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The experimental intensity of 30 keV electron small angle scattering by a gaseous molecule is much different from the calculation using usual independent atom model. This is due to the rearrangement of electron distribution in a molecule by the formation of chemical bonds, and is called chemical bonding effect (CBE). The molecules studied are mainly hydrocarbons such as methane, acetylene, ethane, etc. and some non-hydrocarbons. The measurement was carried out on both elastic and total scattering and the effect was found for not only elastic but also inelastic scattering. The effect is relatively large for hydrogen rich molecules as H2O, NH3 and hydrocarbons, but is essentially related to the number of atoms contained in molecules. The origin of CBE will attribute mainly to the concentration of inner atomic electrons resulting from chemical bonding.  相似文献   

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Within the Born-Oppenheimer adiabatic perturbation theory, an equation was obtained for the intensity of fast electron scattering by polyatomic molecules. All of its parameters are explicitly defined by vibronic interaction in a molecule; due to this, quantum chemical calculations are fully applicable to electron diffraction studies of molecular geometries. Engels Anti-Aircraft Missile Higher Military School. Translated fromZhurmal Strukturnoi Khimii, Vol. 35, No. 2, pp. 40–45, March–April, 1994. Translated by L. Smolina  相似文献   

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4-Thiacyclohexanone has been shown to be most stable in the chair conformation. The bond lengths were found to be ra(CO) = 1.223(5) Å, ra(C-S) = 1.804(3) Å, ra(C-C)av = 1.527(3) Å, ra(C-H) = 1.116(6) Å. A simple molecular-mechanics calculation agreed with the electron-diffraction results.  相似文献   

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By means of gas phase electron diffraction it has been shown that the five-membered ring in 1,3-dimethyl-2-chloro-diazaboracyclopentane is essentially planar, while there seems to be a slight deviation from planarity about the N atoms. The most important bond lengths (ra) and bond angles are (standard deviations in parentheses): r(B-N) = 1.413(3) Å; r(C-N)av = 1.455(2) Å; r(B-Cl) = 1.770(4) Å; ∠NBN = 110.8(3)°; ∠B2N3C4 = 108.6(3)°; ∠N3C4C5 = 105.7(3)°.  相似文献   

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The molecular structure of gaseous 2-cyclopentene-1,4-dione has been studied by electron diffraction. The molecule is planar to within the experimental error. The results obtained for some of the more important parameters with estimated uncertainties of 2σ are r(C-H) = 1.093 Å (0.013), r(C0) = 1.208 Å (0.002), r(CC) = 1.341 Å (0.005), r(CH-CO) = 1.493 Å (0.005), r(CO-CH2) = 1.525 Å (0.005), ∠CC-C = 110.4° (0.3), ∠CH-CO = 124.9° (1.1), ∠CC-H. = 118.7° (5.8), ∠H-C-H = 113.2° (8.7) l(C-H) = 0.0853 A (0.0113), l(CO) = 0.0428 Å (0.0021), l(CC) = 0.0448 Å (0.0037) and l(C-C) = 0.0561 Å (0.0029). The structure is discussed in connection with the structures of related molecules.  相似文献   

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A scheme for the obtaining the electron density function W(Q s ) in a curvilinear vibrational coordinate system and scattering equation sM(s) is described in the framework of a vibrational model.Engels Anti-Aircraft Rocket Command Institute. Translated from Zhurnal Strukturnoi Khimii, Vol. 30, No. 6, pp. 33–37, November–December, 1989.  相似文献   

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We apply first-principles computational methods to study elastic scattering of low-energy electrons by 2-deoxyribose and 2-deoxyribose monophosphate, which are of interest as components of the DNA backbone, and to tetrahydrofuran (THF), which has been studied as a deoxyribose analog. To investigate the dependence of the scattering process on the molecular conformation, we examine Cs and C2 conformers of THF as well as the planar C(2v) geometry imposed in earlier calculations. There is little difference between the elastic cross sections determined at the nonplanar geometries, but there are noticeable differences between those results and the cross sections computed using the planar ring. By comparing results for tetrahydrofuran obtained with and without inclusion of polarization effects, we obtain energy shifts that are applied to the computed resonance positions for deoxyribose and deoxyribose monophosphate.  相似文献   

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Polar graphs for differential cross section (dcs) called spatial dcs maps are presented as graphical representation of the angular distribution of vibrationally inelastic electron scattering by polyatomic molecules. The objective of this paper is to show that an intuitive understanding of the principal features of these graphs can be obtained from a simple analysis of the normal modes of vibration of the target molecule and plane-wave functions representing the scattering electron. The procedure is illustrated on the H2 and CH4 molecules.  相似文献   

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