• 제목/요약/키워드: doping material

검색결과 787건 처리시간 0.029초

나노와이어 junctionless 트랜지스터의 문턱전압 및 평탄전압 모델링과 소자설계 가이드라인 (Threshold and Flat Band Voltage Modeling and Device design Guideline in Nanowire Junctionless Transistors)

  • 김진영;유종근;박종태
    • 대한전자공학회논문지SD
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    • 제48권12호
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    • pp.1-7
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    • 2011
  • 본 연구에서는 나노와이어 junctionless 트랜지스터의 문턱전압과 평탄전압을 위한 해석학적 모델링을 제시하였고 3차원 소자 시뮬레이션으로 검증하였다. 그리고 junctionless 트랜지스터의 소자설계 가이드라인을 설정하는 방법과 그 예를 제시하였다. 제시한 문턱전압과 평탄전압 모델은 3차원 시뮬레이션 결과와 잘 일치하였다. 나노와이어 반경과 게이트 산화층 두께가 클수록 또 채널 불순물 농도가 높을수록 문턱전압과 평탄전압은 감소하였다. 게이트 일함수와 원하는 구동전류/누설전류 비가 주어지면 나노와이어 반경, 게이트 산화층 두께, 채널 불순물 농도에 따른 junctionless 트랜지스터의 소자설계 가이드라인을 설정하였다. 나노와이어 반경이 작을수록 산화층의 두께가 얇을수록 채널 불순물 농도가 큰 소자를 설계할 수 있음을 알 수 있었다.

Rutile Ti1-xCoxO2-δ p-type Diluted Magnetic Semiconductor Thin Films

  • Seong, Nak-Jin;Yoon, Soon-Gil;Cho, Young-Hoon;Jung, Myung-Hwa
    • Transactions on Electrical and Electronic Materials
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    • 제7권3호
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    • pp.149-153
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    • 2006
  • An attempting to produce a p-type diluted magnetic semiconductor (DMS) using $Ti_{1-x}Co_xO_{2-\delta}-based$ thin films was made by suitable control of the deposition parameters including deposition temperature, deposition pressure, and doping level using a pulsed laser deposition method. T$Ti_{0.97}Co_{0.03}O_{2-\delta}-based$ (TCO) films deposited at $500^{\circ}C$ at a pressure of $5\times10^{-6}$ Torr showed an anomalous Hall effect with p-type characteristics. On the other hand, films deposited at $700^{\circ}C$ at $5\times10^{-6}$ Torr showed n-type behaviors by a decreased solubility of cobalt. The charge carrier concentration in the p-type TCO films was approximately $7.9\times10^{22}/cm^3$ at 300 K and the anomalous Hall effect in the p-type TCO films was controlled by a side-jump scattering mechanism. The magnetoresistance (MR), measured at 5 K in p-type TCO films showed a positive behavior in an applied magnetic field and the MR ratio was approximately 3.5 %. The successful preparation of p-type DMS using the TCO films has the potential for use in magnetic tunneling junction devices.

Electrical and Optical Study of PLED & OLEDS Structures

  • Mohammed, BOUANATI Sidi;SARI, N. E. CHABANE;Selma, MOSTEFA KARA
    • Transactions on Electrical and Electronic Materials
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    • 제16권3호
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    • pp.124-129
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    • 2015
  • Organic electronics are the domain in which the components and circuits are made of organic materials. This new electronics help to realize electronic and optoelectronic devices on flexible substrates. In recent years, organic materials have replaced conventional semiconductors in many electronic components such as, organic light-emitting diodes (OLEDs), organic field-effect transistors (OFETs) and organic photovoltaic (OPVs). It is well known that organic light emitting diodes (OLEDs) have many advantages in comparison with inorganic light-emitting diodes LEDs. These advantages include the low price of manufacturing, large area of electroluminescent display, uniform emission and lower the requirement for power. The aim of this paper is to model polymer LEDs and OLEDs made with small molecules for studying the electrical and optical characteristics. The purpose of this modeling process is, to obtain information about the running of OLEDs, as well as, the injection and charge transport mechanisms. The first simulation structure used in this paper is a mono layer device; typically consisting of the poly (2-methoxy-5(2'-ethyl) hexoxy-phenylenevinylene) (MEH-PPV) polymer sandwiched between an anode with a high work function, usually an indium tin oxide (ITO) substrate, and a cathode with a relatively low work function, such as Al. Electrons will then be injected from the cathode and recombine with electron holes injected from the anode, emitting light. In the second structure, we replaced MEH-PPV by tris (8-hydroxyquinolinato) aluminum (Alq3). This simulation uses, the Poole-Frenkel -like mobility model and the Langevin bimolecular recombination model as the transport and recombination mechanism. These models are enabled in ATLAS- SILVACO. To optimize OLED performance, we propose to change some parameters in this device, such as doping concentration, thickness and electrode materials.

