• Title/Summary/Keyword: Buffer layer

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Epitaxial Growth of BSCCO Thin film Fabricated by Layer-by-layer Sputtering

  • Yang, Sung-Ho;Park, Yong-Pil;Lee, Hee-Kab
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2000.07a
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    • pp.212-217
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    • 2000
  • Bi$_2$Sr$_2$CuO$_{x}$(Bi-2201) thin films have been fabricated by atomic layer-by-layer deposition using ion beam sputtering(IBS) process. During the deposition, 14 wt%-ozone/oxygen mixture gas of typical pressure of 5.0$\times$10$^{-5}$ Torr is supplied with ultraviolet light irradiation for oxidation. XRD and RHEED investigations reveal that a buffer layer with compositions different from Bi-2201 is formed at the early deposition stage of less than 10 units cell and then Bi-2201 oriented along the c-axis is grown.n.

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Efficiency Enhancement of Organic Light Emitting Diode Using $TiO_2$ Buffer Layer

  • Lee, Heui-Dong;Oh, Min-Cheol;Kim, Jae-Chang;Yoon, Tae-Hoon
    • 한국정보디스플레이학회:학술대회논문집
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    • 2004.08a
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    • pp.632-635
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    • 2004
  • We have studied the effect of $TiO_2$ layer deposited by RF magnetron sputtering which is used as an ultra thin hole-injection buffer layer in organic light-emitting diode (OLED). The $TiO_2$ thin film layer prevents metallic ions from diffusing from the ITO layer to the organic layers and improves the balance of hole and electron injections and the interface characteristics between the electrode and the organic layer. With 2 nm thickness of $TiO_2$, the quantum efficiency was improved by 45 % compared to the device fabricated without the $TiO_2$ layer.

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Epitaxial Growth of BSCCO Films by Leyer-by-Layer Deposition (순차 증착에 의한 BSCCO 박막의 에피택셜 성장)

  • 안준호;박용필;김정호
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.14 no.10
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    • pp.855-860
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    • 2001
  • Bi$_2$Sr$_2$CuO$_{x}$(Bi-2201) thin film were fabricated by atomic layer-by -layer deposition using an ion beam sputtering method. 10 wt% and 90 wt% ozone mixed oxygen were used with ultraviolet light irradiation to assist oxidation. XRD and RHEED investigations revealed that a buffer layer is formed at the early stage of deposition (less than 10 unit cell), and then c-axis oriented Bi-2201 grows on top of it.t.

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Properties of CoCrTa Thin Film Introduce Two Step methode and Amorphous Si Under Layer for Perpendicular Magnetic Recording Media (Two Step방식과 아몰퍼스 Si 하지층 도입에 따른 수직자기기록 매체용 CoCrTa 박막의 특성 평가)

  • Park, Won-Hyo;Kim, Kyung-Hwan
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2003.07a
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    • pp.550-552
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    • 2003
  • We prepared $Co_{77}Cr_{20}Ta_3$ Magnetic layer for perpendicular magnetic recording media with introduce Two-step methode and Amorphous Si Underlayer on slide glass substrate. The thickness of magnetic layer were 100nm, and Underlayer were varied from 5 to 100 nm. The multi layer Properties of crystal structure were examined with XRD. Prepared thin films showed improvement of dispersion angle of c-axis orientation ${\Delta}{\theta}_{50}$ caused by inserting Buffer-layer and amorphous Si underlayer.

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In-situ monitoring technique for deposition process of CdS buffer layer for CIGS thin film solar cells (CIGS 박막 태양전지용 CdS 버퍼층 제조 공정의 in-situ 모니터링 기술)

  • Kown, Young-Jun;Ahn, Se-Jin;Yoon, Jae-Ho;Yoon, Kyung-Hoon
    • 한국신재생에너지학회:학술대회논문집
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    • 2008.05a
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    • pp.434-435
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    • 2008
  • An in-situ monitoring technique for deposition process of CdS buffer layer was developed in this work. A quartz crystal microbalance (QCM) was used to measure the frequency change during the CdS deposition process and the relation ship between frequency change and film thickness and optical transmittance was investigated. The film thickness shows a linear relationship with frequency change, demonstrating that frequency change measured by QCM can be used a in-situ monitoring tool for CdS deposition process.

