• Title/Summary/Keyword: $TaN_x$ film

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Electrical Properties of Metal-Ferroelectric-Insulator-Semiconductor Field-Effect Transistor Using an Au/$(Bi,La)_4Ti_3O_{12}/LaZrO_x$/Si Structure

  • Jeon, Ho-Seung;Lee, Gwang-Geun;Kim, Joo-Nam;Park, Byung-Eun;Choi, Yun-Soo
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2007.11a
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    • pp.171-172
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    • 2007
  • We fabricated the metal-ferroelectric-insulator-semiconductor filed-effect transistors (MFIS-FETs) using the $(Bi,La)_4Ti_3O_{12}\;and\;LaZrO_x$ thin films. The $LaZrO_x$ thin film had a equivalent oxide thickness (EOT) value of 8.7 nm. From the capacitance-voltage (C-V) measurements for an Au/$(Bi,La)_4Ti_3O_{12}/LaZrO_x$/Si MFIS capacitor, a hysteric shift with a clockwise direction was observed and the memory window width was about 1.4 V for the bias voltage sweeping of ${\pm}9V$. From drain current-gate voltage $(I_D-V_G)$ characteristics of the fabricated Fe-FETs, the obtained threshold voltage shift (memory window) was about 1 V due to ferroelectric nature of BLT film. The drain current-drain voltage $(I_D-V_D)$ characteristics of the fabricated Fe-FETs showed typical n-channel FETs current-voltage characteristics.

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The Electric Conductivity $SrBi_2Ta_2O_9$ Capacitors using Rf Magnetron Sputtering Technique

  • Cho, C.N.;Shin, C.G.;Song, M.J.;Choi, W.S.;Park, G.H.;So, B.M.;Kim, C.H.
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2008.04b
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    • pp.3-5
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    • 2008
  • The $SrBi_2Ta_2O_9$ thin films are deposited on Pt-coated electrode(Pt/$TiO_2/SiO_2$/Si) using RF magnetron sputtering method. The ferroelectric properties of SBT capacitors with annealing temperatures were studied. Through the x-ray diffraction analysis and the scanning electron microscopy (SEM), it could be observed that crystallization of the SBT thin film started around $650^{\circ}C$ and complete crystallization was accomplished around $750^{\circ}C$ and grains grew from a small spheric form to rod-like. For the leakage current density of the SBT capacitor depending upon various annealing atmospheres, capacitor annealed in the oxygen atmosphere showed the most excellent characteristic, and they were respectively about $2.13\times10^{-9}[A/cm^2]$ at 5V and 340.

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Measurement of Effective Transverse Piezoelectric Coefficients $(e_{31,f})$ of Fabricated Thick PZT Films on $SiN_x/Si$ Substrates ($SiN_x/Si$ 기판에 제조된 후막 PZT의 횡 압전 계수 $(e_{31,f})$ 측정)

  • Jeon, Chang-Seong;Park, Joon-Shik;Lee, Sang-Yeol;Kang, Sung-Goon;Lee, Nak-Kyu;Ha, Kyoang-Hwan
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2004.07b
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    • pp.965-968
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    • 2004
  • Effective transverse Piezoelectric Coefficients $(e_{31,f})$ of thick PZT $(Pb(Zr_{0.52}Ti{0.48}Ti_{0.48})O_3)$ films on $SiN_x/Si$ substrates were measured with PZT thicknesses and top electrode dimensions. $e_{31,f}$ is one of important Parameters characterizing Piezoelectricity of PZT films. Thick PZT films have been used as various sensors and actuators because of their high driving force and high breakdown voltage. Thick PZT films were fabricated on Pt/Ta/$SiN_x$/Si substrates using sol-gel method. Thicknesses of PZT films were $1{\mu}m$ and $1.8{\mu}m$. $|e_{31,f}|$ values of $1.8{\mu}m$-thick-PZT films were higher than those of $1{\mu}$-thick-PZT films. Maximum $|e_{31,f}|$ of $1.8{\mu}$-thick-PZT films was about $50^{\circ}C/m^2$.

