• Bulletin of the Korean Chemical Society
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• 제23권12호
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• pp.1754-1758
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• 2002

Tetrathiafulvalene(TTF) reacts with $PdCl_2,Pd(NO_3)_2$ and $Pd(hfacac)_2$(hexafluoroacetylacetonate) in ethanol to give $(TTF)_{1.5}PdCl_2$ (1a), $(TTF)_3Pd(NO_3)_2$ (1b) and $(TTF)_4Pd(hfacas)_2$ nd (1c), respectively. $PdCl(TCNQ)_{2.5}{\cdot}CH_3OH(2a)$was obtained from the reaction of $PdCl_2$ with LiTCNQ in methanol via the partial replacement of $Cl^-$ in $PdCl_2$ by $TCNQ^-$anion, whereas the total substitution of the labile $NO_3^-$ in $Pd(NO_3)_2$ yielded pd(TCNQ)·$CH_3OH$ (2b). $Pd(hfacac)_2(TCNQ)_2\cdot3CH_3OH$ (2c) was obtained from $Pd(hfacac)_2$ and LiTCNQ in methanol. The prepared compounds were characterized by spectroscopic (IR, UV, XPS) methods and magnetic (EPR, magnetic susceptibility) studies. The powdered electrical conductivities (${\sigma}_{rt}$) of the prepared compounds at room temperature were about~$10^{-7}S{\cdot}cm^{-1}$. The effective magnetic moments were lass than the spin-only value of one unpaired electron and no EPR signals from Pd metal ions were observed in any of the compounds, indicating that the Pd ions were diamagnetic and the magnetic moments arose from$(TTF)_n$ or $(TCNQ)_n$ moieties. The experimental evidences revealed that the charge transfer had occurred form $(TTF)_n$ moiety to the central Pd metal ion in 1a, 1b and 1c. Thus the TTF donors were ions in 2a and 2b were diamagnetic Pd(II) oxidation state. In contrast, the Pd metal ion was oxidized to Pd(IV) state in 2c as a result of an addition of $TCNQ^-$anion to $Pd(hfacac)_2$ in methanol. The oxidation states of the Pd metal ions were confirmed using the x-ray photoelectron spectroscopy.

• Bulletin of the Korean Chemical Society
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• 제30권5호
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• pp.1157-1163
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• 2009

Complexes of Pd(btnbmtp)$Cl_2$ and Pt(btnbmptp)$Cl_2$ (btnbmtp = 2,5-bis(thiophen)-1-nonyl-3,4-bis(methylthio)- pyrrole) were prepared and their crystal structures were determined at room temperature. In the structures, the two thiophene moieties lie in cis form with an average dihedral angle of $55.26^{\circ}$ to the pyrrole frame. The luminescence properties of the free ligand and the complexes were investigated in solution and solid states. The luminescence of the compounds were not favored by substituting thiophene moieties to the pyrrole frame, compared to the unsubstituted nbmptp (nbmptp = 1-nonyl-3,4-bis(methylthio)pyrrole). In particular, thiophene substitution quenched the emission from the complexes dissolved in ,$CH_2Cl_2$ and reduced the charge transfer transitions from S atoms of the thio moieties to Pt in crystalline state, which was very characteristic of Pt(nbmptp)$Cl_2$.

• Transactions on Electrical and Electronic Materials
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• 제12권4호
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• pp.164-168
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• 2011

Nanocrystalline cadmium sulphide (CdS) thin films were prepared using chemical bath deposition (CBD), and the structural, optical and photoconductive properties were investigated. The crystal structure of CdS thin film was studied by X-ray diffraction. The crystallite size, dislocation density and lattice constant of CBD CdS thin films were investigated. The dislocation density of CdS thin films initially decreases with increasing film thickness, and it is nearly constant over the thickness of 2,500 ${\AA}$. The dislocation density decreases with increasing the crystallite size. The Urbach energies of CdS thin films are obtained by fitting the optical absorption coefficient. The optical band gap of CdS thin films increases and finally saturates with increasing the lattice constant. The Urbach energy and optical band gap of the 2,900 A-thick CdS thin film prepared for 60 minutes are 0.24 eV and 2.83 eV, respectively. The activation energies of the 2,900 ${\AA}$-thick CdS thin film at low and high temperature regions were 14 meV and 31 meV, respectively. It is considered that these activation energies correspond to donor levels associated with shallow traps or surface states of CdS thin film. Also, the value of ${\gamma}$ was obtained from the light transfer characteristic of CdS thin film. The value of ${\gamma}$ for the 2,900 A-thick CdS thin film was 1 at 10 V, and it saturates with increasing the applied voltage.

