R,2-, R,3-, and R,4-Dehydrophenol Radical Anions
A R T I C L E S
anion (NO2-) is formed at higher energies. Isolation of the resulting
C6H4O•- (m/z 92) ions were carried out by a combination of SWIFT
and chirp excitation pulses,8,9 and these ions were subsequently cooled
with argon pulsed to a pressure of ∼10-4 Torr. In some experiments,
the carboxylate anions were prepared by ESI of the conjugate acid from
a 1:1 methanol-water solution (v/v) containing 0.1% ammonia.
Scheme 1
Generation of r,4-Dehydrophenoxide Radical Anion by Dis-
sociative Electron Capture of 4-Diazo-2,5-cyclohexadienone. 4-Diazo-
2,5-cyclohexadienone was prepared by literature methods and stored
at -40 °C in the dark.11 The wet diazide was dried in the sample lock
of the solids probe at ∼10-2 Torr and then was introduced into the
high vacuum system. After briefly heating the sample to 40 °C to drive
off residual water, it was ionized with 6 eV electrons to afford a
C6H4O•- anion at m/z 92. This ion was subsequently transferred to the
analyzer cell where it was cooled with a pulse of argon (∼10-4 Torr)
and isolated for further investigation.
Generation of r,2-Dehydrophenoxide Radical Anion by Oxygen
Atom Transfer to o-Benzyne Radical Anion. Atomic oxygen radical
anion was generated by dissociative electron impact on nitrous oxide
and then was reacted with benzene to afford o-benzyne radical anion.12
This ion was allowed to react with a static pressure of carbon dioxide
(∼10-7 Torr) in the source cell and at these low pressures oxygen atom
transfer takes place in preference to adduct formation. The resulting
R,2-dehydrophenoxide radical anion was transferred to the analyzer
cell where it was cooled with argon (∼10-4 Torr) and isolated for further
investigation.
include ZPE corrections and are at 0 K (electron affinities) or 298 K
(proton affinities and bond dissociation energies).
In an attempt to obtain reliable energetic data and to assess several
popular computational approaches, B3LYP/6-311+G(3df,2p)//MP2/6-
31+G(d), G2+(MP2),16 and G317 calculations were carried out. The
second of these methods effectively corresponds to a QCISD(T)/6-
311+G(3df,2p) energy but was obtained on a MP2(FC)/6-31+G(d)
geometry as follows:
Structure Authentication. Each of the C6H4O•- isomers was
converted into phenoxide ion by reaction with tert-butyl mercaptan or
diethylhydroxylamine. The resulting hydrogen atom transfer product
was bracketed with standard reference acids and further characterized
by collision-induced dissociation (CID). These results were compared
to control experiments performed on authentic phenoxide ion generated
by fluoride anion deprotonation of phenol. The R,2- and R,4-isomers
also were derivatized to the corresponding quinone radical anions by
reaction with sulfur dioxide. These latter species were characterized
by bracketing their electron binding energies and comparing the results
to the known electron affinities of o- and p-quinone.
Computations. All calculations were carried out using GAMESS13
and Gaussian 9814 or earlier versions of the program on SGI and IBM
workstations. Geometries were optimized at the HF and MP2 levels
with the 6-31G(d) and 6-31+G(d) basis sets. Closed-shell systems were
treated by using restricted wave functions and open-shell species were
handled by using the unrestricted formalism. In both cases, analytical
vibrational frequencies were computed at both theoretical levels for
each stationary point. Zero-point energies and temperature corrections
to 298 K were computed by scaling the vibrational frequencies using
the following factors: 0.9135 (HF, ZPE), 0.8929 (HF, ν’s), 0.9646
(MP2, ZPE), and 0.9427 (MP2, ν’s), where ZPE refers to the vibrational
zero-point energy correction.15 All of the cited energies in this work
E[G2+(MP2)] ) E[QCISD(T)/6-311+G(d,p)] + E[MP2/6-311+
G(3df,2p)] - E[MP2/ 6-311+G(d,p)] + hlc + ZPE + TC (1)
where hlc is the high level correction term for G2 theory and TC is a
temperature correction to 298 K. Hartree-Fock ZPEs and vibrational
frequencies for the temperature corrections were used in each case,
but in some instances there are significant differences (g1.0 kcal mol-1
)
with the MP2 corrections. In these situations both sets of results are
given.
