John M. Dyke

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Name:
Organization: University of Southampton , England
Department: School of Chemistry
Title: Emeritus Professor(PhD)
Co-reporter:Luca Schio, Michele Alagia, Antonio A. Dias, Stefano Falcinelli, Vitali Zhaunerchyk, Edmond P. F. Lee, Daniel K. W. Mok, John M. Dyke, and Stefano Stranges
The Journal of Physical Chemistry A 2016 Volume 120(Issue 27) pp:5220-5229
Publication Date(Web):April 5, 2016
DOI:10.1021/acs.jpca.6b01039
In this work, hydrogen peroxide has been studied with threshold photoelectron (TPE) spectroscopy and photoelectron (PE) spectroscopy. The TPE spectrum has been recorded in the 10.0–21.0 eV ionization energy region, and the PE spectrum has been recorded at 21.22 eV photon energy. Five bands have been observed which have been assigned on the basis of UCCSD(T)-F12/VQZ-F12 and IP-EOM CCSD calculations. Vibrational structure has only been resolved in the TPE spectrum of the first band, associated with the X̃2Bg H2O2+ ← X̃1A H2O2 ionization, on its low energy side. This structure is assigned with the help of harmonic Franck–Condon factor calculations that use the UCCSD(T)-F12a/VQZ-F12 computed adiabatic ionization energy (AIE), and UCCSD(T)-F12a/VQZ-F12 computed equilibrium geometric parameters and harmonic vibrational frequencies for the H2O2 X̃1A state and the H2O2+ X̃2Bg state. These calculations show that the main vibrational structure on the leading edge of the first TPE band is in the O–O stretching mode (ω3) and the HOOH deformation mode (ω4), and comparison of the simulated spectrum to the experimental spectrum gives the first AIE of H2O2 as (10.685 ± 0.005) eV and ω4 = (850 ± 30) and ω3 = (1340 ± 30) cm–1 in the X̃2Bg state of H2O2+. Contributions from ionization of vibrationally excited levels in the torsion mode have been identified in the TPE spectrum of the first band and the need for a vibrationally resolved TPE spectrum from vibrationally cooled molecules, as well as higher level Franck–Condon factors than performed in this work, is emphasized.
Co-reporter:Dr. Edmond P. F. Lee;Dr. Daniel K. W. Mok; Dudley E. Shallcross; Carl J. Percival;Dr. David L. Osborn; Craig A. Taatjes; John M. Dyke
Chemistry - A European Journal 2012 Volume 18( Issue 39) pp:12411-12423
Publication Date(Web):
DOI:10.1002/chem.201200848

Abstract

CH2OO, the simplest Criegee intermediate, and ozone are isoelectronic. They both play very important roles in atmospheric chemistry. Whilst extensive experimental studies have been made on ozone, there were no direct gas-phase studies on CH2OO until very recently when its photoionization spectrum was recorded and kinetics studies were made of some reactions of CH2OO with a number of molecules of atmospheric importance, using photoionization mass spectrometry to monitor CH2OO. In order to encourage more direct studies on CH2OO and other Criegee intermediates, the electronic and photoelectron spectra of CH2OO have been simulated using high level electronic structure calculations and Franck–Condon factor calculations, and the results are presented here. Adiabatic and vertical excitation energies of CH2OO were calculated with TDDFT, EOM-CCSD, and CASSCF methods. Also, DFT, QCISD and CASSCF calculations were performed on neutral and low-lying ionic states, with single energy calculations being carried out at higher levels to obtain more reliable ionization energies. The results show that the most intense band in the electronic spectrum of CH2OO corresponds to the 1A′ 1A′ absorption. It is a broad band in the region 250–450 nm showing extensive structure in vibrational modes involving O–O stretching and C-O-O bending. Evidence is presented to show that the electronic absorption spectrum of CH2OO has probably been recorded in earlier work, albeit at low resolution. We suggest that CH2OO was prepared in this earlier work from the reaction of CH2I with O2 and that the assignment of the observed spectrum solely to CH2IOO is incorrect. The low ionization energy region of the photoelectron spectrum of CH2OO consists of two overlapping vibrationally structured bands corresponding to one-electron ionizations from the highest two occupied molecular orbitals of the neutral molecule. In each case, the adiabatic component is the most intense and the adiabatic ionization energies of these bands are expected to be very close, at 9.971 and 9.974 eV at the highest level of theory used.

Diazonium, nitro-
1,4,7,10,13,16,19,22-Octathiacyclotetracosane
Krypton(1+), nitrosyl-
Propyl
Oxonium, carbonyl(nitrosooxy)-
Methyldioxy, iodo-
ethyl N-diazocarbamate
[(1Z)-3,3-dimethylbut-1-en-1-yl]benzene
METHYLIUM, CHLOROFLUORO-
Borate(1-), tetrakis[3,5-bis(trifluoromethyl)phenyl]-, rubidium