Energy Band Structure and Photocatalytic Property of Fe-doped Zn2TiO4 Material

  • Jang, Jum-Suk;Borse, Pramod H.;Lee, Jae-Sung;Lim, Kwon-Taek;Jung, Ok-Sang;Jeong, Euh-Duck;Bae, Jong-Seong;Won, Mi-Sook;Kim, Hyun-Gyu
    • Bulletin of the Korean Chemical Society
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    • 제30권12호
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    • pp.3021-3024
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    • 2009
  • $Zn_2Ti_{1-x}Fe_xO_4\;(0\;{\leq}\;x\;{\leq}\;0.7)$ photocatalysts were synthesized by polymerized complex (PC) method and investigated for its physico-chemical as well as optical properties. $Zn_2Ti_{1-x}Fe_xO_4$ can absorb not only UV light but also visible light region due to doping of Fe in the Ti site of $Zn_2TiO_4$ lattice because of the band transition from Fe 3d to the Fe 3d + Ti3d hybrid orbital. The photocatalytic activity of Fe doped $Zn_2TiO_4$ samples for hydrogen production under UV light irradiation decreased with an increase in Fe concentration in $Zn_2TiO_4$. Consequently, there exists an optimized concentration of iron for improved photocatalytic activity under visible light (${\lambda}{\leq}$420 nm)

Synthesis of Amorphous Er3+-Yb3+ Co-doped TiO2 and Its Application as a Scattering Layer for Dye-sensitized Solar Cells

  • Han, Chi-Hwan;Lee, Hak-Soo;Lee, Kyung-Won;Han, Sang-Do;Singh, Ishwar
    • Bulletin of the Korean Chemical Society
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    • 제30권1호
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    • pp.219-223
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    • 2009
  • $TiO_2$ doped with $Er^{3+\;and\;Yb^{3+}$ was used for fabricating a scattering layer and a nano-crystalline $TiO_2$ electrode layer to be used in dye-sensitized solar cells. The material was prepared using a new sol-gel combustion hybrid method with acetylene black as fuel. The $Er^{3+}$-$Yb^{3+}$ co-doped titanium oxide powder synthesized at 700oC had embossed structure morphology with a size between 27 to 54 nm that agglomerated to produce micron size particles, as observed by the scanning electron micrographs. The XRD patterns showed that the $Er^{3+}$-$Yb^{3+}$ co-doped titanium oxide had an amorphous structure, while using the same method without doping $Er^{3+}\;or\;Yb^{3+},\;TiO_2$ was obtained in the crystallite form with thea dominance of rutile phase. Fabricating a bilayer structure consisting of nano-crystalline $TiO_2$ and the synthesized $Er^{3+}$-$Yb^{3+}$ co-doped titanium oxide showed better scattering property, with an overall increase of 15.6% in efficiency of the solar cell with respect to a single nano-crystalline $TiO_2$ layer.

무연 BNBT 세라믹스의 압전특성에 미치는 La2O3의 영향 (Effects of La2O3 on the Piezoelectric Properties of Lead-Free (Bi0.5Na0.5)0.94Ba0.06TiO3 Piezoelectric Ceramics)

  • 손영진;윤만순;어순철
    • 한국재료학회지
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    • 제15권12호
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    • pp.756-759
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    • 2005
  • A lead free piezoelectric material, bismuth sodium barium titanate $(Bi_{0.5}Na_{0.5})_{0.94}Ba_{0.06}TiO_3$ (BNBT), was considered as an environment-friendly alternatives for the current PZT system. A perovskite BNBT was synthesized by conventional bulk ceramic processing technique. In order to improve piezoelectric properties, $La_2O_3$ as a dopant was incorporated into the BNBT system up to 0.025 moi, ana the effects on subsequent the piezoelectric ana dielectric properties were systematically investigated. With increasing $La_2O_3$ contents, the equilibrium grain shape was remarkably evidenced and sintered density was increased. Piezoelectric and dielectric properties were s]town to have maximum values at the $La_2O_3$ contents of 0.02 mol. $La^{3+}$ ions seemed to act as a softener in the BNBT system and to enhance dielectric and piezoelectric properties in this study.

Efficient White Organic Light-emitting Device by utilizing a Blue-emitter Doped with a Red Fluorescent Dopant

  • Lim, Jong-Tae;Ahn, Young-Joo;Kang, Gi-Wook;Lee, Nam-Heon;Lee, Mun-Jae;Kang, Hee-Young;Lee, Chang-Hee;Ko, Young-Wook;Lee, Jin-Ho
    • Journal of Information Display
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    • 제4권2호
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    • pp.13-18
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    • 2003
  • We synthesized bis (2-methyl-8-quinolinolato)(triphenylsiloxy) aluminum (III) (SAlq), a blue-emitting material having a high luminous efficiency, through a homogeneous-phase reaction. The photoluminescence (PL) and electroluminescence (EL) spectra of SAlq show two peaks at 454 nm and 477 nm. Efficient white light-emitting devices are fabricated by doping SAlq with a red fluorescent dye of 4-dicyanomethylene-2-methyl-6-{2-(2,3,6,7-tetrahydro-1H,5H-benzo[i,j]quinolizin-8yl) vinyl}-4H-pyran (DCM2). The incomplete energy transfer from blue-emitting SAlq to red-emitting DCM2 results in light-emission of both blue and orange colors. Devices with the structure of ITO/TPD (50 nm)/SAlq:DCM2 (30 nm, 0.5 %)/$Alq_3$ (20 nm)/LiF (0.5 nmj/Al show EL peaks at 456 nm and 482 nm originating from SAlq and at 570 nm from DCM2, resulting in the Commission Internationale d'Eclairage (CIE) chromaticity coordinates of (0.32, 0.37). The device exhibits an external quantum efficiency of about 2.3 % and a luminous efficiency of about 2.41m/W at 100 $cd/m^2$. A maximum luminance of about 23,800 $cd/m^2$ is obtained at the bias voltage of 15 V.

