AM1 study of photoelectronic spectra

Ionization energies of four model compounds with known conformations,i.e., benzo-1,3-dioxole, 2-methoxyphenol, benzo-1,3-dioxole-5-carbaldehyde (piperonal), and 4-hydroxy-3-methoxybenzaldehyde, have been calculated by theab initio AM1 method, using the formalized scheme of configuration interactions. It has been demonstrated that this method is adequate for the study of photoelectronic spectra of methoxy(hydroxy)-substituted benzenes. The ionization energies of 1,2-dimethoxybenzene, 3,4-dimethoxybenzaldehyde, and 4-hydroxy-3,5-dimethoxybenzaldehyde have been calculated for various orientations of theo-methoxy(hydroxy) groups. It has been revealed that three first ionization potentials corresponding to the states with vacancies on the -MO depend on the torsion angle. It has been established by comparison of calculated and experimental ionization potentials that in gas the compounds with adjacent methoxy groups have one O-Me bond parallel with the plane of the benzene ring, while another group is nearly perpendicular to this plane. Conformations of the heavy-atom framework are planar for gaseous molecules with adjacent methoxy and hydroxy groups.For Part 7, see Ref. 1.Translated fromIzyestiya Akademii Nauk. Seriya Khimicheskaya, No. 12, pp. 2365–2368, December, 1995.     

VUV spectra of the xenon fluorides

The absorption spectra of gaseous XeF₂, XeF₄, and XeF₆ have been accurately measured in the photon energy range from 6 to 35 eV with the use of the synchrotron radiation of DESY. The vibrational structure of several Rydberg transitions could be resolved. The spectra are interpreted and most of the structures could be assigned. From these data, information about the ionized species is obtained. The assignment of the first two IP's of XeF₄ is corrected.     

Magnetic susceptibility and x-ray photoelectronic spectra of CoO-MgO solid solutions

Conclusions Employing the magnetic susceptibility and x-ray photoelectronic spectroscopy methods it was shown that the high values of the Co(II) magnetic moments in a CoO-MgO solid solution in the air are due to the adsorption of oxygen in the paramagnetic form.Translated from Izvestiya Akademii Nauk SSSR, Seriya Khimicheskaya, No. 4, pp. 908–909, April, 1977.     

Theoretical and experimental infrared spectra of hydrated and dehydrated Nafion

The time‐dependent IR spectra during dehydration of fully hydrated Nafion show the reversible disappearance of the 1061 cm^?1 and 969 cm^?1 concurrent with the emergence of peaks at ～928 cm^?1 and ～1408 cm^?1. The first pair of group modes is associated with a dissociated exchange group (sulfonate) with a local C_3V symmetry. The C_3V group modes shift with state‐of‐hydration: The 969 cm^?1 peak completely vanishes and the 1061 cm^?1 is reduced to a small shoulder at 1070 cm^?1 at end of dehydration. The C_3V group modes are replaced by the pair of group modes of an associated exchange group (sulfonic acid) with C₁ local symmetry. The density functional theory normal mode analysis confirms that the sulfonic acid/sulfonate site plays a dominant role in the C₁ and C_3V group modes, respectively. This work clarifies the importance of assigning fluoropolymers peaks as group modes rather than traditional single functional group assignments as is often the case with the ～1061 cm^?1 and ～969 cm^?1 C_3V group modes. © 2013 Wiley Periodicals, Inc. J. Polym. Sci., Part B: Polym. Phys. 2013 , 51, 1329–1334     

Infrared spectra of 6-thioguanine tautomers. An experimental and theoretical approach

Both amino-thiol N9H and amino-thiol N7H tautomeric forms of 6-thioguanine have been identified in approximately equal abundance in infrared studies of these molecules isolated in the hydrophobic environment of an argon matrix at 12 K. The relative concentrations of the amino-thiol N9H and amino-thiol N7H ([SH, N9H]/[SH, N7H] = K(N9H-N7H) = 1.00 +/- 0.02) are estimated from the observed relative infrared absorbances. From these relative concentrations, the difference in the Gibbs free energy of these two tautomers (deltaG500(N9H-N7H) = -0.012 +/- 0.005 kJ mol(-1) have been estimated. The infrared and Raman spectra of 6-thioguanine in solid state are also discussed in terms of hydrogen bonding and stacking interactions in the crystal which are not considered in the calculation. In an effort to interpret the experimental results, ab initio calculation of the infrared spectrum has been made for the amino-thione N7H tautomer at 3-21G level. Comparison with experimental spectra is of some help in the assignment of the infrared and Raman spectra for 6-thioguanine in the solid state.     

