2012
DOI: 10.1063/1.4757727
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Nonadiabatic effects in substitutional isomers of Jahn-Teller molecules: The strange case of hydroxymethoxy

Abstract: The effects of nonadiabatic interactions attributable to a seam of conical intersections on the electronic structure of the 1,2(2)A states of hydroxymethoxy (HO)CH(2)O is explored. Illuminating comparisons are made between hydroxymethoxy and ethoxy and isopropoxy, all of which can be thought of as substitutional isomers of the methoxy radical. Surprisingly, the potential energy surfaces and conical topographies for hydroxymethoxy are shown to be dramatically different from those evidenced in ethoxy or isopropo… Show more

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Cited by 10 publications
(18 citation statements)
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“…A relaxed potential energy scan has a barrier to interconversion of 158 cm -1 for the ground 2 A state surface. This is lower than the multireference calculations from Dillon and Yarkony, 26 who report a barrier to interconversion of 361 cm -1 for the ground 2 A state, and with Eisfeld and Francisco, who report a barrier of at most 550 cm -1 for the 2 A state rotamer interconversion. The barrier to interconversion for the excited 2 A state is higher, at 968 cm -1 , which agrees very well with the multireference calculations from Dillon and Yarkony (993 cm -1 ).…”
Section: A H-oco Torsionmentioning
confidence: 54%
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“…A relaxed potential energy scan has a barrier to interconversion of 158 cm -1 for the ground 2 A state surface. This is lower than the multireference calculations from Dillon and Yarkony, 26 who report a barrier to interconversion of 361 cm -1 for the ground 2 A state, and with Eisfeld and Francisco, who report a barrier of at most 550 cm -1 for the 2 A state rotamer interconversion. The barrier to interconversion for the excited 2 A state is higher, at 968 cm -1 , which agrees very well with the multireference calculations from Dillon and Yarkony (993 cm -1 ).…”
Section: A H-oco Torsionmentioning
confidence: 54%
“…48 The ground and first excited states of CH 2 (OH)O • , using the C s symmetry labels valid at HOCO = 0°, are described by 2 A and 2 A state labels. The molecular orbitals associated with the two lowest energy electronic states of H 2 C(OH)O • have also already been calculated, 11,26 and are associated with a half-filled a (a ) symmetry p y (p x ) orbital at the O1 atom for the ground (excited) electronic state (note: in this representation, the heavy atoms are taken to lie in the xz plane The lowest eBE peak in the spectrum, peak A, has a fwhm of 0.036 eV, a value close to the experimental resolution, suggesting minimal rotational broadening. See Section II.A for more details.…”
Section: A Experimental Photoelectron Spectra and Ea(h 2 C(oh)o • )mentioning
confidence: 99%
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