• Title/Summary/Keyword: $Ta_2O_{5}$

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RTN과 Wet Oxidation에 의한 $Ta_2O_5$의 전기적 특성의 최적화

  • 정형석;임기주;양두영;황현상
    • Proceedings of the Korean Vacuum Society Conference
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    • 2000.02a
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    • pp.104-104
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    • 2000
  • MOS소자의 크기가 작아짐에 따라 gate 유전막의 두께 또한 얇아져야 한다. 두께가 얇아짐에 따라 gate 유전막으로써 기존의 SiO2는 direct tunneling으로 인해 높은 누설전류를 수반한다. 그래서 높은 유전상술르 가지는 물질들에 대한 연구의 필요성이 대두되고 있다. 그중 CVD-Ta2O5는 차세대 MOSFET소자기술에 있어서 높은 유전상수($\varepsilon$r+25)와 우수한 step coverage 때문에 각광을 받고 있는 물질중에 하나이다. 본 연구에서는 Ta2O5를 gate를 유전막으로 사용하고 RTN처리와 wet oxidation을 접목시켜 이들의 전기적인 특성을 향상시킬 수 있었다. p-형 wafer 위에 D2와 O2를 사용하여 SiO2(100 )를, NH3를 이용하여 Nitridation(10 )을 전처리로써 각각 실시하였고 그 위에 MOCVD방법으로 Ta2O5를 80 성장시켰다. 첫 번째 시편은 45$0^{\circ}C$ 10min동안 wet oxidation을 시켰고, 두 번째 시편은 $700^{\circ}C$ 60sec동안 NH3 분위기에서 RTN 처리를 하였다. 세 번째 시편은 동일조건으로 RTN 처리후 wet oxidation을 하였다. 그 후 각각의 시편을 capacitor를 제작하고 그 전기적 특성을 관찰하였다. Wet oxidation만을 시킨 시편은 as-deposited Ta2O5 시편에 비해서 -1.5V에서 누설전류는 약 2~3 order정도 감소되었고 accumulation 영역에서의 capacitance 값은 oxide층의 성장(5 )을 무시하면 거의 변화하지 않았다. RTN처리만 된 시편의 경우는 -1.5V에서 누설전류는 2~3order 정도 증가되었지만, accumulation 영역에서 capacitance 값은 거의 2qwork 증가하였다. 이 두가지 공정을 접목시킨 즉 RTN 처리후 wet oxidation 처리된 시편의 경우는 as-deposited Ta2O5 시편에 비해서 -1.5V에서 누설전류는 1 order 정도 감소하였고, accumulation 지역에서의 capacitance 값은 약 2배 증가하였다. 즉 as deposited Ta2O5 시편의 accumulation 지역의 capacitance 값은 12.8 fF/um2으로써 그 유효두께는 27.0 이었지만, RTN 처리후에 wet oxidation 시킨 시편의 accumulation 지역의 capacitance값은 21.2fF/um2으로써 그 유효두께는 16.3 이 되었다. 결론적으로 as deposited Ta2O5 시편에 RTN 처리후 wet oxidation을 실시한 결과 capacitance 값이 약 2배정도 증가하였고 누설전류는 약 1 order 정도 감소됨을 확인하였다.

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Structural and Microwave Dielectric Properties of $Mg_{5}B_{4}O_{15}$ (B=Ta, Nb) Ceramics with Sintering Temperature (소결온도에 따른 $Mg_{5}B_{4}O_{15}$ (B=Ta, Nb) 세라믹스의 구조 및 마이크로파 유전 특성)