As the species of interest in this work are inherently multiconfigu-
rational, MCSCF geometries and Hessians also were computed with
the 6-31G(d) and 6-31+G(d) basis sets.18 To account for some of the
dynamic correlation in these species, single-point calculations were
carried out at the MCQDPT2 level with the 6-311+G(d) basis set. All
of the resulting energies were ZPE corrected and adjusted to 298 K,
except for the electron affinities which are at 0 K, by using unscaled
MCSCF vibrational frequencies.
Results and Discussion
Deprotonation of o-, m-, and p-nitrobenzoic acid by fluoride
ion in the gas phase affords the corresponding carboxylate anions
(2), which lose carbon dioxide upon 5-6 eV SORI-CID.
Further fragmentation of the phenide isomers at 2-3 eV yields
the desired R,2-, R,3-, and R,4-dehydrophenoxide radical anions
(Scheme 1 and Figure 1). These cleavages previously have been
reported in the analytical chemistry literature,7 but the structures
and reactivities of the resulting C6H4O•- ions were not explored.
To establish the structures of 3o, 3m, and 3p, their reactivities
were examined. It was anticipated that these radical anions
should have the σ-system of a phenyl radical and the π-system
of a phenoxide ion and would display radical reactivity similar
to related distonic radical cations containing an aryl radical
moiety. In accord with these expectations, all three isomers
(11) Puza, M.; Doetschman, D. Synthesis 1971, 481-488.
(12) Guo, Y.; Grabowski, J. J. J. Am. Chem. Soc. 1991, 113, 5923-5931.
(13) Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Scuseria, G. E.; Robb, M.
A.; Cheeseman, J. R.; Zakrewski, V. G.; Montgomery, J. A. Jr.; Stratmann,
R. E.; Burant, J. C.; Dapprich, S.; Millam, J. M.; Daniels, A. D.; Kudin,
K. N.; Strain, M. C.; Farkas, O.; Tomasi, J.; Barone, V.; Cossi, M.; Cammi,
R.; Mennucci, B.; Pomelli, C.; Adamo, C.; Clifford, S.; Ochterski, J.;
Petersson, G. A.; Ayala, P. Y.; Cui, Q.; Morokuma, K.; Malick, D. K.;
Rabuck, A. D.; Raghavachari, K.; Foresman, J. B.; Cioslowski, J.; Oritz,
J. V.; Baboul, A. G.; Stefanov, B. B.; Lui, G.; Liashenko, A.; Piskorz, P.;
Komaromi, I.; Gomperts, R.; Martin, R. L.; Fox, D. J.; Ketih, T.; Al-Laham,
M. A.; Peng, C. Y.; Nanayakkara, A.; Gonzalez, C.; Challacombe, M.;
Gill, P. M. W.; Johnson, B.; Chen, W.; Wong, M. W.; Andres, J. L.;
Gonzalez, C.; Head-Gordon, M.; Replogle, E. S.; Pople, J. A. Gaussian
98, ReVisions A.6-9, Gaussian, Inc., Pittsburgh, PA, 1998.
(14) Schmidt, M. W.; Baldridge, K. K.; Boatz, J. A.; Elbert, S. T.; Gordon, M.
S.; Jensen, J. H.; Koseki, S.; Matsunaga, N.; Nguyen, K. A.; Su, S. J.;
Windus, T. L.; Dupuis, M.; Montgomery, J. A. J. Comput. Chem. 1993,
14, 1347-1363.
(15) Pople, J. A.; Scott, A. P.; Wong, M. W.; Radom, L. Isr. J. Chem. 1993,
33, 345-350.
(16) (a) Curtiss, L. A.; Raghavachari, K.; Pople, J. A. J. Chem. Phys. 1993, 98,
1293-1298. (b) Gronert, S. J. Am. Chem. Soc. 1993, 115, 10 258-10 266.
(17) Curtiss, L. A.; Raghavachari, K.; Redfern, P. C.; Rassolov, V.; Pople, J.
A. J. Chem. Phys. 1998, 109, 7764-7776.
(18) For more details, see ref 4b.
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