Theoretical and experimental approach to spectrofluorometric extractive titrations

Spectrofluorometric extractive titration (SFET) is a sensitive method for determining trace amounts of certain metals. This technique combines titration, extraction and fluorometry and is more sensitive than any of these individual techniques. A theoretical treatment is derived and is compared favorably to an experimental procedure using Ga(III) and Al(III) as metals being titrated by 8-hydroxyquinoline(oxine). A sensitivity value for the experimental SFET is derived and calculated for the Ga(III) and Al(III)-oxine systems.     

Theoretical and experimental studies on the Raman spectra of electrosynthesized polynaphthalene

Polynaphthalene (Pnap) was electrosynthesized through the direct oxidation of naphthalene in boron trifluoride diethyl etherate and was characterized with IR and Raman spectroscopy, matrix‐assisted laser desorption/ionization time‐of‐flight mass spectroscopy, and thermogravimetric analysis. Raman spectra of oligonaphthalene were calculated with Gaussian 98 at the B3LYP/6‐31G* level. Combining the computational and experimental results, we assigned the Raman bands of pristine Pnap. The Raman bands related to the chain‐stretching vibrations of Pnap around 1600 cm^?1 shifted to higher wave numbers as the polymerization degree increased. This phenomenon was in contrast to that of other conducting polymers bearing simple aromatic rings, such as polythiophene and polyfuran. The reason was that the condensed ring of Pnap and the steric repulsion of the interring hydrogen atoms prevented the elongation of conjugation sequences with the polymer chain length. © 2004 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 43: 241–251, 2005     

Oxidation potential of thiophene oligomers: Theoretical and experimental approach

Intrinsic properties of conducting polymers, such as oxidation potential and band gap, are very important for designing new materials with improved properties. Computational chemistry offers suitable tools capable of predicting these quantities. This work presents electrochemical information about accurate oxidation potentials of oligothiophenes and polymer band gap. These are compared to theoretical predictions based on electronic structure calculations at Density Functional Theory levels, coupled with self‐consistent reaction field. All computational protocols gave a qualitative prediction of the experimental trend. © 2011 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys, 2011     

Theoretical study of electronic structure of rhodium mononitride and interpretation of experimental spectra

Potential energy curves of 22 electronic states of RhN have been calculated by the complete active space second‐order perturbation theory method. The X¹Σ₀⁺ is assigned as the ground state, and the first excited state a³Π₀+ is 978 cm^?1 higher. The ¹Δ(I) and B¹Σ⁺ states are located at 9521 and 13,046 cm^?1 above the ground state, respectively. The B¹Σ⁺ state should be the excited state located 12,300 cm^?1 above the ground state in the experimental study. Moreover, two excited states, C¹Π and b³Σ⁺, are found 14,963 and 15,082 cm^?1 above the X¹Σ⁺ state, respectively. The transition C¹Π₁–X¹Σ₀⁺ may contribute to the experimentally observed bands headed at 15,071 cm^?1. There are two excited states, D¹Δ and E¹Σ⁺, situate at 20,715 and 23,145 cm^?1 above the X¹Σ⁺ state. The visible bands near 20,000 cm^?1 could be generated by the electronic transitions D¹Δ₂–a³Π₁ and E¹Σ⁺₀–X¹Σ⁺₀ because of the spin–orbit coupling effect. © 2013 Wiley Periodicals, Inc.     

Theoretical formalism and experimental verification of line shapes of NMR intermolecular multiple-quantum coherence spectra

Although the theories and potential applications of intermolecular multiple-quantum coherences (iMQCs) have been under active investigations for over a decade, discussion of iMQC NMR signal formation was mainly confined in the time domain. In this paper, a full line-shape theory was developed to describe iMQC signals in the frequency domain. Relevant features of the line shape, such as peak height, linewidth, and phase, were investigated in detail. Predictions based on the theory agree well with experimental and simulated results. Since radiation-damping effects always couple with iMQCs in highly polarized liquid-state NMR systems, and strongly radiation-damped signals have many spectral characteristics similar to those of iMQCs, a detailed comparison was also made between them from different spectral aspects. With detailed comparison of peak height, linewidth, and phase, this work demonstrates that the iMQC and radiation-damping phenomena result from two completely different physical mechanisms despite that both present similar signal features and coexist in highly polarized liquid-state NMR systems.     