• 대한화학회지
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• 제40권7호
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• pp.483-491
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• 1996

Cyclopentadiene과 exo-cyclic 이중결합을 가진 5각고리 화합물간의 Diels-Alder반응을 PM3 방법을 이용하여 연구하였다. Dienophile의 종류가 바뀌어도 전이상태의 구조는 커다란 변화를 나타내지 않았다. 반면에 dienophile의 exocyclic C(=O)-R 결합의 회w전에 의하여 나타나는 두 conformer들은 서로 다른 생성물을 얻을 수 있었으며, 이들의 반응성을 FMO들의 energy gap을 이용하여 설명하였다. 반면에 dienophile의 접근방향에 따른 exo, endo경로의 선택성을 살펴보기 위하여 전이상태에서의 deformation enerhy와 활성와 에너지간의 상관관계를 살펴보았다. 반응의 최저 에너지 경로를 Curtin-Hammett principle을 사용하여 논의 하였다.

• Bulletin of the Korean Chemical Society
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• 제30권12호
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• pp.2962-2968
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• 2009

The photodissociation dynamics of 1,2-bromochloroethane ($C_2H_4BrCl$) was investigated near 234 nm. A two-dimensional photofragment ion-imaging technique coupled with a [2+1] resonance-enhanced multiphoton ionization scheme was utilized to obtain speed and angular distributions of the nascent Br($^2P_{3/2}$) and Br${\ast}($^2P_{1/2}$) atoms. The total translational energy distributions for the Br and Br${\ast}$ channels were well characterized by Gaussian functions with average translational energies of 100 and 84 kJ/mol, respectively. The recoil anisotropies for the Br and Br${\ast}$ channels were measured to be ${\beta}$ = 0.49 ${\pm}$ 0.05 for Br and 1.55 ${\pm}$ 0.05 for Br${\ast}$. The relative quantum yield for Br${\ast}$ was found to be ${\Phi}_{Br{\ast}}$ = 0.33 ${\pm}$ 0.03. The probability of nonadiabatic transition between A' states was estimated to be 0.46. The relevant nonadiabatic dynamics is discussed in terms of interaction between potential energy surfaces in Cs symmetry.

• Bulletin of the Korean Chemical Society
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• 제28권11호
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• pp.1958-1962
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• 2007

The title complex, Ir(H)(CO)(PEt3)2(η 2-C60) (2), has been prepared by the reaction of excess C60 (4 equiv) with a tetrairidium complex Ir4(CO)8(PEt3)4 (1) in refluxing chlorobenzene in 40% yield as green crystals. Compound 2 has been characterized by cyclic voltammetry (CV), spectroscopic methods (mass, IR, 1H and 31P NMR), and a single crystal X-ray diffraction study. The molecular structure reveals that the iridium atom of 2 is coordinated by two axial ligands of a hydrogen atom and a carbonyl group, and three equatorial ligands of two phosphorus atoms and an η 2-C60 moiety. The CV study exhibits three reversible one-electron redox waves for the successive reductions of 2, together with additional four redox waves due to free C60 reductions, which was formed by decomposition of 2 in the reduced states. The three reversible redox waves of 2 are shifted to more negative potentials by ca. 270 mV compared to free C60, reflecting both metal-to-C60 π-back-donation and the electron-donating nature of the two phosphorus ligands.

• 대한치과보철학회지
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• 제18권1호
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• pp.49-57
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• 1980

The adhesive mechanisms on the metal-ceramic restorations have been reported to be mechanical interlocking, chemical bonding, compressive force, and Van der Waal's force, etc. Of these, the mechanical interlocking and chemical bonding forces are thought to affect the adhesive force between Ni-Cr alloy and porcelain. This study investigates the adhesion of Ni-Cr alloy to porcelain according to surface treatment. For this purpose, the following experiments were made; The compositions of Ni-Cr alloy as cast by emission spectrograph, and the oxides produced on Ni-Cr alloy during degassing at $1850^{\circ}F$ for 30 minutes in air and in vacuum were analyzed by X-ray diffractograph. The metal phases of Ni-Cr alloy were observed according to porcelain-baking cyclic heat treatment by photo microscope and the distribution and the shift of elements of Ni-Cr alloy and porcelain and the failure phases between Ni-Cr alloy and porcelain by scanning electron microscope. The adhesive force between Ni-Cr alloy and porcelain was measured according to surface treatment with oxidization and roughening by Instron Universal Testing Machine. Results were as follows; 1. The metal phases of Ni-Cr alloy as cast and degassing state showed the enlarged and fused core, but when subjected to porcelain-baking cyclic heat treatment, showed a dendrite growing. 2. The kinds of metal oxides produced on Ni-Cr alloy during degassing were found to be NiO and $Cr_2O_3$. 3. The distribution of elements at the interface of Ni-Cr alloy and porcelain in degassing state showed demarcation line, but in roughening state, showed mechanical interlocking phase. 4. The shift of elements at the interface occurred in both states, but the shift amount was found to be larger in roughening than in degassing. 5. The adhesive force between Ni-Cr alloy and porcelain was found to be $3.45{\pm}0.93kg/mm^2$, in degassing and $3.82{\pm}0.99kg/mm^2$, in roughening. 6. The failure phase between Ni-Cr alloy and porcelain showed the mixed type failure.

