Electron delocalization inAuNXM(X=Sc,Ti, Cr, Fe) clusters: A density functional theory and photofragmentation study

2004 ◽  
Vol 69 (8) ◽  
Author(s):  
Ewald Janssens ◽  
Hiromasa Tanaka ◽  
Sven Neukermans ◽  
Roger E. Silverans ◽  
Peter Lievens
2015 ◽  
Vol 93 (6) ◽  
pp. 673-684 ◽  
Author(s):  
Elahe Jalali ◽  
Davood Nori-Shargh

The origin of the symmetry breaking in the axial symmetrical configurations of enolic propanedial (1), propanedithial (2), and propanediselenal (3) have been investigated by means of time-dependence density functional theory and natural bond orbital interpretations. The results obtained at the quantum chemistry composite (G2MP2, CBS-QB3), ab initio molecular orbital (MP2/6-311++G**), and hybrid density functional theory (B3LYP/6-311++G**) levels of theory showed that the hydrogen-centered synchronous axial symmetrical (C2v) configurations of compounds 1–3 possessing the maximum π-electron delocalization within the M1=C2–C3=C4–M5–H6 keto-enol groups are less stable than their corresponding plane symmetrical (Cs) forms. Importantly, the symmetry breaking in the C2v configurations of the enol forms of compounds 1–3 to their corresponding plane symmetrical Cs configurations is due to the pseudo Jahn–Teller effect (PJTE) by mixing the ground A1 and excited B2 electronic states resulting in a PJT (A1 + B2) ⊗ b2 problem. We may expect that by the decrease of the energy gaps between reference states in the C2v forms that are involved in the PJTE decrease from compound 1 to compound 3, the PJT stabilization energy (PJTSE) may increase but the results obtained showed that the corresponding PJTSEs decrease. This fact can be justified by the increase of the electron delocalizations from the nonbonding orbitals of the C=M moieties to the antibonding orbitals of the H–M bonds, which leads to an increase of the π-electron delocalization within the M1=C2–C3=C4–M5–H6 keto-enol groups. In confrontation between the impacts of the resonance-assisted hydrogen bond and PJTE in the structural and configurational properties of compounds 1–3, PJTE has an overwhelming contribution and causes the symmetry breaking of the C2v configurations to their corresponding Cs forms. The correlations between the structural parameters, synchronicity indices, natural charges, PJTSEs, electron delocalizations, and the hardness of compounds 1–3 have been investigated.


2014 ◽  
Vol 70 (10) ◽  
pp. 987-991 ◽  
Author(s):  
Katarzyna Gajda ◽  
Bartosz Zarychta ◽  
Katarzyna Kopka ◽  
Zdzisław Daszkiewicz ◽  
Krzysztof Ejsmont

The crystal structure of 9H-carbazole, C12H9N, (I), has been redetermined at low temperature for use as a reference structure in a comparative study with the structures of 1-nitro-9H-carbazole, C12H8N2O2, (II), and 9-nitrocarbazole, C12H8N2O2, (III). The molecule of (I) has crystallographically imposed mirror symmetry (Z′ = 0.5). All three solid-state structures are slightly nonplanar, the dihedral angles between the planes of the arene and pyrrole rings ranging from 0.40 (7)° in (III) to 1.82 (18)° in (II). Nevertheless, a density functional theory (DFT) study predicts completely planar conformations for the isolated molecules. To estimate the influence of nitro-group substitution on aromaticity, the HOMA (harmonic oscillator model of aromaticity) descriptor of π-electron delocalization has been calculated in each case. The HOMA indices for the isolated and solid-state molecules are relatively consistent and decrease in value for aromatic rings that are substituted with a π-electron-withdrawing nitro group. Substitution of the arene ring influences the π-electron delocalization in the ring only weakly, showing strong resistance to a perturbation of its geometry, contrary to what is observed for nitro substitution of the five-membered heterocyclic pyrrole ring. In (II), the molecules are arranged in near-planar dimers connected to each other by strong N—H...O hydrogen bonds that stack parallel to the crystallographicbaxis. A similar stacking arrangement is observed in (III), although here the stacked structure is formed by stand-alone molecules.


2019 ◽  
Vol 16 (7) ◽  
pp. 592-599
Author(s):  
Farrokh Roya Nikmaram ◽  
Khadijeh Kalateh

Corannulene (C20H10) and its fluorinated derivatives, C20H10-xFx (x=1-10), are investigated at the B3LYP/6-31G level of density functional theory. The degree of electron delocalization is evaluated using Nucleus Independent Chemical Shift (NICS) method, Electric Field Gradient (EFG) method and factor of Ellipticity (ε). In this study, the benzene is the scale of comparison as a more aromatic structure. The aromaticity has been evaluated at three points of structures; center of five-member ring (5-MR), center of fluorine-substituted ring (6-MR), and center of other six-member rings. This comparison shows that substitution of fluorine for four and five hydrogen atoms in the Corannulene structure, C20H10-xFx (x=4, 5), results in more aromaticity compared to the other substitutions, and C20H10 and C20H10-xFx (x=1, 3) are more antiaromatic. It seems that the EFG method is more reliable for forecasting the aromaticity of structures, than NICS method. The factor of Ellipticity and bond lengths resulted from Atom in Molecule (AIM) analysis support the EFG method.


2019 ◽  
Vol 21 (44) ◽  
pp. 24478-24488 ◽  
Author(s):  
Martin Gleditzsch ◽  
Marc Jäger ◽  
Lukáš F. Pašteka ◽  
Armin Shayeghi ◽  
Rolf Schäfer

In depth analysis of doping effects on the geometric and electronic structure of tin clusters via electric beam deflection, numerical trajectory simulations and density functional theory.


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