• Title/Summary/Keyword: bond valence method

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Dielectric Properties of (Ba0.7Sr0.3-3x/2Lax)(Ti0.9Zr0.1)O3 Ceramics with La3+ Substitution for Sr2+-Site ((Ba0.7Sr0.3-3x/2Lax)(Ti0.9Zr0.1)O3 세라믹의 Sr2+-자리에 대한 La3+ 치환에 따른 유전 특성)

  • Si Hyun Kim;Ju Hye Kim;Eung Soo Kim
    • Korean Journal of Materials Research
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    • v.33 no.11
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    • pp.465-474
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    • 2023
  • The effects of La3+ substitution for Sr2+-site on the crystal structure and the dielectric properties of (Ba0.7Sr0.3-3x/2Lax) (Ti0.9Zr0.1)O3 (BSLTZ) (0.005 ≤ x ≤ 0.02) ceramics were investigated. The structural characteristics of the BSLTZ ceramics were quantitatively evaluated using the Rietveld refinement method from X-ray diffraction (XRD) data. For the specimens sintered at 1,550 ℃ for 6 h, a single phase with a perovskite structure and homogeneous microstructure were observed for the entire range of compositions. With increasing La3+ substitution (x), the unit cell volume decreased because the ionic size of La3+ (1.36 Å) ions is smaller than that of Sr2+ (1.44 Å) ions. With increasing La3+ substitution (x), the tetragonal phase fraction increased due to the A-site cation size mismatch effect. Dielectric constant (εr) increased with the La3+ substitution (x) due to the increase in tetragonality (c/a) and the average B-site bond valence of the ABO3 perovskite. The BSLTZ ceramics showed a higher dielectric loss due to the smaller grain size than that of (Ba0.7Sr0.3)(Ti0.9Zr0.1)O3 ceramics. BSLTZ (x = 0.02) ceramics met the X7R specification proposed by the Electronic Industries Association (EIA).

The Structure and Energy of D-Sorbitol from an Empirical force-Field (Empirical Force-Field 방법에 의한 D-Sorbitol 의 구조와 에너지에 관한 연구)

  • Park Young Ja
    • Journal of the Korean Chemical Society
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    • v.29 no.2
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    • pp.104-110
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    • 1985
  • Empirical force-field method has been applied to D-sorbitol, the crystal structure of which has been studied by the single crystal X-ray and neutron diffraction analyses. The calculated C-C bond lengths agree with those observed within 0.009${\AA}$. The C-O bond lengths show a larger deviation of 0. 023${\AA}$. The calculated C-C-C and C-C-O valence angles agree with those observed within $2.3^{\circ}$ and $1.9^{\circ}$respectively. Because torsion angles are influenced by packing forces, they show considerably flarger r. m. s. deviations. Calculations of the conformational energies of the model compound at selected C(1)-C(2)-C(3)-C(4) torsion angles made with the program MMI, produced result that the prediction of the observed preferred conformation of the carbon chain appeares to be less satisfactory.

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The Chemical Bond of Cu Atom in Layer and Chain for Y123 and Y124 Superconductors (Y123 초전도체 및 Y124 초전도체에서 층과 사슬에 존재하는 구리 원자의 화학결합)

  • Man Shick Son;U-Hyon Paek;Lee Kee-Hag
    • Journal of the Korean Chemical Society
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    • v.36 no.4
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    • pp.477-484
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    • 1992
  • Using semiempirical molecular orbital method, ASED-MO of extended Huckel Theory, we were investigated chemical bonds and electronic properties of Cu atom in a chain and a layer for Y123 and Y124 superconductors from VEP (valence electron population), DOS (density of state), and COOP (crystal orbital overlap population). In order to investigate environmental effects of Cu atom for Y123 and Y124 superconductors, we introduced charged cluster models with point charge and without point charge into our calculations. As a result of ASED-MO calculations, the Cu atom in the layer acts as electron acceptor and the Cu atom in the chain acts as electron donor for Y123 and Y124 superconductors. The oxidation state of Cu atom for Y123 and Y124 superconductors without point charge is higher in the chain than in the layer. The oxidation state of Cu atom in the layer for Y123 superconductor is higher than that in the layer for Y124 superconductor. The Cu atom in the layer and the chain for Y123 superconductor does not largely affect on the environmental effect. However, the Cu atom in the layer and the chain for Y124 superconductor does largely affect on it. Also, electron population and chemical bonding of Cu1-O4, Cu2-O4, and Cu1-Cu2 for Y123 superconductor are far different from Y124 superconductor.

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The Analytic Gradient with a Reduced Molecular Orbital Space for the Equation-of-Motion Coupled-Cluster Theory: Systematic Study of the Magnitudes and Trends in Simple Molecules

  • Baek, Gyeong Gi;Jeon, Sang Il
    • Bulletin of the Korean Chemical Society
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    • v.21 no.7
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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.