$ for that with buffer layer. For the $Pt(111)/TiO_3/SiO_3/Si$ substrates, the specimen without $Y_2O_3$buffer layer did not show the hysteresis curve, while the buffer-layered has the remnant polarization of $1.14_{mu}C/cm^2$. It was concluded that the leakage current density and the ferroelectricity for the $YMnO_3$ thin films could be controlled by varying crystalline phases and their preferred orientation which depend on the kind of substrates and whether the $Y_2O_3$buffer layer exist or not.

Effect of Plating Conditions on Electroless Copper Plating on SiC Fabric (직조된 SiC 섬유에 무전해 구리도금 시 도금 조건의 영향)

  • Lee, Kee Hwan;Sohn, Youhan;Han, Taeyang;Lee, Kyung Jin;Kim, Hye Hung;Han, Jun Hyun
    • Journal of Surface Science and Engineering
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    • 제50권4호
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    • pp.244-250
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    • 2017
  • Effects of plating conditions (dispersant concentration, plating time, and ultrasonication) on electroless Cu plating on SiC fabric woven by crossing of SiC continuous fibers vertically were studied. The ultrasonic dispersion treatment not only did not improve the dispersion of the SiC fibers, but also did not change the plating thickness. The ultrasonication in the pretreatment step of electroless plating did not improve the dispersion of the fibers, while the ultrasonication in the plating step enhanced the dispersion of the fibers and decreased the thickness of the Cu films. It was possible to control the thickness of the Cu coating layer as well as the dispersion of the fibers in the fabric by changing the plating conditions such as dispersant concentration, plating time, and ultrasonication, but it was very difficult to coat copper on the intersection of vertical fibers in the fabric.