9 research outputs found
Theoretical modeling of hydrogen bond infrared spectra in molecular crystals of 2-thiopheneacetic acid : Fermi resonance and Davydov coupling effects
A quantum theoretical approach, within the adiabatic approximation and taking into account a strong non-adiabatic correction via the resonant exchange between the fast mode excited states of the two moieties of the dimer. The intrinsic anharmonicity of the low-frequency mode through a Morse potential, direct and indirect damping, and a selection rule breaking mechanism for forbidden transitions, is applied to reproduce the υX-H IR line shape of cyclic dimers of moderately H-bonded species in the crystalline phase. The results are used to gain an insight into the experimental spectral line shapes obtained by the transmission method. This approach fits satisfactorily the experimental line shape of 2-thiopheneacetic acid and predicts their evolution with isotopic substitution. Numerical calculations show that mixing of all these effects allows one to reproduce the main features of the experimental IR line shapes
Temperature and H/D Isotopic Effects in the IR Spectra of the Hydrogen Bond in Solid-State 2-Furanacetic Acid and 2-Furanacrylic Acid
Strong vibronic coupling effects in polarized IR spectra of the hydrogen bond in N-methylthioacetamide crystals
Polarized IR Spectra of the Hydrogen Bond in 2-Thiopheneacetic Acid and 2-Thiopheneacrylic Acid Crystals: H/D Isotopic and Temperature Effects
Davydov coupling as a factor influencing the H-bond IR signature: Computational study of the IR spectra of 3-thiopheneacrylic acid crystal
A unified quantum model susceptible to elucidate the dissimilarity of IR spectral density of dicarboxylic acid crystals: Phthalic and terephthalic acid crystals cases
Intermolecular Interactions in the Solid State of Ionic Secondary Mannich Bases
Two new secondary Mannich bases, 4-bromo-2-[(aminopropyl)methyl]-phenol
(<b>1</b>) and 4-nitro-2-[(aminopropyl)methyl]-phenol (<b>2</b>), were synthesized. Crystal structures were determined at
liquid nitrogen temperature. It was found that in both compounds the
proton transfer forms exist in the solid state. In the case of <b>1</b>, this was unexpected, because of the weak acidity of <i>p</i>-bromophenol being the parent component of this Mannich
base. The reason for that was found to be the formation of the O<sup>–</sup>···H–N<sup>+</sup> hydrogen bonded
tetramer in the solid state. Two cyclic aggregates R<sub>4</sub><sup>2</sup>(8) and R<sub>2</sub><sup>2</sup>(12) describe the pattern
of hydrogen bonded interactions in the crystals of both compounds.
Additionally, C–H···π interactions stabilize
the crystal structures. The hydrogen bonds in <b>1</b> are slightly
stronger (N···O distances 2.708 and 2.733 Å) than
in <b>2</b> (2.721 and 2.765 Å, respectively) despite the
fact that <i>p</i>-nitrophenol participating in <b>2</b> is a stronger acid. The influence of permittivity of surroundings
and the hydrogen bonding pattern on the properties of intermolecular
hydrogen bonds are discussed on the basis of B3LYP and MP2 calculations
with basis sets 6-31+G(d,p) and 6-31++G(2d,2p). The coupling between
hydrogen bonds in crystals was studied with the application of the
IR spectra of isotopically diluted species. It was found that such
a coupling is stronger for <b>2</b>, forming weaker hydrogen
bonds. Both the theory of IR spectra and quantum chemical calculations
demonstrate that the source of the observed behavior is electronic
participation in vibronic absorption
Intermolecular Interactions in the Solid State of Ionic Secondary Mannich Bases
Two new secondary Mannich bases, 4-bromo-2-[(aminopropyl)methyl]-phenol
(<b>1</b>) and 4-nitro-2-[(aminopropyl)methyl]-phenol (<b>2</b>), were synthesized. Crystal structures were determined at
liquid nitrogen temperature. It was found that in both compounds the
proton transfer forms exist in the solid state. In the case of <b>1</b>, this was unexpected, because of the weak acidity of <i>p</i>-bromophenol being the parent component of this Mannich
base. The reason for that was found to be the formation of the O<sup>–</sup>···H–N<sup>+</sup> hydrogen bonded
tetramer in the solid state. Two cyclic aggregates R<sub>4</sub><sup>2</sup>(8) and R<sub>2</sub><sup>2</sup>(12) describe the pattern
of hydrogen bonded interactions in the crystals of both compounds.
Additionally, C–H···π interactions stabilize
the crystal structures. The hydrogen bonds in <b>1</b> are slightly
stronger (N···O distances 2.708 and 2.733 Å) than
in <b>2</b> (2.721 and 2.765 Å, respectively) despite the
fact that <i>p</i>-nitrophenol participating in <b>2</b> is a stronger acid. The influence of permittivity of surroundings
and the hydrogen bonding pattern on the properties of intermolecular
hydrogen bonds are discussed on the basis of B3LYP and MP2 calculations
with basis sets 6-31+G(d,p) and 6-31++G(2d,2p). The coupling between
hydrogen bonds in crystals was studied with the application of the
IR spectra of isotopically diluted species. It was found that such
a coupling is stronger for <b>2</b>, forming weaker hydrogen
bonds. Both the theory of IR spectra and quantum chemical calculations
demonstrate that the source of the observed behavior is electronic
participation in vibronic absorption