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FIGURE 1.2. Transient absorption spectra produced by 266 nm photolysis of o -biphenylyl
azide in acetonitrile at ambient temperature with time windows of (a) 0.3-1.3 ps and (b) 2-
500 ps. Source : Reprinted with permission from Ref. 26.
As expected, relaxed singlet nitrene 1 p -BpN does not exhibit any significant
population decay on the 100 ps timescale (
9 ns). 28 However, the transient
absorption spectrum of the initially formed singlet nitrene ( 1 p -BpN) undergoes
vibrational cooling (VC) 36-39 (Fig. 1.1b), which manifests as a decay on the red edge
(380 nm) and a rise on the blue edge (345 nm) of the absorption band with the same
time constant (
t
t ΒΌ
11 ps). The time-dependent band narrowing is characteristic of
vibrational cooling of species initially formed with excess vibrational energy. A
derivative of 1 o -BpN, 3,5-dichloro- ortho -biphenyl nitrene also undergoes vibra-
tional cooling in cyclohexane with a time constant of 11 ps. 40 Furthermore, in a
related ultrafast study of 2-fluorenyl azide, a similar spectral evolution was also
observed. 41 This rules out the possibility that the spectral changes are due to rotation
around the C
C bond of the biphenyl moiety.
1 o -BpN decays with a time constant of 16
3 ps (Fig. 1.2b). The 16 ps time
constant represents the population decay of the singlet nitrene ( 1 o -BpN) by
isomerization to both isocarbazole and a benzazirine (and subsequently the benza-
zirine ring expands to form a 1,2-didehydroazepine, Scheme 1.2). The spectrum of
1 o -BpN does not undergo reshaping characteristic of vibrational cooling, even
though the decay of
1 o -BpN takes place on the timescale of vibrational cooling.
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