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Synthesis of Novel Platinum Precursor and Its Application to Metal Organic Chemical Vapor Deposition of Platinum Thin Films

  • Lee, Sun-Sook;Lee, Ho-Min;Park, Min-Jung;An, Ki-Seok;Kim, Jin-Kwon;Lee, Jong-Heun;Chung, Taek-Mo;Kim, Chang-Gyoun
    • Bulletin of the Korean Chemical Society
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    • v.29 no.8
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    • pp.1491-1494
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    • 2008
  • A novel platinum aminoalkoxide complex, Pt$(dmamp)_2$ has been prepared by the reaction of cis-$(py)_2PtI_2$ with two equivalents of Na(dmamp) (dmamp = 1-dimethylamino-2-methyl-2-propanolate). Single-crystal X-ray crystallographic analysis shows that the Pt(dmamp)2 complex keeps a square planar geometry with each two nitrogen atoms and two oxygen atoms having trans configuration. Platinum films have been deposited on TaN/ Ta/Si substrates by metal organic chemical vapor deposition (MOCVD) using Pt$(dmamp)_2$. As-deposited platinum thin films did not contain any appreciable amounts of impurities except a little carbon. As the deposition temperature was increased, the films resistivity and deposition rate increased. The electrical resistivity (13.6 $\mu\Omega$cm) of Pt film deposited at 400 ${^{\circ}C}$ is a little higher than the bulk value (10.5 $\mu\Omega$cm) at 293 K. The chemical composition, crystalline structure, and morphology of the deposited films were investigated by X-ray photoelectron spectroscopy, X-ray diffraction, and atomic force microscopy.

Annealing Effects of Indium Tin Oxide films grown on 91ass by radio frequency magnetron sputtering technique

  • Jan M. H.;Choi J. M.;Whang C. N.;Jang H. K.;Yu B. S.
    • Journal of the Korean Vacuum Society
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    • v.14 no.3
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    • pp.159-164
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    • 2005
  • Indium tin oxide (ITO) films were deposited on a glass slide at a thickness of 280 nm by radio frequency(rf) magnetron sputtering from a ceramic target composed of $In_2O_3\;(90\%)\;+\;SnO_2\;(10\%)$. We investigated the effects of the annealing temperature (Ta) between 200 and 350'E for 30 min in air on such properties as thermal stability, surface morphology, and crystal structure of the films. X-ray diffraction spectra revealed that all the films were oriented preferably with [222] direction and [440] direction and the peak intensity increased with increasing annealing temperature. X-ray photoelectron spectroscopy (XPS) showed that the sodium was out-diffused from the glass substrate at the annealing temperature of $350^{\circ}C$. The sodium composition of the ITO film amlealed at $350^{\circ}C\;for\;30\;min\;was\;2.5\%$ at the surface. Also the sodium peak almost disappeared after 3 keV $Ar^+$sputtering for 6 min. The visible transmittance of all ITO films was over $77\%$.

Basic characteristics of metal-ferroelectric-insulator-semiconductor structure using a high-k PrOx insulator layer

  • Noda, Minoru;Kodama, Kazushi;Kitai, Satoshi;Takahashi, Mitsue;Kanashima, Takeshi;Okuyama, Masanori
    • Electrical & Electronic Materials
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    • v.16 no.9
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    • pp.64.1-64
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    • 2003
  • A metal-ferroelectric [SrBi$_2$Ta$_2$O$\_$9/ (SBT)-high-k-insulator(PrOx)-semiconductor(Si) structure has been fabricated and evaluated as a key part of metal-ferroelectric-insulator-semiconductor-field-effect-transistor MFIS-FET memory, aiming to improve the memory retention characteristics by increasing the dielectric constant in the insulator layer and suppressing the depolarization field in the SBT layer. A 20-nm PrOx film grown on Si(100) showed both a high of about 12 and a low leakage current density of less than 1${\times}$ 10e-8 A/$\textrm{cm}^2$ at 105 MV/cm. A 400-nm SBT film prepared on PrOx/Si shows a preferentially oriented (105) crystalline structure, grain size of about 130 nm and subface roughness of 3.2 nm. A capacitance-voltage hysteresis is confirmed on the Pt/SBT/PrOx/Si diode with a memory window of 0.3V at a sweep voltage width of 12 V. The memory retention time was about 1 104s, comparable to the conventional Pt/SBT/SiO$\_$x/N$\_$y/(SiO$\_$N/)/Si. The gradual change of the capacitance indicates that some memory degradation mechanism is different from that in the Pt/SBT/SiON/Si structure.

