• 제목/요약/키워드: Amorphous Oxide Semiconductor

검색결과 144건 처리시간 0.028초

Metal/Ferroelectric/Insulator/Semiconductor 구조의 결정 구조 및 전기적 특성에 관한 연구 (Characteristics of the Crystal Structure and Electrical Properties of Metal/Ferroelectric/Insulator/Semiconductor)

  • 신동석;최훈상;최인훈;이호녕;김용태
    • 한국진공학회지
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    • 제7권3호
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    • pp.195-200
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    • 1998
  • 본 연구에서는 강유전체 박막의 게이트 산화물로 사용한 $Pt/SrBi_2Ta_2O_9(SBT)/CeO_2/Si(MFS)$와 Pt/SBT/Si(MFS) 구조의 결정 구조 및 전기적 성질 의 차이를 연구하였다. XRD 및 SEM 측정 결과 SBT/$CeO_2$/Si박막은 약5nm정도의 $SiO_2$층 이 형성되었고 비교적 평탄한 계면의 미세구조를 가지는 반면, SBT/Si는 각각 약6nm와 7nm정도의 $SiO_2$층과 비정질 중간상층이 형성되었음을 알 수 있다. 즉 CeO2 박막을 완충층 으로 사용함으로써 SBT박막과 Si기판의 상호 반응을 적절히 억제할 수 있음을 확인하였다. Pt/SBT/$CeO_2/Pt/SiO_2$/와 Pt/SBT/Pt/$SiO_2$/Si구조에서 Polarization-Electric field(P-E) 특 성을 비교해 본 결과 CeO2박막의 첨가에 따라 잔류분극값은 감소하였고 항전계값은 증가하 였다. MFIS구조에서 memory window값은 항전계값과 직접적 관련이 있으므로 이러한 항 전계값의 증가는 MFIS구조에서의 memory window값이 증가할 수 있음을 나타낸다. Pt-SBT(140nm)/$CeO_2$(25nm)/Si구조에서 Capacitance-Voltage(C-V) 측정 결과로부터 동작 전압 4-6V에서 memory wondows가 1-2V정도로 나타났다. SBT박막의 두께가 증가할수록 memory window값은 증가하였는데 memory wondows가 1-2V정도로 나타났다. SBT박막의 두께가 증가할수록 memory window값은 증가하였는데 이는 SBT박막에 걸리는 전압강하가 증가하기 때문인 것으로 생각되어진다. Pt/SBT/$CeO_2$/Si의 누설전류는 10-8A/cm2정도였고 Pt/SBT/Si 구조에서는 약10-6A/cm2정도로 약간 높은 값을 나타내었다.

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원자층 증착을 이용한 친환경 소재의 제조 (Fabrication of Environmental-friendly Materials Using Atomic Layer Deposition)

  • 김영독
    • 공업화학
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    • 제23권1호
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    • pp.1-7
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    • 2012
  • 본 총론에서는 원자층 증착을 이용한 친환경 소재의 개발에 대한 최근 연구 결과들을 간단하게 소개하려 한다. 원자층 증착의 장점은 박막의 두께를 미세하게 조절할 수 있다는 것과, 3차원적으로 복잡한 구조를 가지는 담체의 형상을 유지하면서 균일한 박막을 제조할 수 있다는 것이다. 이러한 원자층 증착의 장점은 친환경소재를 제조하는 데 중요한 역할을 할 수 있다. Anodic aluminum oxide (AAO)와 같은 다공성 membrane을 담체로 이용하여, 다공성 구조는 그대로 유지하면서 10나노미터 정도의 $TiO_2$박막을 균일하게 증착할 경우 톨루엔 등의 휘발성 유기물 필터로 사용할 수 있는데, 이는 AAO의 특이한 기하학적 구조와 비정질 $TiO_2$의 강한 휘발성 유기물 흡착력의 조합에 의한 결과이다. 톨루엔 분해용 광촉매 및 이산화탄소 개질 반응에 의한 수소 생산 촉매 반응에 있어서도 나노다이아몬드나 니켈 담체 위에 $TiO_2$의 증착량을 미세하게 조절하여 $TiO_2$가 표면을 완전히 덮지 않고 부분적으로만 덮고 있는 구조를 만들 경우 촉매의 효율 및 수명을 극대화할 수 있게 된다. 이러한 예들은 원자층 증착이 기존의 반도체산업뿐만 아니라 환경소재의 개발에도 중요한 도구가 될 수 있음을 의미한다.

