The strong inter-relationship between cyclohepta-1,3,5-triene (CHT) and norcaradiene (NCD) systems observed in some reactions has been extended to include the energy surfaces for some low-lying ionic states. Equilibrium structures for ionic states of CHT with A? symmetry were routinely found; the structures emerging with A?? symmetry were NCD ionic states. A detailed analysis of these surfaces as a function of the C to C distance showed that while minima occurred for both state symmetries, curve crossing occurs in C symmetry, which is avoided by distortion to C symmetry. The CHT -> NCD structural change is attributed to initial conrotatory closure of the singly occupied molecular orbital. A new synchrotron-based photoelectron spectrum (PES) for CHT up to 25 eV shows little vibrational structure. We have assigned the PES up to 17 eV using a variety of theoretical methods. The calculated lowest ionic state, XA?, is predicted to have a very low vibrational frequency of 87 cm, leading to a high density of vibrational states. The Franck-Condon envelopes calculated for the two lowest states are almost completely contained within the envelope of the lowest PES band. A comparison of the predicted PES of CHT and NCD showed much closer agreement of the PES with that of CHT. An analysis of the H and C nuclear magnetic resonance (NMR) spectra of CHT showed no evidence of NCD. The increased chemical shifts arising from the higher frequencies used here lead to significant changes in appearance when compared with earlier NMR spectra.

The ground and ionic states of cyclohepta-1,3,5-triene and their relationship to norcaradiene states: New 1H and 13C NMR spectra and analysis of a new experimental photoelectron spectrum by ab initio methods

Coreno Marcello;De Simone Monica;Grazioli Cesare;
2020

Abstract

The strong inter-relationship between cyclohepta-1,3,5-triene (CHT) and norcaradiene (NCD) systems observed in some reactions has been extended to include the energy surfaces for some low-lying ionic states. Equilibrium structures for ionic states of CHT with A? symmetry were routinely found; the structures emerging with A?? symmetry were NCD ionic states. A detailed analysis of these surfaces as a function of the C to C distance showed that while minima occurred for both state symmetries, curve crossing occurs in C symmetry, which is avoided by distortion to C symmetry. The CHT -> NCD structural change is attributed to initial conrotatory closure of the singly occupied molecular orbital. A new synchrotron-based photoelectron spectrum (PES) for CHT up to 25 eV shows little vibrational structure. We have assigned the PES up to 17 eV using a variety of theoretical methods. The calculated lowest ionic state, XA?, is predicted to have a very low vibrational frequency of 87 cm, leading to a high density of vibrational states. The Franck-Condon envelopes calculated for the two lowest states are almost completely contained within the envelope of the lowest PES band. A comparison of the predicted PES of CHT and NCD showed much closer agreement of the PES with that of CHT. An analysis of the H and C nuclear magnetic resonance (NMR) spectra of CHT showed no evidence of NCD. The increased chemical shifts arising from the higher frequencies used here lead to significant changes in appearance when compared with earlier NMR spectra.
2020
Istituto Officina dei Materiali - IOM -
Istituto di Struttura della Materia - ISM - Sede Secondaria Trieste
Photoelectron spectroscopy
Singly occupied molecular orbitals
Chemical analysis
Molecular orbitals
Photoelectrons
Photons
Photoelectron spectrum
Equilibrium structures
Theoretical methods
Vibrational structures
Nuclear magnetic resonance spectroscopy
Nuclear magnetic resonance (NMR)
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/375843
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