• Transactions on Electrical and Electronic Materials
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• 제15권1호
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• pp.24-27
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• 2014

In this study, the effects of Mn-doping and the electrode materials on the memory characteristics of $ZnO_xS_{1-x}$ resistive random access memory (ReRAM) devices on plastic are investigated. Compared with the undoped Al/$ZnO_xS_{1-x}$/Au and Al/$ZnO_xS_{1-x}$/Cu devices, the Mn-doped ones show a relatively higher ratio of the high resistance state (HRS) to low resistance state (LRS), and narrower resistance distributions in both states. For the $ZnO_xS_{1-x}$ devices with bottom electrodes of Cu, more stable conducting filament paths are formed near these electrodes, due to the relatively higher affinity of copper to sulfur, compared with the devices with bottom electrodes of Au, so that the distributions of the set and reset voltages get narrower. For the Al/$ZnO_xS_{1-x}$/Cu device, the ratio of the HRS to LRS is above $10^6$, and the memory characteristics are maintained for $10^4$ sec, which values are comparable to those of ReRAM devices on Si or glass substrates.

• 한국자기학회지
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• 제18권2호
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• pp.75-78
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• 2008

$AB_2X_4$((A, B)=Transition Metal, X=O, S, Se) 물질에서의 8면체 자리의 이온 거동과 4면체 자리 이온과의 상호작용에 대하여 많은 연구가 이루어지고 있다. 본 연구에서는 4면체 자리에 비자성 이온인 Zn 이온을 치환함에 따른 자기구조의 변화를 관측하여 8면체 자리의 자기구조를 분석하고자 하였다. Cr이온의 일부를 Fe로 치환한 $[Co_{0.9}Zn_{0.1}]_A[Cr_{1.98}{^{57}Fe_{0.02}}]_BO_4$의 닐온도($T_N$는 90K로 $CoCr_{1.98}{^{57}Fe_{0.02}}O_4$ 비하여 감소하였다. 4.2 K에서의 초미세자기장값의 분석결과, 초미세자기장값의 작은 차이를 보이는 잘 분리된 2-set 형태로 나타났으며, $CoCr_{1.98}{^{57}Fe_{0.02}}O_4$의 초미세자기장값은 488, 478 kOe 인데 반하여, $Co_{0.9}Zn_{0.1}Cr_{1.98}{^{57}Fe_{0.02}}O_4$의 초미세자기장값은 $B_1=486$, $B_2=468$ kOe으로 나타났다. Zn 이온의 치환에 따라서 초미세자기장값의 변화를 알 수 있었다. 이러한 결과로 인하여, Zn 이온이 x=0.1 치환된 물질의 경우, 스핀재정렬온도($T_S$)가 18K으로 감소함을 알 수 있다.

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2004년도 하계학술연구발표회 논문개요집
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• pp.180-181
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• 2004

• Bulletin of the Korean Chemical Society
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• 제35권4호
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• pp.1182-1190
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• 2014

$Cd_{1-x}Zn_xS$-sensitized $K_4Nb_6O_{17}$ composite photocatalysts (designated $Cd_{1-x}Zn_xS/K_4Nb_6O_{17}$) were prepared via a simple deposition-precipitation method. The samples were characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM), energy dispersive X-ray spectrometry (EDS), $N_2$ sorption, ultraviolet-visible light diffuse reflectance spectroscopy (UV-Vis DRS), photoluminescence measurements (PL), and X-ray photoelectron spectroscopy (XPS). The $Cd_{0.8}Zn_{0.2}S$ particles were scattered on the surface of $K_4Nb_6O_{17}$, and had a relatively uniform size distribution around 50 nm. The absorption edge of $K_4Nb_6O_{17}$ was shifted to the visible light region and the recombination of photo-generated electrons and holes suppressed after $Cd_{0.8}Zn_{0.2}S$ loading. The $Cd_{0.8}Zn_{0.2}S$(25 wt %)/$K_4Nb_6O_{17}$ composite possessed the highest photocatalytic activity for hydrogen production under visible light irradiation, evolving 8.278 mmol/g in 3 h. Recyclability tests were performed, and the composite photocatalysts were found to be fairly stable. The mechanism of charge separation between the photogenerated electrons and holes at the $Cd_{0.8}Zn_{0.2}S/K_4Nb_6O_{17}$ composite was discussed.