• 대한화학회지
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• 제28권5호
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• pp.271-278
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• 1984

염기성 용액에서 기계적으로 연마한 고순도 철의 전위를 환원 전위로부터 부동화 전위로 급격히 변화시켜서 부동화 막이 전극표면에 형성되게 하면서 철의 반사율 변화와 타원편광반사법(Ellipsometry) 측정을 하였다. 철 표면이 부동화 될때 일어나는 반사광의 편광 파라메터(${\Delta},\;{\psi}$)와 반사율(R) 변화를 자동화된 타원편광반사계로 기록하였고, 이로부터 철을 부동화 상태에 들어가게 하는 표면막의 두께(${\tau}$)와 광학상수(n, k)들의 변화하는 값을 계산할 수 있었다. 광학상수 값들로 나타나는 막의 성질이 시간에 따라 급격한 전이를 하는 것은 관찰되지 않았으며, 비교적 짧은 시간(수초)내에 정상 상태 값에 접근하였다. 효과적으로 부동화를 일으키는 막의 두께는 $14\;{\sim}\;23{\AA}$의 범위에 있었다. 형성된 부동화 막은 용액의 pH가 큰 경우에는 얇고 치밀한 구조를 가진 것으로 보이며, pH가 작은 경우에는 두께는 두껍지만 pH가 큰 경우보다 덜 치밀한 부동화 막이 형성되는 것으로 보였다. 이들 부동화 막은 약간의 흡광성을 가지는 것으로 나타났다.

• 대한화학회지
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• 제47권1호
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• pp.67-71
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• 2003

7차 교육과정에 따라 개발된 7학년 과학교과서 물질 영역의 탐구활동을 분석하여 교과서의 개발과 학습에 대한 교육적 시사점을 찾고자 하였다. 교과서의 탐구활동을 탐구유형, 탐구과정, 탐구상황 등의 3개의 영역으로 나누어 분석하였다. 6개 출판사에서 발간된 과학교과서의 ‘물질의 세 가지 상태', ‘분자운동', ‘상태변화와 에너지'를 분석 대상으로 하였다. 7학년 물질 영역의 탐구 활동 분석 결과를 종합하였을 때, 탐구 유형이나 탐구 과정 요소 및 탐구 상황의 편중성이 두드러졌으며, 이러한 부분을 보완할 수 있는 탐구 활동으로 학생들을 지도하여야 할 것이다. 또한, 과학과의 교육 목표에 부합되는 교과서 개발을 위해 탐구 활동을 검토하고 교과서 검정 기준에 탐구 활동의 평가틀을 제공하여야 할 것이다.

• 대한화학회지
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• 제40권6호
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• pp.394-400
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• 1996

결합성 사슬이합체를 형성할 수 있는 올리고펩티드-$(HPPHPPP)_n$-(H: 소수성 아미노산, P: 친수성 아미노산)는 온도, 수소이온 농도, 이온세기, 변성시약 등에 의해 구조적인 변화가 가능하다. 본 연구에서는 변성시약과 온도에 의한 올리고펩티드의 전이 현상을 이론적으로 고찰하였다. 사슬이합체로는 올리고펩티드20R, 변성시약으로는 구아니듐-염산을 사용하였다(20R에는 사슬 내의 정전기적 반발력이 10개가 존재하고, 사슬사이의 정전기적 반발력이 10개가 존재한다). 변성 시약에 의한 올리고펩티드의 나선에서 코일로의 전이는 급격한 것으로 보아, 변성이 일어나는 전이상태에서 올리고펩티드들은 완전한 나선구조와 무질서한 코일구조로만 되어있다. 반면에 온도에 의한 전이는 변성시약에 의한 전이보다 완만하게 일어난다. 낮은 온도에서 긴 나선 구조를 가지는 올리고펩티드가 짧은 나선 구조를 가지는 것보다 다량으로 존재한다. 온도가 증가할수록 부분적으로 변성된 분자들의 몰분율이 증가하여, 전이가 일어나는 온도에서 부분적으로 변성된 올리고펩티드가 널리 분포되어 있다.