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91.
Electronic structure calculations have been performed for flat graphite sheets and periodically distorted sheets with different values of deformation angle and hydrogen adsorption. These characteristics do not all behave monotonically with increasing deformation angle. At small deformation angles, the electrons pass from the atoms of terraces to those of edges, while at larger angles the reverse pattern is observed. The position of the Fermi level also varies nonmonotonically. The binding energy of hydrogen depends significantly on the adsorption site, and the difference can be doubled. Based on the ata obtained, it was concluded that a priori statements derived from the “general concepts” on the difference in the physicochemical properties of, for example, terrace and edge atoms on high-index facets are unreliable.  相似文献   
92.
应用EHMO法研究了一系列含dppm双二苯基膦甲烷桥的双核过渡金属配合物[PdBr(dppm)]_2,M_2Cl_2(μ-CO)(dppm)_2(M=Pd,Rh),[RhCl(CO)(dppm)]_2,M_2-(μ-Cl)_2Cl_4(dppm)_2(M=Nb、Ta、Re、Ru)的电子结构。根据配合物的成键特征,对其金属-金属的相互作用进行了分析。计算结果可以作为解释这类配合物的某些物理化学性质的理论依据。  相似文献   
93.
用abinitioMO方法,在MP2(ful)/6311G水平下,全优化计算了叠氮化钠(NaN3)分子的线状和环状两种稳定构型及其转化过渡态的几何参数、电荷分布、分子总能量和振动频率,并研究了它们的热力学性质及转化速率常数和平衡常数.结果表明,线状比环状构型稍稳定(能量低6.04kJ/mol);两者相互转化的能垒分别为13.15kJ/mol(线型→环状)和7.11kJ/mol(环状→线型).热力学和动力学计算均表明:NaN3通常主要以线型结构存在(占85%以上),且随温度升高而增多(在1000K大于91%).  相似文献   
94.
应用INDO/S半经验量子化学方法,对簇合物离子Mo3S和Mo3S4Mn+(M=Fe、Ni,n=4;M=Cu,n=5)分别进行分子轨道计算。根据计算得到的簇离子中的原子表观电荷和成键指标,说明Fe、Ni、Cu+与Mo3S成键作用的相对强度依次是Fe-Mo>Ni-Mo>Cu+-Mo。比较了用含组态作用的INDO/S方法计算得到的电子跃迁能与实验得到的电子吸收光谱值,并讨论了吸收峰归属情况。对于M为Fe、Ni的簇离子Mo3S4M4+,最低能量的电子跃迁吸收峰起源于异金属间电荷转移跃迁(MM’CT);而Mo3S4Cu(5+)簇离子观察到的吸收峰主要是Mo3S芯的局域内电荷转移跃迁。根据理论计算结果,由Cu+离子到Mo3S的电荷转移跃迁谱线,大约在46000cm-1以上才能观察到吸收峰。从Mo3S4Fe4+次低能量吸收峰的实验值16600cm-1和理论值16500cm-1与Mo3S的最低能量吸收峰的实验值16600cm-1和理论值16900cm-1比较,表明无论从理论上或实验上都能证实簇离子Mo3S4Fe4+在能量为16600cm-1处的吸收峰是起因于Mo3S芯的局域内电荷转移跃迁。  相似文献   
95.
Single-phase samples of REAgMg (RE=La, Ce, Eu, Yb) and EuAuMg were prepared by reacting the elements in sealed tantalum tubes in a high-frequency furnace. LaAgMg and CeAgMg adopt the hexagonal ZrNiAl-type structure, while EuAgMg, YbAgMg, and EuAuMg crystallize with the orthorhombic TiNiSi type. Chemical bonding was exemplarily investigatedfor EuAgMg and EuAuMg on the basis of TB-LMTO-ASAcalculations. Magnetic susceptibility measurements indicatePauli paramagnetism for LaAgMg and YbAgMg with room-temperature susceptibilities of 2.4(1)×10−9 and 1.5(1)×10−9 m3/mol, respectively. CeAgMg remains paramagnetic down to 2 K. The experimental magnetic moment of 2.52(2) μB/Ce above 50 K is compatible with trivalent cerium. EuAgMg and EuAuMg are paramagnetic above 50 K with experimentalmagnetic moments of 7.99(5) μB/Eu for the silver and 7.80(5) μB/Eu for the gold compound, indicating divalent europium. Ferromagnetic ordering is detected at TC=22.0(3) K (EuAgMg) and TC=36.5(5) K (EuAuMg). At 4.2 K and 5 T the saturation magnetizations are 7.1(1) and 7.3(1) μB/Eu for EuAgMg and EuAuMg, respectively. According to the very small hysteresis, EuAgMg and EuAuMg may be classified as soft ferromagnets. All compounds are metallic conductors. For EuAgMg and EuAuMg freezing of spin-disorder scattering is observed below TC. At 78 K 151Eu Mössbauer spectra show isomer shifts of −9.00(4) and −8.72(8) mm/s for EuAgMg and EuAuMg, respectively. Full magnetic hyperfine field splitting is detected at 4.2 K with hyperfine fields of 17.4(1) and 18.3(2) T at the europium nuclei of EuAgMg and EuAuMg.  相似文献   
96.
