5672 J. Am. Chem. Soc., Vol. 121, No. 24, 1999
PaVlik et al.
Scheme 9
The sudden decrease in φF suggests the existence of a decay
channel, which has been referred to as “channel three”.15 In
benzene, this decay pathway, which originates in a vibrationally
excited π,π* state, results in the formation of the ground-state
diradical prefulvene, the presumed precursor of benvalene.16
Although the analogous meta-bonded valence isomer of
pyridine, azabenzvalene, has never been isolated or definitively
detected, theoretical calculations predict that the S2 (π,π*) state
of pyridine crosses both the S1 (n,π*) and So states along a
concerted pathway, leading to the ground-state azaprefulvene
diradical,17 the suggested intermediate responsible for intra-triad
isomerizations (Schemes 5 and 6). Quenching of these intra-
triad reactions by added N2 is consistent with their origin from
an excited state possessing excess vibrational energy.
In contrast to the intra-triad reactions, the inter-triad inter-
conversions of 2,3- and 2,5-dimethylpyridines (1) and (3) are
enhanced by the addition of N2, are the major products observed
upon irradiation in condensed media, and are the only photoi-
somerization products formed upon irradiation with light of
wavelength >290 nm. Furthermore, the suggested Dewar
pyridine intermediates (Scheme 8) can also be detected upon
irradiation of 1 or 3 in the condensed phase at low temperature.
Accordingly, these reactions occur from an excited state of lower
energy. A number of facts indicate that this lower energy state
is the T1 state of the dimethylpyridine.
In the case of pyridine and methylpyridines, the quantum yield
for intersystem crossing is known to increase substantially as
the excitation energy is decreased from SofS2 (π,π*) absorption
to the SofS1 (n,π*) region.18,19 Thus, the net effect of decreasing
the excitation energy is to increase the triplet population.
Although no evidence has been detected for any triplet state,
gas-phase chemistry in pyridine,20 photolysis of pyridine at 254
nm in an argon matrix has been shown to result in the formation
of Dewar pyridine.21 Furthermore, this reaction was enhanced
when the matrix was changed to xenon. This enhancement in
xenon indicates strongly that the triplet state of pyridine is
involved in the isomerization.21
2,3-dimethylpyridine (1) undergoes only 3,6-bonding to yield
1c. 1,3-Sigmatropic shift of nitrogen from C-6 to C4 (path B,
Scheme 8b) or of C-4 from C-3 to N (path C, Scheme 8b),
followed by rearomatization of 1c′ (an enantiomer of 1c) or
1d, results only in the regeneration of 1, the reactant. Alterna-
tively, 1c could also rearrange via 1,3-sigmatropic shift of C-2
from C-3 to C-5 (path A, Scheme 8b) or of C-5 from C-6 to
C-2 (path D, Scheme 8b), followed by rearomatization of 3c or
3d, to result in the 2,5-dimethylpyridine (3), the inter-triad
product.
1H NMR spectroscopy (Figure 2) also revealed that 2,5-
dimethylpyridine (3) undergoes 3,6-bonding to form 3c′. 1,3-
Sigmatropic shift of nitrogen from C-6 to C-4 (path A, Scheme
9) would convert 3c′ into its enantiomer 3c. Rearomatization
thus regenerates 2,5-dimethylpyridine (3). 1,3-Sigmatropic shift
of C-2 from C-3 to C-5 (path B, Scheme 9), followed by
rearomatization of 1c′, results in the formation of 2,3-dimeth-
ylpyridine (1), the inter-triad product.
1
The relative intensities of the H NMR spectral signals for
Dewar pyridines 1c and 3c, formed from dimethylpyridines 1
and 3, indicate that, after the same duration of irradiation, the
yield of 3c from 3 is larger than the yield of 1c from 1. This
may be due to the greater stability of 3c, which bears methyl
substituents at both the CdC and CdN double bonds as
compared to 1c, which has one of its methyl groups at a
bridgehead position. These relative yields of the Dewar pyridines
are consistent with the yields of the inter-triad reactions
observed. Thus, as shown in Table 1, 2,5-dimethylpyridine (3),
which in the condensed phase gives Dewar pyridine in the
greater yield, is also converted in the gas phase to the inter-
triad product 2,3-dimethylpyridine (1) in the greater yield.