• 대한전기학회논문지
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• 제43권4호
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• pp.613-619
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• 1994

Dielectric properties of Ba(ZnS11/3TTaS12/3T)OS13T+x ZnO(x=0, 0.4, 0.8, 1.0 wt%) ceramics have been investigated at microwave frequencies. With excess ZnO, the sinterability was improved and the dielectric constant($\varepsilon$S1rT) and the unloaded quality factor(QS1UT) were increased. The structure changed into hexagonal from pseudocubic as being annealed at 140$0^{\circ}C$ in excess ZnO composition. Also, the temperature coefficient of the resonant frequency ($\tau$S1fT) turned into (-)ppm/$^{\circ}C$ when sintered at 155$0^{\circ}C$ for 2 hours. But the specimen sintered in ZnO muffling showed increased density and $\varepsilon$S1rT but lowerde QS1uT. Among the specimen investigated, expecially the composition added with 0.4wt% excess ZnO showed the most optimum dielectric values ($\varepsilon$S1rT=28, QS1uT x f=120000GHz) better than those of original Ba(ZnS11/2T TaS12/3T)OS13T ceramics.

• Corrosion Science and Technology
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• 제11권1호
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• pp.1-8
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• 2012

The development of martensitic grades which can be processed in continuous galvanizing lines requires the reduction of the oxides formed on the steel during the hot dip process. This reduction mechanism was investigated in detail by means of High Resolution Transmission Electron Microscopy (HR-TEM) of cross-sectional samples. Annealing of a martensitic steel in a 10% $H_2+N_2$ atmosphere with the dew point of $-35^{\circ}C$ resulted in the formation of a thin $_{C-X}MnO.SiO_{2}$ (x>1) oxide film and amorphous $_{a-X}MnO.SiO_{2}$ oxide particles on the surface. During the hot dip galvanizing in Zn-0.13%Al, the thin $_{C-X}MnO.SiO_{2}$ (x>1) oxide film was reduced by the Al. The $_{a-X}MnO.SiO_{2}$ (x<0.9) and $a-SiO_{2}$ oxides however remained embedded in the Zn coating close to the steel/coating interface. No $Fe_{2}Al_{5-X}Zn_{X}$ inhibition layer formation was observed. During hot dip galvanizing in Zn-0.20%Al, the $_{C-X}MnO.SiO_{2}$ (x>1) oxide film was also reduced and the amorphous $_{a-X}MnO.SiO_{2}$ and $a-SiO_{2}$ particles were embedded in the $Fe_{2}Al_{5-X}Zn_{X}$ inhibition layer formed at the steel/coating interface during hot dipping. The results clearly show that Al in the liquid Zn bath can reduce the crystalline $_{C-X}MnO.SiO_{2}$ (x>1) oxides but not the amorphous $_{a-X}MnO.SiO_{2}$ (x<0.9) and $a-SiO_{2}$ oxides. These oxides remain embedded in the Zn layer or in the inhibition layer, making it possible to apply a Zn or Zn-alloy coating on martensitic steel by hot dipping. The hot dipping process was also found to deteriorate the mechanical properties, independently of the Zn bath composition.

• 한국결정성장학회지
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• 제28권5호
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• pp.222-227
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• 2018

$Zn_{1-x}Co_x$ Zeolitic Imidazolate Framework-8(ZIF)(x = 0~0.05)를 2-methylimidazole을 사용하여 $Zn^{2+}$와 $Co^{2+}$를 공침시켜 합성하고, 이를 $600^{\circ}C$에서 2시간 열처리하여 순수한 ZnO 나노입자와 Co가 도핑된 ZnO 나노입자를 합성했다. x가 < 0.05일 경우, 2-methylimidazole 링커가 $Zn^{2+}$ 및 $Co^{2+}$ 모두에 강하게 배향되어 균질한 Zn/Co ZIFs가 합성되었으며, 열처리를 통해 Co가 균일하게 도핑된 ZnO를 합성할 수 있었다. 반면, $x{\geq}0.05$일 때는 불균질한 Zn/Co ZIFs가 합성되었으며, 열처리 이후 $Co_3O_4$ 이차상이 형성되었다. 합성된 나노입자들에 대한 가스감응특성 평가 결과, 3 at%의 Co가 도핑된 ZnO 센서는 순수한 ZnO와는 달리 trimethylamine에 대해 고감도, 고선택적 가스감응특성을 나타냈다. 본 연구의 bimetallic ZIF 유도 산화물 나노복합체 합성방법은 고성능 가스센서를 설계하는데 활용될 수 있을 것으로 기대된다.

