Kvaskoff et al.
JOCArticle
Conclusion
CASSCF34 optimizations and single-point CASPT2 calcula-
tions35 were performed for open-shell and related systems, and
were carried out with the MOLCAS suite of programs,36 using
the 6-31G* basis set. The CASSCF calculations used an
8-electron, 8-orbital active space, e.g. for 19: 3π, 3π*, and the
2 p-AOs on the nitrene-N atom. The reference weights of the
CASSCF wave function remained stable in the range 77-80%.
Cartesian coordinates, energies, vibrational frequencies, and
details of the correlated orbitals in the CASSCF active space
are listed in the Supporting Information.
The isomeric 3-pyridazylcarbene 10 and 2-pyridylnitrene
19 were investigated. There is little evidence for interconver-
sion of these two isomers, but each has a rich chemistry. Mild
FVT of triazolopyridazine 8 generates the diazomethyl
valence tautomer 9, which on either matrix photolysis or
flash vacuum thermolysis (FVT) gives rise to 3-pyridazyl-
carbene 10. The carbene was detected by ESR spectroscopy
in the photolysis reaction. Matrix photolysis with IR
observation reveals ring-opening of the carbene to diazoalk-
enyne 11, which again loses N2 to generate a new carbene,
pent-2-en-4-yn-1-ylidene 12; this too was detected by ESR
spectroscopy, and it rearranges to pentadienyne 13, ethynyl-
cyclopropene 14, and, at elevated temperatures, 1,4-penta-
diyne 15.
Photolysis of matrix-isolated tetrazolo[1,5-a]pyridine/
2-azidopyridine 22T/22A yields both triplet 2-pyridylnitrene
19 and its ring-opened isomer, the cyanodienylnitrene 23,
which are detected by ESR spectroscopy. 1,3-Diazacyclo-
heptatetraene 21 is formed cleanly on matrix photolysis as
observed by IR spectroscopy. It is also a major product of
FVT of 22T/22A under mild conditions. Photolysis of 21
above 300 nm causes its rearrangement to the spiroazirene
25, identified by its Ar-matrix IR spectrum.
FVT of 8/9 causes formation of Z- and E-glutacononitriles
27Z,E and minor amounts of 2- and 3-cyanopyrroles 28 and
29 in addition to 13-15. FVT of tetrazolopyridine/2-azido-
pyridine 22T/22A also affords compounds 27-29, but the
ratios of yields of these products are very different in the two
systems.
Calculations support the postulate that both 3-pyridazyl-
carbene (via 1,7-diazacycloheptatetraene 17) and 2-pyridyl-
nitrene 19 can undergo ring-opening to vinylnitrene 23, but
they can lead to different conformers of 23; one, 23EZ, is
predominantly a precursor of glutacononitriles 27; the other,
23ZZ, is a precursor of 2- and 3-cyanopyrroles via 2-cyano-
2H-pyrrole 32. Another potential route to cyanopyrroles
proceeds via electrocyclization of 1,3-diazacycloheptate-
traene 21 to diazabicyclo[3.2.0]heptatriene 24 and spiroazir-
ene 25. The ring-opening-reclosure reaction via dienyl-
nitrene 23 emerges as the energetically most favorable
mechanism of ring-contraction in 2-pyridylnitrenes.
Experimental Section
General procedures have been published.16,27,29 In matrix
isolation for IR spectroscopy, Ar gas and sample vapor were
codeposited on a CsI target maintained at 25 K. The Ar flow rate
was maintained at ca. 4 mbar per min to obtain a thin,
transparent matrix. After depositing the matrix for ca. 30 min,
the CsI target was cooled to 10 K, and IR spectra were recorded
with 1 cm-1 resolution. For ESR spectroscopy a similar cryostat
was used, where the sample and Ar were condensed on a Cu rod
at ca. 15 K. Photolyses were carried out with use of a 1000 W
high-pressure Xe/Hg lamp equipped with a monochromator
and appropriate cutoff and interference filters, a 75 W low
pressure Hg lamp (254 nm), or excimer lamps operating at 222
(25 mW/cm2) and 308 nm (50 mW/cm2).
FVT experiments with matrix isolation employed a 10 cm
long, 0.7 cm i.d. electrically heated quartz tube suspended in a
vacuum chamber (2.0 ꢀ 10-6 mbar) directly flanged to the
cryostat cold head, with a wall-free flight path of ca. 3 cm
between the exit of the quartz tube and the CsI or Cu targets.