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Opto-electrical properties for a HgCdTe epilayers grown by hot wall epitaxy (Hot wall epitaxy에 의해 성장된 HgCdTe 에피레이어의 광전기적특성)

  • 홍광준
    • Proceedings of the Materials Research Society of Korea Conference
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    • 2003.11a
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    • pp.152-152
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    • 2003
  • Hg$\sub$l-x/Cd$\sub$x/Te (MCT) was grown by hot wall epitaxy. Prior to the MCT growth, the CdTe (111) buffer layer was grown on the GaAs substrate at the temperature of 590$^{\circ}C$ for 15 min. When the thickness of the CdTe buffer layer was 5 $\mu\textrm{m}$ or thicker, the full width at half maximum values obtained from the x-ray rocking curves were found to significantly decrease. After a good quality CdTe buffer layer was grown, the MCT epilayers were grown on the CdTe (111) /GaAs substrate at various temperatures in situ. The crystal quality for those epilayers was investigated by means of the x-ray rocking curves and the photocurrent experiment The photoconductor characterization for the epilayers was also measured The energy band gap of MCT was determined from the photocurrent measurement and the x composition rates from the temperature dependence of the energy band gap were turned out

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A Study on the Characteristic of PZT Thin Film Deposited on New Buffer Layer by Sputtering (스퍼터링으로 제조한 새로운 완충막 위의 PZT 박막 특성에 관한 연구)

  • 주재현;주승기
    • Journal of the Korean Ceramic Society
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    • v.30 no.4
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    • pp.332-338
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    • 1993
  • TiN/Ti is the best buffer layer between PZT thin film and si substrate among the Ti, TiN, ZrN, TiN/Ti, ZrN/Ti. The amorphous PZT films deposited on TiN/Ti buffer layer directly transform into perovskite phase when rapid thermal annealed for 30sec above 55$0^{\circ}C$. As Rapid Thermal Annealing(RTA) temperature increased, the remanent polarization(Pr) and dielectric constant($\varepsilon$r) increased and then showed Pr=21 $\varepsilon$r=593 when rapid thermal annealed 80$0^{\circ}C$ for 30sec. On the contrary the leakage current increased with increasing RTA temperature due to the formation of void made by Pb evaporationand grain cohesion.

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Modeling of Anode Voltage Drop for PT-IGBT at Turn-off (턴-오프 시 PT-IGBT의 애노드 전압 강하 모델링)

  • Ryu, Se-Hwan;Lee, Ho-Kil;Ahn, Hyung-Keun;Han, Deuk-Young
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.21 no.1
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    • pp.23-28
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    • 2008
  • In this paper, transient characteristics of the Punch Through Insulated Gate Bipolar Transistor (PT-IGBT) have been studied. On the contrary to Non-Punch Through Insulated Gate Bipolar Transistor(NPT-IGBT), it has a buffer layer and reduces switching power loss. It has a simple drive circuit controlled by the gate voltage of the MOSFET and low on-state resistance of the bipolar junction transistor. The transient characteristics of the PT-IGBT have been analyzed analytically. Excess minority carrier and charge distribution in active base region, the rate of anode voltage with time are expressed analytically by adding the influence of buffer layer. The experimental data is obtained from manufacturer. The theoretical predictions of the analysis have been compared with the experimental data obtained from the measurement of a device(600 V, 15 A) and show good agreement.

Binding energy study from photocurrent signal in HgCdTe layers

  • Hong, Kwang-Joon
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2010.06a
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    • pp.379-379
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    • 2010
  • $Hg_{1_x}Cd_xTe$ (MCT) was grown by hot wall epitaxy. Prior to the MCT growth, the CdTe (111) buffer layer was grown on the GaAs substrate at the temperature of $590^{\circ}C$ for 15 min. When the thickness of the CdTe buffer layer was $5\;{\mu}m$ or thicker, the full width at half maximum values obtained from the x-ray rocking curves were found to significantly decrease. After a good quality CdTe buffer layer was grown, the MCT epilayers were grown on the CdTe (111) /GaAs substrate at various temperatures in situ. The crystal quality for those epilayers was investigated by means of the x-ray rocking curves and the photocurrent experiment. The photoconductor characterization for the epilayers was also measured. The energy band gap of MCT was determined from the photocurrent measurement and the x composition rates from the temperature dependence of the energy band gap were turned out.

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Effect of plasma polythiophene as a buffer layer inserted on OLEDs (버퍼층으로서 플라즈마 polythiopheneol 유기EL소자에 미치는 영향)

  • Park, S.M.;Lee, B.J.;Kim, H.G.;Lim, K.B.;Kim, J.T.;Park, S.H.;Lim, E.C.;Lee, E.H.;Lee, D.C.
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2002.05c
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    • pp.177-180
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    • 2002
  • The purpose of this thesis is to develope buffer materials by the plasma polymerization method. In this article the buffer materials, plasma poly thiophene(PPTh) is used to study the interface of eter/organic in organic light emitting diodes(OLED). The interface of meter/organic materials is the important and critical objectives in development of OLED. The hole transport layer was N,N'-dipheneyl-N, N'bis-(3-methypheneyl)-1,1'dipheneyl-4,4'-diamine (TPD); the host material of mission layer was 8-tris-hydroxyquinoline aluminium (Alq3). When PPTh was inserted between ITO and TPD, emission efficiency increased.

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