Theoretical and matrix-isolation experimental study of the infrared spectra of 5-azauracil and 6-azauracil

The infrared absorption spectra of 5-azauracil and 6-azauracil isolated in low-temperature Ar and N₂ matrices are reported. Within the limits of accuracy of spectroscopic measurements, both compounds appear to exist, in Ar and N₂ matrices, exclusively in dioxo tautomeric forms. An assignment of the observed infrared absorption bands is proposed based on the comparison of experimental frequencies and intensities with those calculated theoretically at ab initio Hartree-Fock level with 6-31G** basis set. Infrared spectra predicted at this level of theory reproduce the experimental spectra sufficiently accurately to enable a reliable assignment. Basis set dependency (6-31G**, 3–21G) of the theoretical result was also accounted for and it turned out that for accurate prediction of frequencies and intensities the use of basis set augmented with polarization functions is of crucial importance.     

Theoretical and experimental study of the structure and vibration spectra of 4,4′-carbonyl-di-morpholine

4,4′-Carbonyl-di-morpholine was synthesized and characterized by X-ray diffraction, the FTIR and NMR spectra. The extended MO calculations using density functional theory (DFT) and self-consistent field molecular orbital Hartree-Fock theory were carried out. The results of the calculations were compared with experimental data. The experimental and calculated results were supported each other. The performance of a hybrid B3LYP density functional was compared with the ab initio restricted Hartree-Fock method. With the basis sets of the 6-311G** quality, the DFT calculated bond lengths, dipole moments and harmonic vibrations were predicted in a very good agreement with available experimental data.     

Theoretical studies on the BC2N monolayers with promising photoelectronic characteristics and remarkable environmental stabilities

In this study, density functional theory calculations were performed to investigate the geometric structures, thermodynamic and mechanical stabilities, electronic, and optical properties of two BC₂N monolayers with honeycomb structure. The computational results demonstrate that the BC₂N monolayers have not only visible-light absorption, but also high reducing capacity of photo-induced electrons and excellent carrier mobility. Also, ab initio molecular dynamics simulations with considering the O₂ and H₂O molecule were carried out, which suggest that the crystal structures of both BC₂N monolayers can be well maintained in the moisture-laden air filled with O₂ molecules at 800 K. Accordingly, these BC₂N monolayers with promising photoelectronic characteristics and environmental stability could be utilized as metal-free visible-light-driven photocatalysts in high-temperature environment with moisture and oxygen, which is worthy of being further investigated in experimental and theoretical studies.     

Theoretical and experimental studies of enflurane. Infrared spectra in solution, in low-temperature argon matrix and blue shifts resulting from dimerization

Theoretical studies are performed on enflurane (CHFCl-CF(2)-O-CHF(2)) to investigate the conformational properties and vibrational spectra. Calculations are carried out at the B3LYP/6-31G(d) level along with a natural bond orbital (NBO) analysis. Experimental infrared spectra are investigated in carbon tetrachloride solution at room temperature and in argon matrix at 12 K. In agreement with previously reported data (Pfeiffer, A.; Mack, H.-G.; Oberhammer, H. J. Am. Chem. Soc. 1998, 120, 6384), it is shown that the four most stable conformers possess a trans configuration of the C-C-O-C skeleton and a gauche orientation of the CHF(2) group (with respect to the central C-O bond). These conformations are favored by electrostatic interaction between the H atom of the CHF(2) group and the F atoms of the central CF(2) group. Hyperconjugation effects from the O lone pairs to the antibonding orbitals of the neighboring C-H and C-F bonds also contribute to the stability of the four conformers. The vibrational frequencies, infrared intensities, and potential energy distributions are calculated at the same level of theory for the most stable conformers. On the basis of the theoretical results, these conformers are identified in an argon matrix. The influence of the concentration on the nu(CH) vibrations suggests the formations of higher aggregates in solution. Theoretical calculations are carried out on the enflurane dimer. The results show that the dimer is formed between two enflurane conformers having the largest stability. The dimer has an asymmetric cyclic structure, the two enflurane molecules being held together by two nonequivalent C-H...F hydrogen bonds, the C-H bond of the CHFCl group acting as a proton donor, and one of the F atoms of the CHF(2) groups acting as a proton acceptor. The theory predicts a contraction of 0.0014-0.0025 A of the two CH bonds involved in the interaction along with a blue shift of 30-38 cm(-1) of the corresponding nu(C-H) bands, in good agreement with the blue shifts of 35-39 cm(-1) observed in an argon matrix.