Conversely, 2,3-dimethylpyridine (1), which in the condensed
phase gives the Dewar pyridine in the lower yield, is also
converted in the gas phase to the inter-triad product 3 in the
lower yield.
The 0-0 bands for SofS1 and SofS2 absorptions in pyridine
vapor occur at 34 769 and 38 350 cm-1, respectively.11 This
corresponds to Es1 (n,π*) and Es2 (π,π) at 99.4 and 109.7 kcal
mol-1, respectively. Methyl substitution in pyridine significantly
lowers the S2 energy level, while the S1 level is nearly
unchanged.11 The energies of the S1 (n, π*) and S2 (π,π*) states
in 2,6-dimethylpyridine (4), for example, are 100.4 and 105.5
kcal mol-1, and the six dimethylpyridines are expected to have
excited-state energies similar to these values.11 Photochemical
excitation of dimethylpyridines with light of 254 nm is thus
expected to result in the population of S2 (π,π*) excited states
with excess vibrational energy.
Both experimental22 and theoretical studies23 point to the
existence of two triplet forms of pyridine with different intrinsic
lifetimes, brought about by strong pseudo-Jahn-Teller vibronic
coupling of the nearly degenerate 3π,π* and 3n,π* states. This
results in a double minimum in the lowest triplet surface,
yielding a vibrationally relaxed triplet state with a boat-shaped
geometry which is suggested to be involved in the photochemi-
cal generation of Dewar pyridine.22
(13) Yamazaki, I.; Murao, T.; Yamanaka, T.; Yoshihara, K. Faraday
Discuss Chem. Soc. 1983, 75, 395-405.
(14) Kaplan, L.; Wilzbach, K. E. J. Am. Chem. Soc. 1968, 90, 3291-
3292.
(15) Riedle, E.; Weber, T.; Shubert, U.; Neusser, H. J.; Schlag, E. W. J.
Chem. Phys. 1990, 93, 967-978. Suzuki, T.; Ito, M. J. Chem. Phys. 1989,
91, 4564-4570. Hornburger, H.; Sharp, C. M. Chem. Phys. 1986, 101,
67-79. Sobolewski, A. L.; Czerminski, R. Chem Phys. 1989, 130, 123-
128. Sobolewski, A. G. J. Chem. Phys. 1990, 93, 6433-6439. Sobolewski,
A. L.; Lim, E. C.; Siebtand, W. Int. J. Quantum Chem. 1991, 39, 309-
324.
(16) Palmer, I. J.; Ragazos, I. N.; Bernardi, F.; Olivucci, M.; Robb, M.
A. J. Am. Chem. Soc. 1993, 115, 673-682.
(17) Sobolewski, A. L.; Domcke, W. Chem. Phys. Lett. 1991, 180, 381-
386.
(18) Yamazaki, I.; Sushida, K.; Baba, H. J. Chem. Phys. 1979, 71, 381-
387.
The nonradiative decay properties of pyridine are reported
to be similar to those of benzene. Thus, the φF in both
pyridine11-13 and benzene14 shows a characteristic dependence
on excess vibrational energy in the lowest π,π* excited state.
(19) Yamazaki, I.; Murao, T.; Yamanaka, T.; Yoshihara, K. Faraday
Discuss. Chem. Soc. 1983, 75, 395-405.
(20) Lemaire, J. J. Phys. Chem. 1967, 71, 612-615.
(21) John Stone, E. E.; Sodeau, J. R. J. Phys. Chem. 1991, 95, 165-
169.
(11) Yamazaki, I.; Sushida, K.; Baba, H. J. Phys. Chem. 1979, 71, 381-
387.
(12) Yamazaki, I.; Sushida, K.; Baba, H. J. Lumin. 1979, 425-428.
(22) Selco, J. I.; Holt, P. L.; Weisman, R. B. J. Chem. Phys. 1983, 79,
3269-3278.
(23) Naqaoka, S.; Nagashima, U. J. Phys. Chem. 1990, 94, 4467-4469.