Photolysis of Moꢀ and Wꢀcontaining complexes
Russ.Chem.Bull., Int.Ed., Vol. 57, No. 2, February, 2008
291
600 nm was 8700 s–1. By analogy to the isoelectronic
tungsten complex, this constant is the rate constant for
the addition of the first N2 molecule to the coordinatively
unsaturated Mo(DPPE)2 species. Note that the ratio of
the rate constants for the addition of the first N2 molecule
to the isoelectronic coordinatively unsaturated M(DPPE)2
species for Mo and W is 43.
Thus, the irradiation of the phosphine hydride (MH4L4)
or phosphine nitrogen (transꢀM(N2)2L4) complexes of Mo
and W in the region λ < 350 nm results in the elimination
of two H2 or two N2 molecules, respectively, to form the
primary coordinatively unsaturated ML4 species characꢀ
terized by the longꢀwavelength absorption bands with
D500
–lnD500
7
0.08
6
2
1
0.06
0.04
0.02
5
4
3
2
0.3
0.4
0.5
0.6
Time/ms
λ
max 450—460 nm.
Fig. 5. Pulse photolysis of a nitrogenꢀsaturated benzene solution
of transꢀMo(N2)2(DPPE)2 at 300 K: kinetics of changes in the
absorbance at λ = 500 nm (D500) after a photolyzing pulse (1);
lnD500 (2).
The author is grateful to V. A. Nadtochenko for help
in pulse measurements by a nanosecond laser pulse phoꢀ
tolysis technique.
For the pulse photolysis of transꢀW(N2)2(DPPE)2 in
benzene at room temperature, a longꢀwavelength band at
400—600 nm appears in the absorption spectrum of the
solution after a pulse with λ = 354 nm. In this case, as shown in
Fig. 4, the absorbance at λ = 550 nm decays exponentially
References
1. A. P. Pivovarov, Yu. V. Gak, Yu. M. Shulґga, V. D. Makhaev,
A. P. Borisov, Yu. G. Borod´ko, Izv. Akad. Nauk SSSR, Ser.
Khim., 1979, 2590 [Bull. Acad. Sci. USSR, Div. Chem. Sci.,
1979, 28 (Engl. Transl.)].
in an N2 atmosphere with the rate constant k = 200 s–1
.
It is known10 that after a photolyzing pulse of the
nitrogenꢀsaturated solution of transꢀW(N2)2(DPPE)2 in
THF the absorbance decreases at λ = 300 nm, i.e., in the
maximum of the electronic chargeꢀtransfer transition from
tungsten to nitrogen. After a pulse the absorbance at λ =
300 nm is recovered in the twoꢀstep process with the rate
constants k1 = 390 s–1 and k2 = 1.6 s–1. The results obꢀ
tained can be explained10 by the formation from transꢀ
W(N2)2(DPPE)2 (after a pulse) of the coordinatively unꢀ
saturated W(DPPE)2 species followed by their twoꢀstep
interaction with N2 to form W(N2)(DPPE)2 in the first
step, whereas transꢀW(N2)2(DPPE)2 is formed in the secꢀ
ond step. The obtained rate constant for the decay of the
longꢀwavelength absorption band appeared during
the pulse photolysis of transꢀW(N2)2(DPPE)2 in benzene
(k = 200 s–1) is close to the rate constant for the addition
of the first N2 molecule to the coordinatively unsaturated
W(DPPE)2 species in THF (k1 = 390 s–1). Based on our
experimental results and known literature data, one may
conclude that the longꢀwavelength absorption band at
400—600 nm, which appears after the pulse photolysis
of transꢀW(N2)2(DPPE)2 in benzene, belongs to the
W(DPPE)2 coordinatively unsaturated species. For
the pulse photolysis of a benzene solution of transꢀ
Mo(N2)2(DPPE)2 under N2 at 300 K, the absorbance at
λ = 500 nm decays exponentially (Fig. 5). Similar patterns
were also observed for the absorbances at λ = 400 and 600 nm.
The average rate constant for the decay of the longꢀwaveꢀ
length absorption band (k) measured at λ = 400, 500, and
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Received June 27, 2006;
in revised form October 3, 2007