The temperatures used for FVT experiments ranged from 500
to 700 °C
In preparative FVT experiments, the sample was placed in a
sublimation tube and sublimed into a 20 ꢀ 2 cm quartz pyrolysis
tube. The FVT unit was evacuated with an oil diffusion pump
capable of a vacuum of 10-5-10-4 mbar. The pyrolysis pro-
ducts were collected on a coldfinger cooled with liquid nitrogen
(ca. 77 K). After the end of the experiment, the collected product
was dissolved in CDCl3, and NMR and GC-MS analyses were
carried out.
GC-MS analysis used a ZB-5 Zebron GC column (30 m,
0.32 mm i.d., 0.25 μm film thickness), He carrier gas at a flow
rate of 3.7 mL/min, column head pressure 100 kPa, inlet
temperature 200 °C, and GC-MS interface 250 °C. The tempera-
ture program started at 85 °C for 2 min, followed by a ramp of
12 deg/min up to 250 °C.
[1,2,3]Triazolo[1,5-b]pyridazine 8. 3-Pyridazinecarboxalde-
hyde37 was synthesized from furfuryl acetate38 and converted
to its hydrazone.39 The hydrazone (500 mg, 4 mmol) was
dissolved in 50 mL of chloroform, and activated manganese
dioxide (460 mg, 8 mmol, Fluka) was added slowly. The solution
was stirred for 3 h at rt and filtered over Celite, then the solvent
was removed in vacuum. The solid so obtained was purified by
sublimation (70-75 °C, 4 ꢀ 10-5 mbar) to yield colorless
crystals, 348 mg (71%), mp 132-133 °C (lit.39 mp 132-133 °C);
1H NMR (CDCl3) 8.47 (dd, J = 4.3, 1.8 Hz, 1 H), 8.18 (s, 1 H),
8.14 (dd, J = 9.0, 1.8 Hz, 1 H), 7.12 (dd, J = 9.0, 4.3 Hz, 1 H).
Computational Method
Calculations of all species were performed with the B3LYP
method,31 as implemented in the Gaussian 03 suite of pro-
grams,32 with the 6-31G* basis set for geometry and transition
state optimizations. Energies of open-shell S1 nitrenes at the
(U)B3LYP/6-31G* level were estimated with use of the Cra-
mer-Ziegler method.24 Reported energies include zero-point
vibrational energy corrections. All transition states were con-
firmed by intrinsic reaction coordinate calculations. Harmonic
vibrational frequencies were computed with use of the 6-311G**
basis set, and a scaling factor of 0.967 was applied.33 Additional
(35) Andersson, K.; Roos, B. O. CASPT2. In Modern Electronic Struc-
ture Theory; World Scientific Publ. Co.: Singapore, 1995; Vol. 2, Part 1, p 55
˚
(36) (a) Karlstrom, G.; Lindh, R.; Malmqvist, P.-A.; Roos, B. O.; Ryde,
€
U.; Veryazov, V.; Widmark, P.-O.; Cossi, M.; Schimmelpfennig, B.;
(31) (a) Becke, A. D. J. Chem. Phys. 1993, 98, 5648. (b) Lee, C.; Yang, W.;
Parr, R. G. Phys. Rev. B 1988, 37, 785.
ꢀ
(32) Frisch, M. J., et al. Gaussian 03, Revision E.01; Gaussian, Inc.,
Wallingford, CT, 2004. (For the complete reference, see the Supporting
Information.)
Neogrady, P.; Seijo, L. Comput. Mater. Sci. 2003, 28, 222. (b) Andersson,
K., et al. MOLCAS, version 7.2; University of Lund: Lund, Sweden, 2008. (For
the complete reference, see the Supporting Information.)
(33) Irikura, K. K.; Johnson, R. D.; Kacker, R. N. J. Phys. Chem. A 2005,
109, 8430. Wong, M. W. Chem. Phys. Lett. 1996, 256, 391. Scott, A. P.;
Radom, L. J. Phys. Chem. 1985, 100, 16502.
(37) Heinisch., G.; Mayrhofer, A. Monatsh. Chem. 1977, 108, 213.
(38) Klauson-Kaas, N.; Limborg, F. Acta Chem. Scand. 1947, 1, 613.
(39) Maury, G.; Meziane, D.; Srairi, D.; Paugam, J. P.; Paugam, R. Bull.
Soc. Chim. Belg. 1982, 91, 153.
(34) Roos, B. O. Adv. Chem. Phys. 1987, 69, 399.
1610 J. Org. Chem. Vol. 75, No. 5, 2010