give a singlet ground state for PFPCCl (2), with
ΔGS-T = 4.2 kcal/mol.8,13 Similar calculations show
that ΔGS-T = 14.9 kcal/mol in PFPCF (3).11 Singlet
states of carbenes are more sensitive to substituents
than triplet states, and the singlet state of PFPCF is
preferentially stabilized by the strong π-donating/
σ-withdrawing abilities of the fluoro substituent.
PFPCCl and PFPCF readily cyclopropanated a ser-
ies of olefins, including tetramethylethylene, 2-ethyl-1-
butene, trans-butene, and cis-butene; cf. Scheme 2.
Additionally, both carbenes inserted into the tertiary
CꢀH bond of adamantane.
Scheme 1. Preparation of Pentafluorophenylfluorodiazirine
pentafluorophenylbromodiazirine 4c and conversion
of the latter to the desired fluorodiazirine 4b by a
diazirine exchange reaction with tetrabutylammo-
nium fluoride.10,11 Fluorodiazirine 4b was character-
ized by IR, UV, and 13C and 19F NMR spectroscopy.11
In particular, the UV spectrum in pentane revealed
maxima at 323 and 338 nm. Note that diazirine 4c was
used only as a relay compound in the preparation of
fluorodiazirine 4b. No doubt photolysis of 4c would
provide pentafluorophenylbromocarbene and a par-
allel series of products (7-Brꢀ10-Br).
Laser flash photolysis (LFP) of diazirine 4a in pentane
generated PFPCCl (2) which displayed π(phenyl) f
p(carbene) absorptions at 300 and 372 nm and a σ(carbene)
f p(carbene) absorption at 596 nm.8 LFP of diazirine 4b
produced PFPCF (3) which afforded a similar UVꢀvis
spectrum; cf. Figure 1. Here, charge-transfer type transitions
from the nearly degenerate set of high-lying phenyl π orbitals
to the vacant carbenic p orbital are responsible for the
absorptions at 292 and 324 nm, whereas the weak absorption
at 564 nm is associated with electron promotion from the
carbene’s filled σ orbital (HOMO) to its vacant p orbital
(LUMO). The absorptions are computed11,12 at 271 nm
(f = 0.287), 342 nm (f = 0.051), and 621 nm (f = 0.0045).
Both PFPCCl and PFPCF give intense N-ylide spec-
tra with pyridine in pentane. The ylides, 6a and 6b, each
absorbed at 468 nm and formed very rapidly with
k = 8.1 ꢁ 109 Mꢀ1 sꢀ1 (6a) or 6.4 ꢁ 109 Mꢀ1 sꢀ1 (6b).11
Figure 1. Calibrated UVꢀvis spectrum of PFPCF (3) in pen-
tane 200 ns after laser pulse; π (phenyl) f p(carbene) absorp-
tions at 292 and 324 nm, σ(carbene) f p(carbene) absorption
at 564 nm.
Olefin-pentane solutions containing diazirine 4a or 4b
were irradiated for 18 h in Pyrex tubes with a 200 W
focused Osram XE mercury lamp at room temperature.
The cyclopropane products were isolated from the sol-
vent-stripped residues by column chromatography over
silica gel with pentane elution. The products are shown in
1
structures 7ꢀ10; their identities were established by H,
13C, and 19F NMR spectroscopy and by mass spec-
troscopy.11 Isolated yields appear in Table 1 and range
from 59 to 87%. GC demonstrated product purities in
excess of 95%.
In keeping with the singlet nature of PFPCCl and
PFPCF, capillary GC analysis of their reaction products
with cis- and trans-butene showed the products to have
been formed with >99% stereospecificity. With PFPCF
and cis-butene, where the syn-F and anti-F isomers of
product 10-F could be separated, NMR analysis indicated
that the syn-F isomer predominated by a factor of 2.2.14
This stereoselectivity resembles that observed with PhCF
and cis-butene, where syn-F/anti-F was about 1.6.15
Although PFPCH (1) possesses a triplet ground
state,7 computational studies at the CCSD(T) level
(10) (a) Moss, R. A. Acc. Chem. Res. 2006, 39, 267. (b) Cox, D. P.;
Moss, R. A.; Terpinski, J. J. Am. Chem. Soc. 1983, 105, 6513.
(11) See the Supporting Information for details.
(12) Results obtained at the TD-B3LYP/6-311þG(d)//B97D/
6-311þG(d) level applying the polarizable conductor self-consistent
reaction field model (CPCM) and n-pentane as the solvent.
(13) CCSD(T) denotes a calculation based on the Coupled Cluster
method that includes single and double excitations fully and triple
(14) In the 19F NMR spectrum, the syn-F isomer has the more
shielded F atom and the smaller vic-HꢀF coupling.11,15
excitations via perturbation theory. With this methodology, ΔGS-T
=
ꢀ5.6 kcal/mol for PFPCH, with the triplet state being more stable than
(15) (a) Moss, R. A.; Lawrynowicz, W. J. Org. Chem. 1984, 49, 3828.
(b) Moss, R. A.; Przybyla, J. Tetrahedron 1969, 25, 647.
the singlet state.8
Org. Lett., Vol. 13, No. 17, 2011
4753