High Performance Flexible Inorganic Electronic Systems

  • 박귀일;이건재
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2012년도 제43회 하계 정기 학술대회 초록집
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    • pp.115-116
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    • 2012
  • The demand for flexible electronic systems such as wearable computers, E-paper, and flexible displays has increased due to their advantages of excellent portability, conformal contact with curved surfaces, light weight, and human friendly interfaces over present rigid electronic systems. This seminar introduces three recent progresses that can extend the application of high performance flexible inorganic electronics. The first part of this seminar will introduce a RRAM with a one transistor-one memristor (1T-1M) arrays on flexible substrates. Flexible memory is an essential part of electronics for data processing, storage, and radio frequency (RF) communication and thus a key element to realize such flexible electronic systems. Although several emerging memory technologies, including resistive switching memory, have been proposed, the cell-to-cell interference issue has to be overcome for flexible and high performance nonvolatile memory applications. The cell-to-cell interference between neighbouring memory cells occurs due to leakage current paths through adjacent low resistance state cells and induces not only unnecessary power consumption but also a misreading problem, a fatal obstacle in memory operation. To fabricate a fully functional flexible memory and prevent these unwanted effects, we integrated high performance flexible single crystal silicon transistors with an amorphous titanium oxide (a-TiO2) based memristor to control the logic state of memory. The $8{\times}8$ NOR type 1T-1M RRAM demonstrated the first random access memory operation on flexible substrates by controlling each memory unit cell independently. The second part of the seminar will discuss the flexible GaN LED on LCP substrates for implantable biosensor. Inorganic III-V light emitting diodes (LEDs) have superior characteristics, such as long-term stability, high efficiency, and strong brightness compared to conventional incandescent lamps and OLED. However, due to the brittle property of bulk inorganic semiconductor materials, III-V LED limits its applications in the field of high performance flexible electronics. This seminar introduces the first flexible and implantable GaN LED on plastic substrates that is transferred from bulk GaN on Si substrates. The superb properties of the flexible GaN thin film in terms of its wide band gap and high efficiency enable the dramatic extension of not only consumer electronic applications but also the biosensing scale. The flexible white LEDs are demonstrated for the feasibility of using a white light source for future flexible BLU devices. Finally a water-resist and a biocompatible PTFE-coated flexible LED biosensor can detect PSA at a detection limit of 1 ng/mL. These results show that the nitride-based flexible LED can be used as the future flexible display technology and a type of implantable LED biosensor for a therapy tool. The final part of this seminar will introduce a highly efficient and printable BaTiO3 thin film nanogenerator on plastic substrates. Energy harvesting technologies converting external biomechanical energy sources (such as heart beat, blood flow, muscle stretching and animal movements) into electrical energy is recently a highly demanding issue in the materials science community. Herein, we describe procedure suitable for generating and printing a lead-free microstructured BaTiO3 thin film nanogenerator on plastic substrates to overcome limitations appeared in conventional flexible ferroelectric devices. Flexible BaTiO3 thin film nanogenerator was fabricated and the piezoelectric properties and mechanically stability of ferroelectric devices were characterized. From the results, we demonstrate the highly efficient and stable performance of BaTiO3 thin film nanogenerator.

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In-situ Synchrotron Radiation Photoemission Spectroscopy Study of Property Variation of Ta2O5 Film during the Atomic Layer Deposition

  • Lee, Seung Youb;Jeon, Cheolho;Kim, Seok Hwan;Lee, Jouhahn;Yun, Hyung Joong;Park, Soo Jeong;An, Ki-Seok;Park, Chong-Yun
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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    • pp.362-362
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    • 2014
  • Atomic layer deposition (ALD) can be regarded as a special variation of the chemical vapor deposition method for reducing film thickness. ALD is based on sequential self-limiting reactions from the gas phase to produce thin films and over-layers in the nanometer scale with perfect conformality and process controllability. These characteristics make ALD an important film deposition technique for nanoelectronics. Tantalum pentoxide ($Ta_2O_5$) has a number of applications in optics and electronics due to its superior properties, such as thermal and chemical stability, high refractive index (>2.0), low absorption in near-UV to IR regions, and high-k. In particular, the dielectric constant of amorphous $Ta_2O_5$ is typically close to 25. Accordingly, $Ta_2O_5$ has been extensively studied in various electronics such as metal oxide semiconductor field-effect transistors (FET), organic FET, dynamic random access memories (RAM), resistance RAM, etc. In this experiment, the variations of chemical and interfacial state during the growth of $Ta_2O_5$ films on the Si substrate by ALD was investigated using in-situ synchrotron radiation photoemission spectroscopy. A newly synthesized liquid precursor $Ta(N^tBu)(dmamp)_2$ Me was used as the metal precursor, with Ar as a purging gas and $H_2O$ as the oxidant source. The core-level spectra of Si 2p, Ta 4f, and O 1s revealed that Ta suboxide and Si dioxide were formed at the initial stages of $Ta_2O_5$ growth. However, the Ta suboxide states almost disappeared as the ALD cycles progressed. Consequently, the $Ta^{5+}$ state, which corresponds with the stoichiometric $Ta_2O_5$, only appeared after 4.0 cycles. Additionally, tantalum silicide was not detected at the interfacial states between $Ta_2O_5$ and Si. The measured valence band offset value between $Ta_2O_5$ and the Si substrate was 3.08 eV after 2.5 cycles.

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