• Macromolecular Research
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• 제8권6호
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• pp.292-297
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• 2000

The theoretical synthesis of the isotactic and syndiotactic poly(methyl methacrylate) were carried out as a model for real polymerization reactions following the normal chain reaction processes by repeating the uniform localization of wave functions with inclusion of the interaction between the end group of the cluster and an attaching molecule by the elongation method, and then, the calculated value was compared with the usual PM$_3$ calculation. The results revealed that a reaction of cluster with monomer molecules has made it possible to calculate the electronic structure and total energy of polymer with nearly infinite length and a matrix of constant dimension. The isotactic poly(methyl methacrylate) is more stable than syndiotactic one. The same tendency have been found between the experimentally measured properties and a calculated total energy to explain the chain motion in isotatic and syndiotactic poly(methyl methacrylate).

• Bulletin of the Korean Chemical Society
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• 제33권12호
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• pp.4155-4160
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• 2012

We characterized the physisorption of p-iodo-phenyl octadecyl ether molecules (I-POE) onto superlattice regions of graphite surfaces using scanning tunneling microscopy (STM). The formation of self-organized I-POE monolayers does not affect the overall structures of moir$\acute{e}$ patterns and their modulation periods. However, the packing density of the I-POE monolayer and the orientations of lamella structures were sensitive to the underlying superlattice structure. Depending on the bias voltage, the STM images selectively showed moir$\acute{e}$ pattern, I-POE layer, or both. Reflecting the local density of states at a certain energy level, the STM images thereby revealed the relative energy level scale of the superlattice with respect to the molecular orbitals of I-POE.

• Bulletin of the Korean Chemical Society
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• 제34권2호
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• pp.453-459
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• 2013

In phtosynthetic light harvesting complexes, the electronic transition energies of chlorophylls are influenced by the Coulombic interaction with nearby molecules. Variation of the interactions caused by structural inhomogeneity in biological environment results in a distribution of disordered electronic transition energies of chlorophylls. In order to provide a practical guide to predict qualitative tendency of such distribution, we model four porphyrin derivatives including chlorophyll a molecule interacting with an external positive charge and calculate their transition energies using the time dependent density functional method. It is found that ${\pi}-{\pi}^*$ transition energies of the molecules are generally blue-shifted by the charge because this stabilizes occupied molecular orbitals to a greater extent than unoccupied ones. Furthermore, new transitions in the visible region emerge as a result of the red-shift in energy of an unoccupied Mg orbital and it is suggested that light-induced electron transfer may occur from the tetrapyrrole ring to the central magnesium when the molecules are interacting with a positive charge.

• EDISON SW 활용 경진대회 논문집
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• 제2회(2013년)
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• pp.77-88
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• 2013

The computational study on the fluoride ion binding with bis(bora)calix[4]arene has been performed using density functional theory and ONIOM model. The computed structure and fluorescent behavior of bis(bora)calix[4]arene was corresponded to experiment value. The binding energy for fluoride anion is computed to be 28.05kJ/mol in the chloroform solution. We also predicted that this sensing mechanism is only valid for fluoride ion in halogens. By analyzing molecular orbitals, binding with fluoride ion reduces energy differences between HOMO and LUMO, which leads to fluorescent sensing.

• Bulletin of the Korean Chemical Society
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• 제3권3호
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• pp.98-103
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• 1982

Extended Huckel calculations have been performed to obtain molecular orbital energies and the corresponding eigenvectors for $[M(III)O_3S_3]$ type complexes [M(111) = V(111), Cr(III), Mn(III), Fe(III) and Co(III)] adopting the valence basis set orbital $(nP_z)$ and the hybridized atomic orbital of ligands. The effects of the hybridized atomic orbital of ligands on the calculated dipole moments and 10 $D_q$ values are investigated. The calculated 10 $D_q$ values and dipole moments are close to the experimental values when the hybridized atomic orbital of ligands is used to obtain the eigenvector for $[M(III)O_3S_3]$ type complexes.

• Bulletin of the Korean Chemical Society
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• 제14권2호
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• pp.191-195
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• 1993

Molecular orbital calculations at the extended Huckel level have been carried out for an electron deficient cluster, $Tl_3(FeL_3)_2{(FeL_4)_3}^{-3}$, where L=CO or $H^-$. The LUMO, $2a_2$", is destabilized by the secondary interaction of the LUMO with $1a_2$" on $(FeL_3)_2$ fragment. This is one of six skeletal bonding orbitals which are associated with $Tl-FeL_3$ bonds. Overlap population analysis has been applied to account for two kinds of Tl-Fe bonds. Replacement of the terminal $C_{3v}$, $FeL_4$, by the $C_{2v}$, $FeL_4$ units in cluster results in slight energy stabilization of the cluster.

