• Title/Summary/Keyword: Charged Vacancy

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Electronic Structure of the SrTiO3(001) Surfaces: Effects of the Oxygen Vacancy and Hydrogen Adsorption

  • Takeyasua, K.;Fukadaa, K.;Oguraa, S.;Matsumotob, M.;Fukutania, K.
    • Applied Science and Convergence Technology
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    • v.23 no.5
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    • pp.201-210
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    • 2014
  • The influence of electron irradiation and hydrogen adsorption on the electronic structure of the $SrTiO_3$ (001) surface was investigated by ultraviolet photoemission spectroscopy (UPS). Upon electron irradiation of the surface, UPS revealed an electronic state within the band gap (in-gap state: IGS) with the surface kept at $1{\times}1$. This is considered to originate from oxygen vacancies at the topmost surface formed by electron-stimulated desorption of oxygen. Electron irradiation also caused a downward shift of the valence band maximum indicating downward band-bending and formation of a conductive layer on the surface. With oxygen dosage on the electron-irradiated surface, on the other hand, the IGS intensity was decreased along with upward band-bending, which points to disappearance of the conductive layer. The results indicate that electron irradiation and oxygen dosage allow us to control the surface electronic structure between semiconducting (nearly-vacancy free: NVF) and metallic (oxygen de cient: OD) regimes by changing the density of the oxygen vacancy. When the NVF surface was exposed to atomic hydrogen, in-gap states were induced along with downward band bending. The hydrogen saturation coverage was evaluated to be $3.1{\pm}0.8{\times}10^{14}cm^{-2}$ with nuclear reaction analysis. From the IGS intensity and H coverage, we argue that H is positively charged as $H^{{\sim}0:3+}$ on the NVF surface. On the OD surface, on the other hand, the IGS intensity due to oxygen vacancies was found to decrease to half the initial value with molecular hydrogen dosage. H is expected to be negatively charged as $H^-$ on the OD surface by occupying the oxygen vacancy site.

A Study of the Effect of Doping on FALC (도핑이 FALC에 미치는 영향에 관한 고찰)

  • Ahn, Ji-Su;Joo, Seung-Ki
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2003.07a
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    • pp.195-198
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    • 2003
  • 본 연구에서는 MILC 및 FALC를 도핑 타입에 따른 온도별 패턴별 인가 전압별로 진행하여 현미경 및 FESEM 관찰을 함으로써 그 메커니즘을 규명하고자 하였다. LPCVD를 이용하여 $1000\;{\AA}$ a-Si 을 glass에 입힌 후 photolithography법 또는 Hard Mask법으로 Ni $200\;{\AA}$ 을 선택적으로 증착하였으며 Pt 전극을 Sputtering법으로 제작하였다. $33\;{\sim}\;200\;V/cm$의 전기장 하에서 MILC 속도가 2배 정도 증가되는 현상이 관찰되었으며 또한 인접패턴에 의해 FALC 속도가 영향을 받는 현상이 관찰되었다. 또한 전자가 움직이는 방향으로 MILC 선단영역 전후에 Void가 발생하는 영역이 존재함을 발견하였다. FESEM 분석을 통하여 FALC 영역 및 Void 영역을 관찰한 결과 도핑 종류에 따라 결정화 양상이 다른 것이 관찰되었으며 Void 분석결과 Charged vacancy가 어닐링시 결집되어 나타나는 것으로 분석할 수 있었다.

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Nonstoichiometry of the Tungsten Oxide (산화 텅스텐의 비화학량론)

  • Ryu, Kwang Hyun;Oh, Eung Ju;Kim, Keu Hong;Yo, Chul Hyun
    • Journal of the Korean Chemical Society
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    • v.39 no.3
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    • pp.157-162
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    • 1995
  • The x values and electrical conductivities of the nonstoichiometric compounds $WO_{3-x}$ have been measured in the temperature range from 350 to 700$^{\circ}C$ under oxygen partial pressure of $2{\times}10_{-1}\;to\;1{\times}10_{-5}$ atm. The enthalpy of the defect formation shows an endothermic process, and the oxygen pressure dependence of the defect formation or 1/n varies from -1/5.2 to -1/5.9. The activation energy and 1/n value for the electrical conductivity are 0.24~0.29 eV and -1/4.3~-1/7.6, respectively. The Tungsten Oxide as a n-type semiconductor has predominently defect model of singly charged oxygen vacancy at low temperature, and of doubly charged oxygen vacancy at high temperature.

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Investigation on the Stability Enhancement of Oxide Thin Film Transistor (산화물반도체 트랜지스터 안정성 향상 연구)

  • Lee, Sang Yeol
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.26 no.5
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    • pp.351-354
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    • 2013
  • Thin-film transistors(TFTs) with silicon-zinc-tin-oxide(SiZnSnO, SZTO) channel layer are fabricated by rf sputtering method. Electrical properties were changed by different annealing treatment of dry annealing and wet annealing. This procedure improves electrical property especially, stability of oxide TFT. Improved electrical properties are ascribed to desorption of the negatively charged oxygen species from the surfaces by annealing treatment. The threshold voltage ($V_{th}$) shifted toward positive as increasing Si contents in SZTO system. Because the Si has a lower standard electrode potential (SEP) than that that of Sn, Zn, resulting in the degeneration of the oxygen vacancy ($V_O$). As a result, the Si acts as carrier suppressor and oxygen binder in the SZTO as well as a $V_{th}$ controller, resulting in the enhancement of stability of TFTs.

