Journal of Organic Chemistry p. 6372 - 6381 (2007)
Update date:2022-08-02
Topics:
Klima, Rodney F.
Jadhav, Abhijit V.
Singh, Pradeep N. D.
Chang, Mingxin
Vanos, Christine
Sankaranarayanan, Jagadis
Vu, Mai
Ibrahim, Nazarin
Ross, Elaine
McCloskey, Shaun
Murthy, Rajesh S.
Krause, Jeanette A.
Ault, Bruce S.
Gudmundsdottir, Anna D.
(Chemical Equation Presented) Photolysis of 3-azido-1,3-diphenyl-propan-1- one (1a) in toluene yields 1,3-diphenyl-propen-1-one (2), whereas irradiation of 3-azido-2,2-dimethyl-1,3-diphenyl-propan-1-one (1b) results in the formation of mainly 2,2-dimethyl-1,3-diphenyl-propan-1-one. Laser flash photolysis (308 nm) of 1a,b in acetonitrile reveals a transient absorption (λmax = ~310 nm) due to the formation of radicals 4a and 4b, respectively, which have lifetimes of ~14 μs at ambient temperature. TD-DFT calculations (B3LYP/6-31+G(d)) reveal that the first and second excited states of the triplet ketone (T1K (n,π*) and T2K (π,π*)) in azide 1a are almost degenerate, at ~74 and 76 kcal/mol above the ground state (S0), respectively. Similarly, azide 1b has T1K and T2K 75 and 82 kcal/mol above S0, respectively. The calculated transition state for cleaving the C-N bond is located 71 and 74 kcal/mol above S0 in azides 1a and 1b, respectively. The calculated bond dissociation energies for breaking the C-N bond are 55 and 58 kcal/mol for azides 1a and 1b, respectively, making C-N bond breakage accessible from T 1K in azides 1 at ambient temperature. In comparison, the irradiation of azides 1 in argon matrices at 14 K lead to the formation of the corresponding triplet alkyl nitrenes (1-n), via intramolecular energy transfer from T2K- The characterization of 1-n was supported by isotope labeling, IR spectroscopy, and molecular modeling.
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