Implant Anneal Process for Activating Ion Implanted Regions in SiC Epitaxial Layers

  • Saddow, S.E.;Kumer, V.;Isaacs-Smith, T.;Williams, J.;Hsieh, A.J.;Graves, M.;Wolan, J.T.
    • Transactions on Electrical and Electronic Materials
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    • 제1권4호
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    • pp.1-6
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    • 2000
  • The mechanical strength of silicon carbide dose nor permit the use of diffusion as a means to achieve selective doping as required by most electronic devices. While epitaxial layers may be doped during growth, ion implantation is needed to define such regions as drain and source wells, junction isolation regions, and so on. Ion activation without an annealing cap results in serious crystal damage as these activation processes must be carried out at temperatures on the order of 1600$^{\circ}C$. Ion implanted silicon carbide that is annealed in either a vacuum or argon environment usually results in a surface morphology that is highly irregular due to the out diffusion of Si atoms. We have developed and report a successful process of using silicon overpressure, provided by silane in a CAD reactor during the anneal, to prevent the destruction of the silicon carbide surface, This process has proved to be robust and has resulted in ion activation at a annealing temperature of 1600$^{\circ}C$ without degradation of the crystal surface as determined by AFM and RBS. In addition XPS was used to look at the surface and near surface chemical states for annealing temperatures of up to 1700$^{\circ}C$. The surface and near surface regions to approximately 6 nm in depth was observed to contain no free silicon or other impurities thus indicating that the process developed results in an atomically clean SiC surface and near surface region within the detection limits of the instrument(${\pm}$1 at %).

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Cu(In,Ga)Se2 박막의 저온 성장 및 NaF 후속처리를 통한 태양전지 셀 특성 연구 (Low-temperature Growth of Cu(In,Ga)Se2 Thin Film and NaF Post Deposition Treatment for Cu(In,Ga)Se2 Solar Cells)

  • 김승태;정광선;윤재호;박병국;안병태
    • Current Photovoltaic Research
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    • 제3권1호
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    • pp.21-26
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    • 2015
  • High efficiency $Cu(In,Ga)Se_2$ solar cells are generally prepared above $500^{\circ}C$. Lowering the process temperature can allow wider selection of substrate material and process window. In this paper, the three-stage co-evaporation process widely used to grow CIGS thin film at high temperature was modified to reduce the maximum substrate temperature. Below $400^{\circ}C$ the CIGS films show poor crystal growth and lower solar cell performance, in spite of external Na doping by NaF. As a new approach, Cu source instead of Cu with Se in the second stage was applied on the $(In,Ga)_2Se_3$ precursor at $400^{\circ}C$ and achieved a better crystal growth. The distribution of Ga in the films produce by new method were investigated and solar cells were fabricated using these films.

High Performance ESD/Surge Protection Capability of Bidirectional Flip Chip Transient Voltage Suppression Diodes

  • Pharkphoumy, Sakhone;Khurelbaatar, Zagarzusem;Janardhanam, Valliedu;Choi, Chel-Jong;Shim, Kyu-Hwan;Daoheung, Daoheung;Bouangeun, Bouangeun;Choi, Sang-Sik;Cho, Deok-Ho
    • Transactions on Electrical and Electronic Materials
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    • 제17권4호
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    • pp.196-200
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    • 2016
  • We have developed new electrostatic discharge (ESD) protection devices with, bidirectional flip chip transient voltage suppression. The devices differ in their epitaxial (epi) layers, which were grown by reduced pressure chemical vapor deposition (RPCVD). Their ESD properties were characterized using current-voltage (I-V), capacitance-voltage (C-V) measurement, and ESD analysis, including IEC61000-4-2, surge, and transmission line pulse (TLP) methods. Two BD-FCTVS diodes consisting of either a thick (12 μm) or thin (6 μm), n-Si epi layer showed the same reverse voltage of 8 V, very small reverse current level, and symmetric I-V and C-V curves. The damage found near the corner of the metal pads indicates that the size and shape of the radius governs their failure modes. The BD-FCTVS device made with a thin n- epi layer showed better performance than that made with a thick one in terms of enhancement of the features of ESD robustness, reliability, and protection capability. Therefore, this works confirms that the optimization of device parameters in conjunction with the doping concentration and thickness of epi layers be used to achieve high performance ESD properties.