• Bulletin of the Korean Chemical Society
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• 제23권8호
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• pp.1121-1126
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• 2002

Two anhydrous crystal structures of fully dehydrated Cd2+ - and Cs+ -exchanged zeolite X, Cd32Cs28Si100Al92O384 (Cd32Cs28-X: a = 24.828(11) $\AA)$ and fully dehydrated Cd,sup>2+ - and Rb+ -exchanged zeolite X, Cd28Rb36Si100Al92O384 (Cd28Rb36-X: a = 24.794(2) $\AA$), have been determined by single-crystal X-ray diffraction techniques in the cubic space group Fd3 at $21(1)^{\circ}C.$ The structures were refined to the final error indices, R1 = 0.058 and R2 = 0.065 with 637 reflections for Cd32Cs28-X and R1 = 0.086 and R2 = 0.113 with 521 reflections for Cd28Rb36-X for which I > $3\sigma(I)$. In the structure of Cd,sub>32Cs28-X, 16 Cd2+ ions fill the octahedral sites I at the centers of the double six rings (Cd-O = $2.358(8)\AA$ and O-Cd-O = $90.8(3)^{\circ}$ ). The remaining 16 Cd2+ ions occupy site II (Cd-O = $2.194(8)\AA$ and O-Cd-O = $119.7(4)^{\circ})$ and six Cs+ ions occupy site II opposite to the single six-rings in the supercage; each is $2.322\AA$ from the plane of three oxygens (Cs-O = 3.193(13) and O-Cs-O = $73.0(2)^{\circ}).$ Aboutten Cs+ ions are found at site II', $1.974\AA$ into the sodalite cavity from their three oxygen plane (Cs-O = $2.947(8)\AA$ and O-Cs-O = $80.2(3)^{\circ}).$ The remaining 12 Cs+ ions are distributed over site III' (Cs-O = 3.143(9) and O-Cs-O= $59.1(2)^{\circ})$. In the structure of Cd28Rb36-X, 16 Cd2+ ions fill the octahedral sites I at the center of the double-sixrings (Cd-O = 2.349(15) and O-Cd-O = $91.3(5)^{\circ}$ ). Another 12 Cd2+ ions occupy two different II sites (Cd-O = $2.171(18)/2.269(17)\AA$ and O-Cd-O = $119.7(7)/113.2(7)^{\circ}).$ Fifteen Rb+ ions occupy site II (Rb-O = $2.707(17)\AA$ and O-Rb-O = $87.8(5)^{\circ}).$ The remaining 21 Rb+ ions are distributed over site III' (Rb-O = $3.001(16)\AA$ and O-Rb-O = $60.7(4)^{\circ})$. It appears that the smaller and more highly charged Cd2+ ions prefer sites I and Ⅱ in that order, and the larger Rb+ and Cs+ ions, which are less able to balance the anionic charge of the zeolite framework, occupy sites II and II' with the remainder going to the least suitable site in the structure, site III'.The maximum Cs+ and Rb+ ion exchanges were 30% and 39%, respectively. Because these cations are too largeto enter the small cavities and their charge distributions may be unfavorable, cation-sieve effects might appear.

• 한국재료학회지
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• 제30권1호
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• pp.1-7
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• 2020

Doping or incorporation with exotic elements are two manners to regulate the optoelectronic properties of transparent conducting (TCO) cadmium oxide (CdO). Nevertheless, the method of doping host CdO by CdTe semiconductor is of high importance. The structural, optical, and electrical properties of CdTe-doped CdO films are studied for the sake of promoting their conducting parameters (CPs), including their conductivity, carrier concentration, and carrier mobility, along with transparency in the NIR spectral region; these are then compared with the influence of doping the host CdO by pure Te ions. X-ray fluorescence (XRF), X-ray diffraction (XRD), optical absorption spectroscopy, and electrical measurements are used to characterise the deposited films prepared by thermal evaporation. Numerous results are presented and discussed in this work; among these results, the optical properties are studied through a merging of concurrent BGN (redshift) and BGW (blue shift) effects as a consequence of doping processes. The impact of hydrogenation on the characterisations of the prepared films is investigated; it has no qualitative effect on the crystalline structure. However, it is found that TCO-CPs are improved by the process of CdTe doping followed by hydrogenation. The utmost TCO-CP improvements are found with host CdO film including ~ 1 %Te, in which the resistivity decreases by ~ 750 %, carrier concentration increases by 355 %, and mobility increases by ~ 90 % due to the increase of N_carr. The improvement of TCO-CPs by hydrogenation is attributed to the creation of O-vacancies because of H₂ molecule dissociation in the presence of Te ions. These results reflect the potential of using semiconductor CdTe -doped CdO thin films in TCO applications. Nevertheless, improvements of the host CdO CPs with CdTe dopant are of a lesser degree compared with the case of doping the host CdO with pure Te ions.