The results of calculations for benzyl chlorides and benzyl bromides that contain substituents in the ring by different quantum-chemical methods are compared. The electron density on the benzyl carbon atom increases as the electron-withdrawing properties of substituents are enhanced due to the shift of the electron density from the benzyl halogen atom to the adjacent carbon atom. A topological analysis according to Bader confirmed the main reason for the change in the paramagnetic shielding of the benzyl13C nuclei. The results of calculations provide, for the first time, an explanation for the resonance upfield13C shift of this atom as the Hammett constant of a substituent increases in compounds of the series under consideration. Translated fromIzvestiya Akademii Nauk. Seriya Khimicheskaya, No. 12, pp. 2111–2119, December, 1997.  相似文献   
97.
LigandscontainingelectrochemicallyresponsivecentrearegoodsubjectsforthestUdyofintfamolecularandhost-guestillteraction.Forthisreason,tYemendousamoulltsofsuchligandsandtheircomplexeshavebeensynthesized.'-'AnobservationfromthestudiesofthesecomPlexesisthattheguestionhasapermrbationonthehostcelltre.2'7-9Forexample,itwasdocumelltedthatintroductionofCo(II)ionontoN-ferrocenylmethyl-l,4,7-triazacyclononane(fcmtacn)causesapositiveshiftintheredoxpotentialofferrocenylgroupfromthatofferrocenegroupinfree…  相似文献   
98.
The novel fluorinated distyrylarylene, 4,4'-bis(2,2-di(4-fluorophenyl)vinyl)biphenyl (DFPVBi), was synthesized and fully characterized. The structure was confirmed with IR, 1↑H NMR, 13↑C NMR, 19↑F NMR and MS analyses. Its electronic and photoluminescence properties were investigated by UV-Vis absorption, cyclic voltammetry and fluorescence spectroscopy. The energy levels of the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO) are --5.77 and --2.75 eV, respectively. The electroluminescence proper- ties of the organic light-emitting diode fabricated by DFPVBi were also studied. The device exhibits a pure blue emission peaked at 454 nm, which indicates a maximum luminance of 5872 cd/m ^2 at 14.2 V and a maximum current efficiency of 2.82 cd/A at 10V, respectively.  相似文献   
99.
The crystal and molecular structures of the following molecules have been determined: 1-acetyl-indoline, 1-acetyl-5-nitro-indoline, l-acetyl-5-nitro-7-bromo-indoline, 1-acetyl-5-bromo-7-nitroindoline, and l-acetyl-5-bromo-7-nitro-indol. Molecular orbital calculations are performed for these compounds and two related species.  相似文献   
100.
A quasirelativistic perturbative method of ab initio calculations on ground and excited molecular electronic states and transition properties within the relativistic effective core potential approximation is presented and discussed. The method is based on the construction of a state‐selective many‐electron effective Hamiltonian in the model space spanned by an appropriate set of Slater determinants by means of the second‐order many‐body multireference perturbation theory. The neglect of effective spin–orbit interactions outside of the model space allows the exploitation of relatively high nonrelativistic symmetry during the evaluation of perturbative corrections and therefore dramatic reduction of the cost of computations without any contraction of the model‐space functions. One‐electron transition properties are evaluated via the perturbative construction of spin‐free transition density matrices. Illustrative calculations on the X0+ ? A1, B0+, and (ii)1 transitions in the ICl molecule are reported. © 2002 Wiley Periodicals, Inc. Int J Quantum Chem, 2002  相似文献   
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