  • Kim, Jae-Sik;Choi, Eui-Sun;Lee, Moon-Kee;Ryu, Ki-Won;Lee, Young-Hie
    • Proceedings of the KIEE Conference
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    • 2006.07c
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    • pp.1420-1421
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    • 2006
  • In this study, structural and micowave dielectric properties of the $Mg_{5}B_{4}O_{15}$ (B=Ta, Nb) cation-deficient perovskite ceeramics. The specimens are prepared through the solid-state route. According to the XRD pattern, $Mg_{4}Ta_{2}O_9$ and $MgTa_{2}O_6$ phase exist in calcined and sintered $Mg_{5}Ta_{4}O_{15}$ powder. Also $Mg_{5}Ta_{4}O_{15}$ phase added with increasing sintering temperature. In the case of calcined and sintered $Mg_{5}Nb_{4}O_{15}$ powder, single phase of $Mg_{5}Nb_{4}O_{15}$ were appeared. The bulk density and quality factor of the $Mg_{5}B_{4}O_{15}$ (B=Ta, Nb) ceramics were increased with sinteming temperature in $1400^{\circ}C{\sim}1450^{\circ}C$, but these were decreased in another sintering temperature. Dielectric constant of the $Mg_{5}Ta_{4}O_{15}$ ceramics was increased continuously with increasing of sintering temperature. And the dielectric constant of the $Mg_{5}Nb_{4}O_{15}$ ceramics was increased in $1400^{\circ}C{\sim}1450^{\circ}C$ but decreased in $1475^{\circ}C$. In the case of the $Mg_{5}Ta_{4}O_{15}$ and $Mg_{5}Nb_{4}O_{15}$ ceramics sintered at $1450^{\circ}C$ for 5h, the dielectric constant, quality factor, and temperature coefficient of the resonant frequency (TCRF) were 8.2, 259,473 GHz, -10.91 $ppm/^{\circ}C$ and 14, 37,350 GHz, -52.3 $ppm/^{\circ}C$, respectively.

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Scattering measurement of dielectric high reflection mirrors by TIS method (TIS 방법을 이용한 유전체 고반사 거울의 산란 측정)

  • 조현주;박흥진;황보창권;문환구;김진태;손승현;이재철
    • Korean Journal of Optics and Photonics
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    • v.8 no.4
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    • pp.283-290
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    • 1997
  • Scattering measurement on high reflection dielectric multilayer mirrors deposited on quartz substrate in a vacuum chamber were performed using a total integrated scattering method. Scattering of (Ta$_2$$O_5$/SiO$_2$) multilayer mirrors deposited at 250-30$0^{\circ}C$ was 0.048-0.050% and did not change with an annealing at 30$0^{\circ}C$ for 4 hours. On the other hand, scattering of (TiO$_2$/SiO$_2$) multilayer mirror at 25$0^{\circ}C$ was 0.029% and it showed the heavy tensile stress after an annealing. The rms roughness of (Ta$_2$$O_5$/SiO$_2$) multilayer mirror was almost the same as that of (TiO$_2$/SiO$_2$)multilayer mirror. The column size of Ta$_2$$O_5$ film was smaller than that of TiO$_2$film and the packing density of (Ta$_2$$O_5$/SiO$_2$) multilayer mirrors was higher than that of (TiO$_2$/SiO$_2$) multilayer mirror. It seems that the higher packing density and smaller column size of Ta$_2$$O_5$ films lead to more scattering.

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Structural Characterization of the (TEX)$Sr_2Co_0.5Nb(Ta)_0.5O_4$(/TEX) and (TEX)$Sr_3CoNb(Ta)O_7$(/TEX)

  • Jo, Han Sang;Ri-Zhu Yin;Ryu, Gwang Hyeon;Yu, Cheol Hyeon
    • Bulletin of the Korean Chemical Society
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    • v.21 no.7
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    • pp.679-684
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    • 2000
  • The Sr2Co0.5Nb(Ta)0.5O4 and Sr3CoNb(Ta)O7 compounds, both with Ruddlesden-Popper structures, have been synthesized by the ceramic method at $1150^{\circ}C$ under atmospheric pressure. The crystallographic structure of the compounds was assigned to the tetr agonal system with space group 14/mmm by X-ray diffraction(XRD) Rietveld refinement. The reduced lattice volume and lattice parameters increased as the Ta with 5d substitutes for the Nb with 4d in the compounds. The Co/Nb(Ta)O bond length has been determined by X-ray absorption spectroscopic(EXAFS/XANES) analysis and the XRD refinement. The CoO6,octahedra were tetragonally distorted by elongation of Co-O bond along the c-axis. The magnetic measurement shows the compounds Sr2Co0.5Nb(Ta)0.5O4 and Sr3CoNb(Ta)O7 have paramagnetic properties and the Co ions with intermediate spin sates between high and low spins in D4h symmetry. All the compounds showed semiconducting behavior whose electrical conductivity increased with temperature up to 1000 K. The electrical conductiviy increased and the activation energy for the conduction decreased as the number of perovskite layers increased in the compounds with chemical formula An+1BnO3n+1.