• 대한화학회지
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• 제26권5호
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• pp.265-273
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• 1982

두다른 방법을 사용하여 사면체 및 사각형[M(Ⅱ)$O_2S_2$] 형태 착물의 쌍극자모멘트에 대한 ${\pi}$결합의 영향을 고찰하였다. 그첫째 방법은 금속이온의 원자가 궤도함수와 리간드 궤도함수 사이의 혼성계수 CM이 ${\sigma}$ 및 ${\pi}$결합 분자궤도함수에 대하여 모두 같다는 가정에 기초를 둔 근사 분자궤도함수 법이며 다른 하나는 반경험적인 LCAO-MO법에 기초를 둔 계산이다. ${\sigma}$ 결합만이 형성되었다고 가정한다면 사면체 및 사각형 착물의 계산한 쌍극자 모멘트는 실험치 보다 작다. 계산한 쌍극자 모멘트에 ${\pi}$결합의 기여분을 모두 고려 해 준다면 사각형 및 사면체 $[M (II)O_2S_2]$형태 착물의 계산한 쌍극자모멘트는 실험치보다 크다. 그러나 ${\pi}$결합이 비편재 되었다고 가정한다면 사면체 [M(II)$O_2S_2$]형태 착물의 계산한 쌍극자 모멘트가 실험치 범위안에 들지만 사각형착물의 쌍극자 모멘트는 실험치에서 벗어난다. 이 결과는 [M(II)$O_2S_2$]]형태 착물이 비극성 용매의 용액에서 사면체 구조로 존재함을 암시하며 이 구조는 실험구조와 일치한다. 사면체 [M(II)$O_2S_2$] 형태착물의 계산한 쌍극자모멘트는 쌍극자모멘트에 ${\pi}$결합이 참여함을 지적한다.

• 대한화학회지
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• 제24권4호
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• pp.269-279
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• 1980

$t^2_2$ 전자배치를 가진 팔면체 및 일그러진 팔면체 $[V(III)A_3B_3]$형태 착물에 대한 자기모멘트를 계산하는 새로운 방법을 발전시켰다. [A 와 B = O, Cl, N, F 또는 Br]. 이 방법에 의하여 계산한 자기모멘트가 실험치와 비교적 잘 일치한다. 일그러진 팔면체 $[V(III)A_3B_3]$형태 착물의 계산한 자기모멘트는 tetragonal distortion의 크기가 증가함에 따라 감소한다. 자기모멘트에 대한 k (orbital reduction factor), $\xi'$ 및 온도의 영향을 또한 고찰하였다. 쌍극자모멘트 및 편극율에 대한 $^3T_1$ 분자궤도함수의 기여분을 계산하는 새로운 방법을 발전시켰다. 이 방법에 의하여 계산한 $^3T_1$ 분자궤도함수의 기여분은 합리적인 범위안에 들었다.

• Bulletin of the Korean Chemical Society
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• 제21권7호
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• pp.720-726
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• 2000

The analytic gradient method for the equation-of-motion coupled-cluster singles and doubles (EOM-CCSD) energy has been extended to employ a reduced molecular orbital (MO) space. Not only the innermost core MOs but also some of the outermost virtua l MOs can be dropped in the reduced MO space, and a substantial amount of computation time can be reduced without deteriorating the results. In order to study the magnitudes and trends of the effects of the dropped MOs, the geometries and vibrational properties of the ground and excited states of BF, CO, CN, N2, AlCl, SiS, P2, BCl, AIF, CS, SiO, PN and GeSe are calculated with different sizes of molecular orbital space. The 6-31 G* and the aug-cc-pVTZ basis sets are employed for all molecules except GeSc for which the 6-311 G* and the TZV+f basis sets are used. It is shown that the magnitudes of the drop-MO effects are about $0.005\AA$ in bond lengths and about 1% on harmonic frequencies and IR intensities provided that the dropped MOs correspond to (1s), (1s,2s,2p), an (1s,2s,2p,3s,3p) atomic orbitals of the first, the second, and the third row atoms, respectively. The geometries and vibrational properties of the first and the second excited states of HCN and HNC are calculated by using a drastically reduced virtual MO space as well as with the well defined frozen core MO space. The results suggest the possibility of using a very smalI MO space for qualitative study of valence excited states.

• Journal of Korean Vacuum Science & Technology
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• 제4권1호
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• pp.1-5
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• 2000

The C 1s photoelectron energy loss spectra of tris (8-hydroxy-quinoline) aluminum (Alq$_3$) and N,N'-diphenyl-N,N'-bis (3-methyl phenyl)-1,1'-bi-phenyl-4,4'-diamine (TPD) thin films have been investigated. Two major loss structures, namely the plasmon dominated loss lines and shake-up satellites, have been observed. The shake-up spectrum of the C 1s photoelectron line is directly related to the $\pi$-$\pi$$\^$*/ energy gap of the molecule which plays an important role in organic electroluminescent materials. The molecular orbitals of Alq$_3$ and TPD and their major components, quinolime and benzene, have been calculated with the AMI semi-empirical method. The amount of the plasma-dominated loss of Alq$_3$ and TPD, which has to do with the delocalization of electrons through the molecule, was about 24 eV, alike in both cases. The main peak of the C 1s shake-up spectrum of Alq$_3$ and TPD, however, was 5.2 eV and 6.8 eV respectively. It was found that the main shake-up peak reflects more the local $\pi$\longrightarrow$\pi$$\^$*/ transition of quinoline and benzene component rather than the excitation of the whole molecule of Alq$_3$ and TPD. The C 1s shake-up spectra, however, revealed some correlation with the optical energy gap of the organic eletroluminescent materials.