• 청정기술
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• 제26권4호
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• pp.311-320
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• 2020

본 연구에서는 단순 침전법으로 제조한 CdS 및 CdZnS/ZnO 광촉매를 이용하여 가시광선하에서 로다민 B, 메틸 오렌지 및 메틸렌 블루 등에 대한 광분해 반응 연구를 수행하였다. 특히 염료와 광촉매의 물리화학적 성질이 전체 광촉매 반응의 반응 경로에 미치는 영향에 대해 중점을 두고 검토하였다. X선 회절분석법, UV-vis 확산반사 분광법 그리고 X선 광전자 분광분석법 등을 이용하여 제조된 촉매들의 물리화학적 특성을 분석하였다. CdS 및 CdZnS/ZnO 광촉매 모두 자외선뿐만 아니라 가시광선 영역에 있어서도 우수한 광흡수 특성을 나타내었다. 메틸 오렌지의 경우에는 CdS 및 CdZnS/ZnO 각각의 광촉매 상에서 동일한 반응기구를 통해 반응이 진행되는 반면, 로다민 B 및 메틸렌 블루는 각각의 광촉매 상에서 서로 다른 반응 경로를 통해 광분해 반응이 진행되는 것으로 나타났다. 특히 메틸렌 블루의 광분해 반응을 보면, CdZnS/ZnO 광촉매 상에서는 주로 단일분자 형태로 전체 반응이 진행되지만, CdS 상에서는 반응 초기부터 이량체를 형성하였다. 이와 같은 결과들은 CdS 및 CdZnS/ZnO 각각의 반도체 광촉매들의 전도대의 띠끝 전위 차이와 염료들의 흡착 특성 차이에 기인한 것으로 판단된다.

• 한국세라믹학회지
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• 제23권4호
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• pp.23-26
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• 1986

The synthetic conditions of $ ZrSiO_4-Cd(S_xS_{1-x})$ stains from CdS, Se, $SiO_2$ , 4ZrO_2$ and Lif were investigated and the colors were examined. Colors of the stains prepared were yellow orange red pink ruby and violet in relation to both the content of CdS-Se in $ZrSiO_4$ and firing temperature. Colors of these series stains were thermally stabilized probably by the structural stability of zirconium silicate. Furthermore by the result of X-ray diffraction analysis it is assumed that color of the zircon cadmium sulphoselenide $ ZrSiO_4-Cd(S_xS_{1-x})$ stain is developed by neither the coloring ions in $ZrSiO_4$ lattice nor the solid solution of $ZrSiO_4$ and $Cd(S_xS_{1-x})$ but by the small crystals of $Cd(S_xS_{1-x})$ being occluded by the zirconium silicate during sintering process.

• 분석과학
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• 제20권5호
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• pp.413-418
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• 2007

방사선 방법에 의해 실리카 나노입자에 CdS 나노입자를 코팅하였다. TEM분석결과, $SiO_2$ 나노입자 표면에 CdS의 입자의 크기는 대략 20 nm임을 확인 하였다. 또한, XRD 분석결과 결정체 화합물임을 확인하였다. PL 분석결과 PVP-CdS 나노입자와 $SiO_2$@CdS 복합체의 경우, 방출특성이 상당히 다르다는 것이 확인되었다. PVP-CdS의 경우, 방출스펙트럼이 550 nm-600 nm 에서 나타나고, $SiO_2$@CdS의 방출스펙트럼의 경우 단파장 이동함을 확인하였다. 또한 새로운 피이크 (450 nm) 나타남을 확인하였는데, 이는 CdS 의 유발양자 제한 효과에 의한 것으로 사료된다.

• 대한화학회지
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• 제29권2호
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• pp.111-120
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• 1985

4 mol% Cd-doped ${\alpha}-Fe_2O_3$, 8 mol% Cd-doped ${\alpha}-Fe_2O_3$ 및 12 mol% Cd-doped ${\alpha}-Fe_2O_3$상에서 CO 산화반응이 각기 연구되었다. Cd의 doping level에 관계없이 반응차수는 1.5차이며 CO에 대하여 1차, $O_2$에 대하여 O.5차이다. 350∼$460^{\circ}C$의 반응온도 범위에서 CO산화반응의 활성화 에너지는 10.10∼11.30Kcal/$mol^{-1}$ 이며 Cd-doped${\alpha}-Fe_2O_3$의 전기전도도 데이타와 반응속도 데이타로부터 CO산화반응 메카니즘이 규명되었다. 특히 Cd doping 효과로부터 ${\alpha}-Fe_2O_3$의 촉매활성이 격자산소의 공위에 포획되어 있는 전자의 여기(excitation)에 기인된다는 사실이 밝혀졌으며 반응분자들의 흡착자리를 알게 되었다.