Two-Dimensional Electron Gas (2DEG) at $Ta_2O_5/SrTiO_3$ Heterointerface

  • Joung, Jin Gwan;Yoo, Kwang Soo;Kim, Jin Sang;Baek, Seung-Hyub
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.02a
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    • pp.161-161
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    • 2013
  • Two-dimensional electron gas (2DEG) has been investigated at the heterointerface between two insulating dielectric perovskite oxides, $LaAlO_3$ (LAO)/$SrTiO_3$ (STO). Properties of the 2DEG have attracted an enormous interest in condensed matter physics due to multifunctional properties such as the coexistence of ferromagnetism and superconductivity, as well as the high electron mobility. Here, we have grown $Ta_2O_5$ thin films using pulsed laser deposition on $SrTiO_3$ substrate to investigate the electric properties of the $Ta_2O_5$/STO heterointerface. Our research reveal that the non-polar $Ta_2O_5$/$TiO_2$ heterointerface favors the formation of 2DEG similar to that at the LAO/STO heterointerface. The metallic behavior was found in this heterointerface with the current about $10{\sim}100{\mu}A$ at 5 V by using conventional I-V measurements, when the $Ta_20_5$ film thickness reaches over critical thickness, $d_c{\simeq}2uc$. The finding that electrons was localized at $Ta_2O_5$/STO heterointerface have attracted to be strong and new candidate for nanoscale oxide device applications.

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High density plasma etching of novel dielectric thin films: $Ta_{2}O_{5}$ and $(Ba,Sr)TiO_{3}$

  • Cho, Hyun
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.11 no.5
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    • pp.231-237
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    • 2001
  • Etch rates up to 120 nm/min for $Ta_{2}O_{5}$ were achieved in both $SF_{6}/Ar$ and $Cl_{2}/Ar$ discharges. The effect of ultraviolet (UV) light illumination during ICP etching on $Ta_{2}O_{5}$ etch rate in those plasma chemistries was examined and UV illumination was found to produce significant enhancements in $Ta_{2}O_{5}$ etch rates most likely due to photoassisted desorption of the etch products. The effects of ion flux, ion energy, and plasma composition on (Ba, Sr)$TiO_3$ etch rate were examined and maximum etch rate ~90 nm/min was achieved in $Cl_{2}/Ar$ ICP discharges while $CH_{4}/H_{2}/Ar$ chemistry produced extremely low etch rates (${\leq}10\;nm/min$) under all conditions.

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Electrical and Chemical Properties of ultra thin RT-MOCVD Deposited Ti-doped $Ta_2O_5$