• 한국자기학회지
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• 제15권2호
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• pp.137-141
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• 2005

Spinel계 유화물 $Zn_xFe_{1-x}Cr_2S_4$(x=0.05, 0.1, 0.2)에 대하여 X선 회절법, 자기저항측정, $M\ddot{o}ssbauer$ 분광법을 이용하여 CMR 특성과 자기적 성질을 연구하였다. 결정구조는 상온에서 입방정으로 정상 spinel 구조를 갖는 것으로 나타났다. 자기저항 실험결과 160K 부근 이하에서는 반도체적 전기전도 특성을 보이며, Curie 온도부근에서 최대자기저항 온도가 나타났다. Zn 조성값이 증가함에 따라 Jahn-Teller 효과에 의한 완화 현상이 증가되었으며, 전기 사중극자 이동값 역시 증가되고, 초미세 자기장값은 감소하였다. CMR 특성은 heterovalency에 의한 이중교환 상호작용이나, $Fe^{2+}$와 $Cr^{3+}$ 그리고 $Fe^{3+}$ 사이의 삼중교환 상호작용과는 다른 동적 Jahn-Teller 효과에 의한 도체-반도체전이와 절반 금속성 에너지 밴드구조에서 스핀전자 전이에 의하여 발생되는 것으로 예측된다.

• 한국세라믹학회지
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• 제28권3호
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• pp.225-233
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• 1991

In this study, we tried to find out the appropriate synthetic condition and magnetic properties of Ni-Zn ferrite {(NixZn1-x)Fe2O4} powders (where X=0, 0.1, 0.2, 0.3, ……0.9, 1). Ferrite powders were prepared by wet-direct method at 86℃ for 6hrs from FeCl36H2O, NiCl26H2O, and ZnCl2. The powders of (NixZn1-x)Fe2O4 (where X=0.4, 0.5, 0.6) have a good crystallinity, but the other ferrite powders consist of crystal and precursor ferrite. The ferrite powder's lattice constant is increased when ratio of ZnO contant is increased in the ferrite composition. And initial permeability was measured after sintering, result indicated regular pattern except (Ni0.4Zn0.6)Fe2O4 when the frequency were changed 10KHz to 10MHz.

• Korean Chemical Engineering Research
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• 제55권1호
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• pp.93-98
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• 2017

본 실험에서는 $Cu_2ZnSnS_4$(CZTS) 태양전지의 흡수층 상부에 다양한 조성을 갖는 $Zn(O_x,S_{1-x})$ 버퍼층을 적용하여 특성 변화를 살펴보았다. $Zn(O_{0.76},S_{0.24})$, $Zn(O_{0.56},S_{0.44})$, $Zn(O_{0.33},S_{0.67})$ 그리고 $Zn(O_{0.17},S_{0.83})$의 4가지 단일막의 경우, 전자-정공의 재결합 억제에 유리한 밴드갭 구조를 나타내는 $Zn(O_{0.76},S_{0.24})$ 버퍼층을 소자에 적용했다. $Zn(O_{0.76},S_{0.24})$ 버퍼층을 소자에 적용 시, 흡수층으로부터 S가 버퍼층으로 확산되어 소자 내에서의 버퍼층은 $Zn(O_{0.7},S_{0.3})$의 조성을 나타냈다. CdS 버퍼층의 $E_V$보다 낮은 에너지 준위를 갖는 $Zn(O_{0.7},S_{0.3})$ 버퍼층은 전자-정공 재결합을 효과적으로 억제하기 때문에 CZTS 태양전지의 $J_{SC}$와 $V_{OC}$ 특성을 향상시켰다. 이를 통해 CdS 버퍼층이 적용된 CZTS 태양전지의 효율인 2.75%가 $Zn(O_{0.7},S_{0.3})$ 버퍼층 적용을 통해 4.86%로 향상되었다.