Electrical Conductivity of the Solid Solutions X $ZrO_2+ (1-X) Yb_2O_3; 0.01{\leq}X{\leq}0.09$

  • Choi Byoung Ki;Jang Joon Ho;Kim, Seong Han;Kim, Hong Seok;Park, Jong Sik;Kim Yoo Young;Kim, Don;Lee Sung Han;Yo Chul Hyun;Kim Keu Hong
    • Bulletin of the Korean Chemical Society
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    • v.13 no.3
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    • pp.248-252
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    • 1992
  • $ZrO_2-dopedYb_2O_3solid$ solutions containing 1, 3, 5, 7 and 9 mol% $ZrO_2were$ synthesized from spectroscopically pure $Yb_2O_3$ and $ZrO_2$ powders and found to be rare earth C-type structure by XRD technique. Electrical conductivities were measured as a function of temperatures from 700 to $1050^{\circ}C$ and oxygen partial pressures from 1${\times}$$10^-5$ to 2${\times}$ $10^-1$atm. The electrical conductivities depend simply on temperature and the activation energies are determined to be 1.56-1.68 $_eV$. The oxygen partial pressure dependence of the electrical conductivity shows that the conductivity increases with increasing oxygen partial pressure, indicating p-type semiconductor. The $PO_2$ dependence of the system is nearly power of 1/4. It is suggested from the linearity of the temperature dependence of electrical conductivity and only one value of 1/n that the solid solutions of the system have single conduction mechanism. From these results, it is concluded that the main defects of the system are negatively doubly charged oxygen interstitial in low. $ZrO_2doping$ level and negatively triply charged cation vacancy in high doping level and the electrical conduction is due to the electronic hole formed by the defect structure.

Infrared Spectra and Electrical Conductivity of The Solid Solutions X MgO + (1-X) ${\alpha}-Nb_2$ $O_5$; 0.01{\leq}X{\leq}0.09

  • Park Zin;Park, Jong Sik;Lee Dong Hoon;Jun Jong Ho;Yo Chul Hyun;Kim Keu Hong
    • Bulletin of the Korean Chemical Society
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    • v.13 no.2
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    • pp.127-131
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    • 1992
  • Changes in network structures of ${\alpha}-Nb_2O_5$ in the X MgO+(1-X) ${\alpha}-Nb_2O_5$ solid solutions occurring as the MgO doping level (X) was varied were investigated by means of infrared spectroscopy and X-ray analysis. X-ray diffraction revealed that all the synthesized specimens have the monoclinic structure. The FT-IR spectroscopy showed that the system investigated forms the solid solutions in which $Mg^{2+}$ ions occupy the octahedral sites in parent crystal lattice. Electrical conductivities were measured as a function of temperature from 600 to $1050{\circ}$ and $P_{O2}$ form $1{\times}10^{-5}$ to $2{\times}10^{-1}$ atm. The defect structure and conduction mechanism were deduced from the results. The $1}n$ value in ${\alpha}{\propto}{P_{O2}^{1}n}}$ is found to be -1/4 with single possible defect model. From the activation energy ($E{\alpha}$ = 1.67-1.73 eV) and the1/n value, electronic conduction mechanism is suggested with a doubly charged oxygen vacancy.

Varistor Application of Cr-doped ZnO-Sb2O3 Ceramics (Cr을 첨가한 ZnO-Sb2O3 세라믹스의 바리스터 응용)

  • Hong, Youn-Woo;Shin, Hyo-Soon;Yeo, Dong-Hun;Kim, Jin-Ho
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.23 no.11
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    • pp.854-858
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    • 2010
  • In this study, we have investigated the effects of Cr dopant on the sintering and electrical properties of ZnO-$Sb_2O_3$ (ZS) ceramics for varistor application. Spinel phases including $\alpha-$ and $\beta$-type was formed at ZS system and $\alpha$-spinel was stabilized by Cr doping in ZS system. Densification of ZS and ZSCr system was retarded to $1000^{\circ}C$ by the formation of spinel at $800^{\circ}C$. The morphology and its distribution of spinel phases in ZS system was homogeneous but disturbed by Cr doping. In ZSCr the densification of ZnO compared with ZS system was more retarded by low concentration of Zn interstitial defects induced by Cr doping in addition to the effect of spinel phase formation. The defects in each system were identified as attractive coulombic center (ZS: 0.13 eV, ZSCr: 0.12 eV) and singly charged oxygen vacancy $V_0^{\cdot}$ (ZSCr: 0.33 eV). In all ZS and ZSCr system have week varistor behavior by the formation of double Schottky barrier at grain boundary but its stability of barrier was very sensitive to sintering temperature.