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Photolysis of (3-methyl-2H-azirin-2-yl)-phenylmethanone: Direct detection of a triplet vinylnitrene intermediate

The photoreactivity of (3-methyl-2H-azirin-2-yl)-phenylmethanone, 1, is wavelength-dependent (Singh et al. J. Am. Chem. Soc. 1972, 94, 1199-1206). Irradiation at short wavelengths yields 2P, whereas longer wavelengths produce 3P. Laser flash photolysis of 1 in acetonitrile using a 355 nm laser forms its triplet ketone (T1K, broad absorption with lambdamax ? 390-410 nm, tau ? 90 ns), which cleaves and yields triplet vinylnitrene 3 (broad absorption with lambdamax ? 380-400 nm, tau = 2 mus). Calculations (B3LYP/6-31+G(d)) reveal that T1K of 1 is located 67 kcal/mol above its ground state (S0) and has a long C-N bond (1.58 A), and the calculated transition state to form 3 is only 1 kcal/mol higher in energy than T1K of 1. The calculations show that 3 has significant 1,3-carbon iminyl biradical character, which explains why 3 reacts efficiently with oxygen and decays by intersystem crossing to the singlet surface. Photolysis of 1 in argon matrixes at 14 K produced ketene imine 7, which presumably is formed from 3 intersystem crossing to 7. In comparison, photolysis of 1 in methanol with a 266 nm laser produces mainly ylide 2 (lambdamax ? 380 nm, tau ? 6 mus, acetonitrile), which decays to form 2P. Ylide 2 is formed via singlet reactivity of 1, and calculations show that the first singlet excited state of the azirine chromophore (S1A) is located 113 kcal/mol above its S0 and that the singlet excited state of the ketone (S1K) is 85 kcal/mol. Furthermore, the transition state for cleaving the C-C bond in 1 to form 2 is located 49 kcal/mol above the S0of 1. Thus, we theorize that internal conversion of S1A to a vibrationally hot S0 of 1 forms 2, whereas intersystem crossing from S1K to T1K results in 3.

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Reference£º
Isoxazole – Wikipedia,
Isoxazole | C3H3NO – PubChem