of the triplet state is increased. In a hydrogen-donating solvent
such as ethanol this is revealed by the significant yield of amine
at room temperature. As one may expect, in an inert solvent and
with a higher absorbed light flux the main reaction from the
triplet state remains dimerization to the azo compound (27% in
MeCN).
However, electronic excitation of the triplet state makes
hydrogen abstraction effective. It has been suggested that the
lowest excited state of triplet arylnitrenes corresponds to a π→n
transition;26 thus, the excited triplet can be likened to an iminyl
radical and is expected to be a much better hydrogen abstractor.
In the matrix such a process obviously takes place intra-
molecularly and leads to the dihydroquinoxaline 8.
Reduction of the nitrene to amine 3 is effective under two
conditions. The first one is triplet photosensitization of the
azide decomposition. As shown in Table 1, Michler’s ketone
(MK, chosen because it allows selective irradiation) sensiti-
zation generates the triplet nitrene and this gives the amine
(presumably via reduction by MK, see below) with a strong
decrease in or elimination of the singlet nitrene products.
The second condition involves electron transfer. The experi-
ments conducted in the presence of DEA show that the yield
of singlet products is marginally affected (except for the
formation of the trace of hydrazine 7) and the yield of amine
3 is greatly increased. This fits with the previous suggestion by
Schuster that the p-nitrophenylnitrene triplet state is a powerful
electron acceptor,12 and strengthens the evidence that a selective
quenching of the triplet state is involved in the formation of the
amine. The electron transfer–proton transfer path is a more
effective mechanism for triplet state reduction than hydrogen
abstraction (compare the yield of 3 in the presence of DEA and
in neat ethanol). This suggests that Michler’s ketone acts both
as sensitizer and as reducing agent and this causes the higher
yield of amine than of azo compound.
The situation changes at low temperature. First of all,
the triplet can be observed in a glassy matrix. The spectrum
measured at 90 K shows the characteristic intense absorption in
the visible (565 nm, log ε ca. 3.4), which is red shifted with
respect to the non-nitrated pyrazolylphenylnitrene (510 nm,
log ε 3.3).18 A similar spectrum has been observed in several
simple phenyl azides,25 although Harder et al. observed very
little visible absorption during the photolysis of p-nitrophenyl
azide in methyltetrahydrofuran glass.15
In conclusion, the data obtained with a model system
demonstrate both singlet and triplet nitrene reactions through
product studies. This reveals the possibility of trapping the
singlet through an intramolecular reaction, while confirming
that intermolecular trapping in solution is a marginal process.
Likewise, nitro substitution only marginally increases the
radical reactivity of the triplet. The utility of nitrophenyl
azides for photochemical labelling of biomolecules is related to
better complexation with the receptors, which would make the
reaction more similar to the present model - rather than to an
intrinsic change in the reactivity of the nitrene.
Experimental
General
Acetonitrile and 95% ethanol were spectroscopic grade
solvents. Azide 1 was prepared and purified as previously
reported.18c Photoproducts 2 to 5 were likewise previously
reported.18c The photoreactions were monitored by HPLC.
A Jasco PU 980 instrument with UV-975 detector was used,
with a 25 cm × 4.6 mm Merck Purospher RP-18 LiChroCART
250-4 column (and a Purospher RP-18 LiChroCART 4-4
precolumn). Various water–acetonitrile mixtures were used
as the eluent. HPLC/mass experiments (on a Finnigan LCQ
instrument) were used for the detection of trace products (see
below).
Room temperature irradiations
As expected from work with other phenylnitrenes,4,6,15,18 only
triplet chemistry takes place under these conditions, since the
thermal barrier for accessing reactions on the singlet surface
cannot be overcome. Heating of the matrix after irradiation
diminishes the viscosity18 and reproduces a situation similar to
that studied by Schuster by laser photolysis of p-nitrophenyl
azide12 with a relatively high triplet nitrene concentration.
Under this condition dimerization to the azo compound is
the main reaction. On the other hand, maintaining the glass at
95–100 K for a long period of time allows hydrogen abstraction
to take place before the matrix softens to a sufficient degree,
and thus coupling of the triplet is unimportant. The reaction
occurs as a pseudo first order process and cleanly leads to
the amine as shown in Fig. 2, obviously through hydrogen
abstraction from the solvent. Harder et al. reported an inter-
mediate spectrum attributed to the iminyl radical in their matrix
study of p-nitrophenyl azide.15 However, in the present case we
have no evidence for the building up of a significant concen-
tration of an intermediate after the nitrene, although this may
escape detection if, as appears to be the case in the study by
Harder, it has a spectrum quite close to that of the amine. The
nitro group somewhat increases the hydrogen atom abstraction
rate, as judged by the fact that under matrix conditions the
amine is practically the only product obtained, while the azo
still competes (amine–azo ratio ca. 2) with the non-nitrated
pyrazolylphenylnitrene under the same conditions.18b
1 × 10Ϫ4 M Solutions of azide 1 in a 1 cm optical path cell
(2 mL) were irradiated by means of a bifilar low-pressure
mercury arc inserted below the cell (Helios Italquartz 15 W).
More concentrated solutions (4 × 10Ϫ3 M) were irradiated by
means of a focused high-pressure mercury arc (Osram HBO
200W/2; in the MK sensitized experiments a cutoff filter
with λtr > 350 nm was inserted). The product distribution as
determined by HPLC is reported in Table 1. Apart from the
previously reported products 2–5, in the experiments in ethanol
HPLC revealed a further product, with a mass spectrum com-
patible with the structure of 1-(2-ethoxyamino-5-nitrophenyl)-
3,5-dimethyl-1H-pyrazole (6). Tr 13.2 min (1 to 1 MeCN–H2O
mixture, 0.5 ml minϪ1). Mass spectrum: m/z 277 (Mϩ ϩ 1),
231 (base peak), 185 (Mϩ Ϫ EtOH, ϪNO2). In the irradiation
in EtOH with 0.1 M DEA, a further trace peak was detected,
with a spectrum compatible with the structure of 1-[2-(2,2-
diethylhydrazino)-5-nitrophenyl]-3,5-dimethyl-1H-pyrazole (7).
Tr 18.5 min (1 to 1 MeCN–H2O mixture, 0.5 ml minϪ1). Mass
spectrum: m/z 304 (Mϩ ϩ 1), 231 (base peak), 185
(Mϩ Ϫ Et2NH, ϪNO2).
Low temperature experiments
1 × 10Ϫ4 M Solutions of the azide 1 in EtOH (2 mL) in a 1 cm
optical path quartz cell with a quartz to glass graded seal were
degassed by means of four freeze–degas–thaw cycles and
sealed. The cell was inserted into an Oxford DN 1704 liquid
nitrogen cryostat fitted with a calibrated ITC4 temperature
controller and placed in a UV-vis Kontron Uvikon 941
spectrophotometer and irradiated from the bottom as above.
Irradiation was discontinued when taking the spectra. In a
typical experiment, the solution was equilibrated for 30 min
at 90 K and then irradiated for 8 min. After this time the
temperature was either gradually raised (see text and Fig. 2)
In contrast to the various intermolecular channels observed
for triplet nitrene both at high and low temperatures, the
seemingly attractive intramolecular hydrogen abstraction
reaction from the pyrazole methyl group is unimportant. The
formation of quinoxaline is only a minor process. Apparently,
the increase in the radical reactivity of the nitrene induced by
the nitro group is not sufficient to make this reaction channel
effective.
2806
J. Chem. Soc., Perkin Trans. 2, 1999, 2803–2807