  • Lee, S. J.;H. F. Luan;A. Mao;T. S. Jeon;Lee, C. h.;Y. Senzaki;D. Roberts;D. L. Kwong
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.1 no.4
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    • pp.202-208
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    • 2001
  • In Recent results suggested that doping $Ta_2O_5$ with a small amount of $TiO_2$ using standard ceramic processing techniques can increase the dielectric constant of $Ta_2O_5$ significantly. In this paper, this concept is studied using RTCVD (Rapid Thermal Chemical Vapor Deposition). Ti-doped $Ta_2O_5$ films are deposited using $TaC_{12}H_{30}O_5N$, $C_8H_{24}N_4Ti$, and $O_2$ on both Si and $NH_3$-nitrided Si substrates. An $NH_3$-based interface layer at the Si surface is used to prevent interfacial oxidation during the CVD process and post deposition annealing is performed in $H_2/O_2$ ambient to improve film quality and reduce leakage current. A sputtered TiN layer is used as a diffusion barrier between the Al gate electrode and the $TaTi_xO_y$ dielectric. XPS analyses confirm the formation of a ($Ta_2O_5)_{1-x}(TiO_2)_x$ composite oxide. A high quality $TaTi_xO_y$ gate stack with EOT (Equivalent Oxide Thickness) of $7{\AA}$ and leakage current $Jg=O.5A/textrm{cm}^2$ @ Vg=-1.0V has been achieved. We have also succeeded in forming a $TaTi_x/O_y$ composite oxide by rapid thermal oxidation of the as-deposited CVD TaTi films. The electrical properties and Jg-EOT characteristics of these composite oxides are remarkably similar to that of RTCVD $Ta_2O_5, suggesting that the dielectric constant of $Ta_2O_5$ is not affected by the addition of $TiO_2$.

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A Study on the Electrical Properties of $Ta_2O_{5}$ Thin Films by Atomic Layer Deposition Method in MOS Structure (MOS구조에서의 원자층 증착 방법에 의한 $Ta_2O_{5}$ 박막의 전기적 특성에 관한 연구)

  • 이형석;장진민;임장권;하만효;김양수;송정면;문병무
    • The Transactions of the Korean Institute of Electrical Engineers C
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    • v.52 no.4
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    • pp.159-163
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    • 2003
  • ln this work, we studied electrical characteristics and leakage current mechanism of $Ta_2O_{5}$ MOS(Metal-Oxide-Semiconductor) devices. $Ta_2O_{5}$ thin film (63 nm) was deposited by ALD(Atomic Layer Deposition) method at temperature of 235 $^{\circ}C$. The structures of the $Ta_2O_{5}$ thin films were examined by XRD(X-Ray Diffraction). From XRD, it is found that the structure of $Ta_2O_{5}$ is single phase and orthorhombic. From capacitance-voltage (C-V) anaysis, the dielectric constant was 19.4. The temperature dependence of current density-electric field (J-E) characteristics of $Ta_2O_{5}$ thin film was studied at temperature range of 300 - 423 K. In ohmic region (<0.5 MV/cm), the resistivity was 2.456${\times}10^{14}$ ($\omega{\cdot}cm$ at 348 K. The Schottky emission is dominant at lower temperature range from 300 to 323 K and Poole-Frenkel emission is dominant at higher temperature range from 348 to 423 K.

The Electrical Properties of $Ta_2O_5$ Thin Films by Atomic Layer Deposition Method (원자층 증착 방법에 의한 $Ta_2O_5$ 박막의 전기적 특성)

  • Lee, Hyung-Seok;Chang, Jin-Min;Jang, Yong-Un;Lee, Seung-Bong;Moon, Byung-Moo
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2002.05c
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    • pp.41-46
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    • 2002
  • In this work, we studied electrical characteristics and leakage current mechanism of Au/$Ta_2O_5$/Si metal-oxide-semiconductor (MOS) devices. $Ta_2O_5$ thin film (63nm) was deposited by atomic layer deposition (ALD) method at temperature of $235^{\circ}C$. The structures of the $Ta_2O_5$ thin films were examined by X-Ray Diffraction (XRD). From XRD, the structure of $Ta_2O_5$ was single phase and orthorhombic. From capacitance-voltage (C-V) analysis, the dielectric constant was 19.4. The temperature dependence of current-voltage (I-V) characteristics of $Ta_2O_5$ thin film was studied from 300 to 423 K. In ohmic region (<0.5 MVcm${-1}$), the resistivity was $2.4056{\times}10^{14}({\Omega}cm)$ at 348 K. The Schottky emission is dominant in lower temperature range from 300 to 323 K and Poole-Frenkel emission dominant in higher temperature range from 348 to 423 K.

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