Tautomerization and dissociation of dimethyl phosphonate ions (CH3O)(2)P(H)=O center dot+: Theory and experiment in concert

Citation
Ln. Heydorn et al., Tautomerization and dissociation of dimethyl phosphonate ions (CH3O)(2)P(H)=O center dot+: Theory and experiment in concert, Z PHYS CHEM, 215, 2001, pp. 141-182
Citations number
86
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
ZEITSCHRIFT FUR PHYSIKALISCHE CHEMIE-INTERNATIONAL JOURNAL OF RESEARCH IN PHYSICAL CHEMISTRY & CHEMICAL PHYSICS
ISSN journal
09429352 → ACNP
Volume
215
Year of publication
2001
Part
2
Pages
141 - 182
Database
ISI
SICI code
0942-9352(2001)215:<141:TADODP>2.0.ZU;2-2
Abstract
The unimolecular gas phase chemistry of the title ion, (CH3O)(2)P(H) = O.+, (1(.+)) and its tautomer dimethyl phosphite, (CH3O)(2)P-OH.+, (2(.+)) was investigated using mass spectrometry based experiments in conjunction with computational quantum chemistry. A facile tautomerization of the "keto" ion 1(.+) into its "enol" isomer 2(.+) is prevented by a high 1,2-H shift barr ier. Instead, 1(.+) readily isomerizes via a 1,4-H shift to the very stable distonic ion CH2O-(CH3O)P(H)OH.+ (1a(.+)) and related ion-dipole complexes which serve as precursors for the low energy loss of CH2=O. Loss of CH2=O is also the major dissociation of the enol ion 2(.+), which is more stable than 1(.+) by 31 kcal/mol. The reaction involves a 1,3-H shift leading to 1 a(.+) and, at a marginally higher energy, a competing 1,4-H shift leading t o the ion-dipole complex CH2O-P(OH)-O(H)CH3.+ (1b(.+)). The resulting produ ct ions, viz (CH3O)P(H)OH.+ and P(OH)-O(H)CH3.-, are separated by a high 1, 2-H shift barrier (44kcal/mol). However, the CH2O moiety in 1a(.+) and 1b(. +) is calculated to reduce this barrier significantly by a mechanism coined as proton-transport catalysis. The identity of the ions was probed by tandem mass spectrometry methods. Th ese include MI (metastable ion) or CID (collision induced dissociation) spe ctra, consecutive MI/CID and CID/CID spectra, NRMS (neutralization-reioniza tion mass spectra), NR/CID and CIDI (collision induced dissociative ionizat ion) spectra, time-resolved CID spectra and deuterium labelling. The energe tics of the CH2=O loss from 1(.+) and 2(.+) was derived from ionization and appearance energies determined by VUV photoionization. The experimental re sults agree quite well with the computational findings. Heats of formation, isomerization barriers and dissociation energies of the various ionic and neutral species were obtained by the wavefunction-based CBS-QB3 method. Ess entially identical energy profiles on the C2H7O3P.+ surface were obtained w ith the computationally less demanding novel MPW1K empirical DFT method in conjunction with the aug-cc-pVTZ basis set. Theory and experiment yield a consistent potential energy profile that desc ribes the isomerization and low energy dissociation chemistry of ions 1(.+) and 2(.+) (Scheme 4). In the mus timeframe ions 1(.+) have completely isom erized into distonic ions 1a(.+) which do not significantly communicate wit h their more stable enol counterparts. However, ion-molecule reactions of 1 (.+) with benzonitrile lead to a complete enolization, This is by virtue of a dipole-assisted lowering of the 1,3-H shift barrier separating isomers 1 a(.+) and 2(.+).