• 공업화학
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• 제26권3호
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• pp.356-361
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• 2015

$Cd_{0.5}Zn_{0.5}S/ZnO$ 형태의 복합체 광촉매를 침전법으로 제조하였고, 이들 화합물의 특성을 XRD, UV-vis DRS, PL 및 FE-SEM 등을 이용하여 조사하였다. 그리고 가시광선 조사 하에서의 로다민 B 분해반응에 대한 광촉매로서의 활성을 조사하였다. ZnO와는 달리 $Cd_{0.5}Zn_{0.5}S/ZnO$는 자외선 뿐만 아니라 가시광선 영역의 빛도 효율적으로 흡수하며 특히 $Cd_{0.5}Zn_{0.5}S$의 함량 증가에 따라 가시광선 영역의 빛에 대한 흡광도도 증가하였다. 또한 $Cd_{0.5}Zn_{0.5}S/ZnO$에 있어서 $Cd_{0.5}Zn_{0.5}S$의 함량이 증가할수록 최종 입자들의 크기가 작아지고 그 결과 비 표면적이 증가하였다. 로다민 B의 광분해 반응에 있어서는 $Cd_{0.5}Zn_{0.5}S$ 함량이 높은 $Cd_{0.5}Zn_{0.5}S/ZnO$ 촉매일수록 상대적으로 높은 광촉매 활성을 보여주었다. 그러므로 $Cd_{0.5}Zn_{0.5}S/ZnO$ 광촉매의 활성에 있어서는 촉매의 흡착능력 뿐만 아니라 $Cd_{0.5}Zn_{0.5}S$와 ZnO 사이의 heterojunction 효과도 중요하게 작용하는 것으로 보인다.

• 분석과학
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• 제14권3호
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• pp.259-265
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• 2001

ZnO, CdS, rutile-$TiO_2$ 및 혼합 rutile-$TiO_2$/ZnO와 같은 여러 반도체를 이용하여 Congo Red를 광 촉매 분해시켰다. 연구 결과 ZnO, CdS, rutile-$TiO_2$ 중에서는 CdS의 광 촉매 효과가 제일 컸는데 이것은 CdS가 제일 작은 band gap 에너지를 가지고 있기 때문이었다. 또한 혼합 촉매에서는 ZnO의 함량이 rutile-$TiO_2$에 비하여 상대적으로 높을수록 분해 반응을 촉진하였다. 이것은 $Zn^{2+}$ 가수분해 생성물이 구조적으로 안정한 화합물인 rutile-$TiO_2$의 표면을 덮음으로서 자외선 흡수를 차단하기 때문에 라디칼 생성을 저해하기 때문이었다.

• Bulletin of the Korean Chemical Society
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• 제33권1호
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• pp.189-193
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• 2012

ZnO nanorods were grown on the $Cd_xZn_{1-x}O$ seed layers with various Cd mole fractions by hydrothermal method. The effects of the Cd mole fraction for $Cd_xZn_{1-x}O$ seed layers on the structural and optical properties of the ZnO nanorods were investigated by scanning electron microscopy, X-ray diffraction, and photoluminescence. The narrowest full-width at half-maximum and largest grain size of the $Cd_xZn_{1-x}O$ seed layers, indicating improvement in crystal quality, were observed at the Cd mole fraction of 0.5. At the Cd mole fraction of 0.5, the largest enhancement in the density, the crystal quality, and the growth rate of the ZnO nanorods was observed while their appearance was not affected significantly by the incorporation of the Cd in the $Cd_xZn_{1-x}O$ seed layers. Consequently, the luminescent properties of the ZnO nanorods were enhanced. The largest improvement in the structural and optical properties of the ZnO nanorods was observed at the Cd mole fraction of 0.5.

• 한국세라믹학회지
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• 제30권11호
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• pp.897-904
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• 1993

CdS doped SiO2 glass coating films which are good candidates for the nonlinear optical materials were prepared by the Sol-Gel method. TEOS, C2H5OH, H2O and HCl were used as starting materials to obtain SiO2 matrix solutions. Then Cd(NO3)2.2H2O and CS(NH2)2 were dissolved into the SiO2 matrix solutions. Coating was performed several times in order to increase the thickness of coated film by the dip-coating method. Then heat treatments were carried out to control the size of CdS microcrystals doped in SiO2 glass matrix with respect to temperatures and times. CdS-doped SiO2 transparent coating films were successfully obtained. CdS crystals were changed from cubic to hexagonal type about $600^{\circ}C$.