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Fabrication and Characterization of MFIS-FET using Au/SBT/LZO/Si structure

  • Im, Jong-Hyun;Lee, Gwang-Geun;Kang, Hang-Sik;Jeon, Ho-Seung;Park, Byung-Eun;Kim, Chul-Ju
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2008.06a
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    • pp.174-174
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    • 2008
  • Non-volatile memories using ferroelectric-gate field-effect transistors (Fe-FETs) with a metal/ferroelectric/semiconductor gate stack (MFS-FETs) make non-destructive read operation possible. In addition, they also have features such as high switching speed, non-volatility, radiation tolerance, and high density. However, the interface reaction between ferroelectric materials and Si substrates, i.e. generation of mobile ions and short retention, make it difficult to obtain a good ferroelectric/Si interface in an MFS-FET's gate. To overcome these difficulties, Fe-FETs with a metal/ferroelectric/insulator/semiconductor gate stack (MFIS-FETs) have been proposed, where insulator as a buffer layer is inserted between ferroelectric materials and Si substrates. We prepared $SrBi_2Ta_2O_9$ (SBT) film as a ferroelectric layer and $LaZrO_x$ (LZO) film as a buffer layer on p-type (100) silicon wafer for making the MFIS-FET devices. For definition of source and drain region, phosphosilicate glass (PSG) thin film was used as a doping source of phosphorus (P). Ultimately, the n-channel ferroelectric-gate FET using the SBT/LZO/Si Structure is fabricated. To examine the ferroelectric effect of the fabricated Fe-FETs, drain current ($I_d$) versus gate voltage ($V_g$) characteristics in logarithmic scale was measured. Also, drain current ($I_d$) versus drain voltage ($V_d$) characteristics of the fabricated SBT/LZO/Si MFIS-FETs was measured according to the gate voltage variation.

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Potential Characteristics of Supercapacitor Based on Ruthenium Oxide-Aqueous Electrolyte (루테늄 산화물-수계 전해액 수퍼캐패시터의 전위 특성)

  • Doh, Chil-Hoon;Choi, Sang-Jin;Moon, Seong-In;Yun, Mun-Su;Yug, Gyeong-Chang;Kim, Sang-Gil;Lee, Ju-won
    • Journal of the Korean Electrochemical Society
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    • v.6 no.2
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    • pp.93-97
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    • 2003
  • The electrode for a supercapacitor was prepared using an amorphous ruthenium oxide, which was synthesized from ruthenium trichloride hydrate$(RuO_2{\cdot}nH_2O)$. A supercapacitor was assembled with an electrode of ruthenium oxide material on a current collector of tantalum, and an electrolyte of 4.8 M sulfuric acid. The result of the AC impedance analyses on $Ta/H_2SO_4(4.8 M)/Pt$ cell showed that tantalum was stable at the potential range of $0.0\~1.1V(vs. SCE)$. Therefore, Ta film could be used the supercapacitor as a current collector. The irreversible hydrolysis in the supercapacitor occurred over ca. 1.0V(vs.SCE) when the supercapacitor was protonated to 0.5V(vs. SCE). The supercapacitor protonated to 0.5V(vs.SCE) showed good electrochemical properties when it was tested at the potential range of 1.0V in the charge-discharge test. The potential range of the electrodes including the positive and the negative electrode was varied between -0.004 and 0.995V(vs. SCE). The potential ranges of the positive and the negative electrode were $-0.004\~0.515V(vs.\;SCE)\;and\; 0.515\~0.995V(vs.\;SCE)$, respectively.