The ortho-benzyne cation is not planar. Issue 6 (19th January 2018)

• Record Type: Journal Article
• Authors: Kaiser, D.; Reusch, E.; Hemberger, P.; Bodi, A.; Welz, E.; Engels, B.; Fischer, I.
• Is Part Of: Physical chemistry chemical physics. Volume 20:Issue 6(2018)
• Page Start: 3988
• Page End: 3996
• Publication Date: 2018-01-19
• Subjects: Chemistry, Physical and theoretical -- Periodicals; 541.3
• DOI: 10.1039/c7cp08055g
• Languages: English
• ISSNs: 1463-9076

Abstract

Abstract : Mass-selected threshold photoelectron spectroscopy with synchrotron radiation and high-level quantum chemical computations revealed that the ground state of the ortho -benzyne cation exhibits a twisted geometry and that the ionisation energies have to be revised. Abstract : A recent review on the photoionisation of the C6 H4 isomer ortho -benzyne suggests that bands reported in earlier photoelectron spectra might be due to side products or contaminations, while computations raise doubts, whether the cation has a planar geometry. We therefore reinvestigate the photoionisation of ortho -benzyne, generated by pyrolysis from benzocyclobutenedione, by photoion mass-selected threshold photoelectron (ms-TPE) spectroscopy using synchrotron radiation. The experiments are accompanied by a theoretical study that investigates the structure of the ortho -benzyne cation systematically as a function of the computational method, up to CASPT2(11, 14) ab initio computations. Our study leads to a re-evaluation of the ionisation energy of ortho -benzyne. It reveals that the ortho -benzyne cation has indeed a twisted C 2 geometry rather than a C 2v structure. A vertical ionisation energy IEvert of 9.77 eV and an adiabatic ionisation energy of IEad = 9.56 eV are computed for ortho -benzyne. A Franck–Condon simulation of the photoelectron spectrum based on the CASPT2 results and including three electronic states of the cation is in agreement with the experiment and yields IEad = 9.51 eV (+50 meV/−100 meV). Since this value is in contrast with previous work, the ionisation energy has to be revised based on our study. Computational methods based on density functional theory give a reasonable description of the cationic ground state, but fail for the corresponding excited electronic states that are indispensible for a proper assignment of the photoelectron spectrum.