Formation of Hydrogen Trioxide
A R T I C L E S
significant multireference character that are difficult to describe
with restricted or unrestricted DFT (RDFT and UDFT).
Therefore, we routinely carried out stability tests16 and used
broken-symmetry UDFT (BS-UDFT) when needed (i.e., in case
of negative eigenvalues of the stability matrix). BS-UDFT im-
plicitly provides a two-configurational description and leads to
reasonable results provided the splitting between the low-spin
state in question and the associated high-spin state is relatively
small.17,18 In this connection it has to be mentioned that standard
functionals based on the generalized gradient approximation
(GGA) account for a significant amount of long-range correla-
tion,19 but lead to a double-counting of correlation effects when
used in connection with BS-UDFT.20 This was another reason
why B3LYP rather than BLYP was used in this work.20
The fact that DFT with the exchange functionals presently
in use accounts for unspecified nondynamic electron correlation
is closely connected with the self-interaction error (SIE) of these
functionals.19,21 The SIE is often the reason for the good
performance of DFT in cases where other single determinant
methods fail.19,21 However, the SIE also results in a serious
failure of DFT when odd-electron situations occur in a chemical
reaction.19-22 For example, H abstraction by a radical (three-
electron situation) is wrongly described by any exchange
functional based on either the local density approximation or
GGA.23 The TS of the reaction is severely underestimated thus
leading often to reactions without barrier. We use in these
situations self-interaction corrected DFT (SIC-DFT) based on
the Perdew-Zunger approach24 and programmed in a pertur-
bational (PSIC) and a self-consistent version (SCF-SIC).19-21
For details, see ref 25.
were carried out with standard procedures based on analytical
energy gradients. Frequency calculations were performed to
characterize the optimized structures as minima or transition
states, where the transition states were found to each have a
single imaginary frequency. In addition, the vibrational frequencies
were used to obtain temperature corrected energies, enthalpies,
entropies, and free energies. For the purpose of modeling the
effects of solvation, the PISA continuum model27 was applied
using acetone as a solvent (dielectric constant ꢀ ) 20.728).
van der Waals complexes are difficult to calculate with DFT.29
However, if complexes are stabilized by H-bonding, which
include both electrostatic and some covalent bonding, DFT
performs better.30 For the purpose of getting reasonable complex
binding energies, we apply the counterpoise method31 to reduce
the basis set superposition error (BSSE).
In some cases, cyclic transition states were optimized using
the ring puckering coordinates of Cremer and Pople.32 These
coordinates make it possible to freeze individual puckering
parameters and to carry out constrained optimizations. For this
purpose the program PUCKER33 was used, which is part of the
quantum chemical package COLOGNE 2003.34 All calculations
were performed with the quantum chemical program packages
COLOGNE 200334 and Gaussian 98.35
Results and Discussion
In the following we will discuss first the ozonation of 1,2-
diphenylhydrazine, then that of 1,2-dimethylhydrazine. Calcula-
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Barone, V.; Cossi, M.; Tomasi, J. J. Chem. Phys. 1997, 107, 3210. (c)
Cammi, R.; Cossi, M.; Tomasi, J. J. Chem. Phys. 1996, 104, 4611. (d)
Mennucci, B.; Tomasi, J. J. Chem. Phys. 1997, 106, 5151. (e) Tomasi, J.;
Mennucci, B. In Encyclopedia of Computational Chemistry; Schleyer, P.v.
R., Allinger, N. L., Clark, T., Gasteiger, J., Kollman, P. A., Schaefer, H.
F., III, Schreiner, P. R., Eds.; Wiley: Chichester, 1988; Vol. 1, p 2547.
(28) CRC Handbook of Chemistry and Physics on CD-ROM, 2000 Version;
Lide, D. R., Ed.; CRC Press LLC: Boca Raton, FL, 2000.
(29) (a) Kristyan, S.; Pulay, P. Chem. Phys. Lett. 1994, 229, 175. (b) Perez-
Jorda, J. M.; Becke, A. D. Chem. Pys. Lett. 1995, 233, 134. (c) Hobza, P.;
Sponer, J.; Reschel, T. J. Comput. Chem. 1995, 16, 1315. (d) Ruiz, E.;
Salahub, D. R.; Vela, A. J. Am. Chem. Soc. 1995, 117, 1141. (e)
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TS energies were determined by SIC-DFT using the following
procedure. The geometry of the DFT calculation was used for
PSIC and SCF-SIC single point calculations. In this way an
estimate of the improved barrier was found. If a TS geometry
could not be determined, that found for a derivative was used
to obtain by single point calculation a SIC-DFT barrier.
Alternatively, increments were used determined for a homo-
logue. Calculations showed that in this way consistent reaction
barriers could be obtained. The corresponding activation en-
thalpies were determined by using vibrational corrections from
the DFT calculation or estimating the latter from values obtained
for another hydrazine.
(30) (a) Sosa, C. P.; Carpenter, J. E.; Novoa, J. J. In Chemical Applications of
Density-Functional Theory; Laird, B. B., Ross, R. B., Ziegler, T., Eds.;
ACS Symposium Series 629; American Chemical Society: Washington,
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For all calculations, Pople’s 6-31G(d,p) basis set26a was used,
however in several cases the 6-311++G(3df,3pd) basis26b was
employed to verify 6-31G(d,p) results. Geometry optimizations
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