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, Gudmundsdóttir Anna D
Department of Chemistry, University of Cincinnati, Cincinnati, Ohio 45221-0172, USA.
J Org Chem. 2007 Aug 17;72(17):6372-81. doi: 10.1021/jo070558q. Epub 2007 Jul 27.
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 (lambda max = approximately 310 nm) due to the formation of radicals 4a and 4b, respectively, which have lifetimes of approximately 14 micros 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,pi*) and T2K (pi,pi*)) in azide 1a are almost degenerate, at approximately 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 T1K 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.
3-叠氮基-1,3-二苯基-丙-1-酮(1a)在甲苯中的光解产生1,3-二苯基-丙烯-1-酮(2),而3-叠氮基-2,2-二甲基-1,3-二苯基-丙-1-酮(1b)的辐照主要导致2,2-二甲基-1,3-二苯基-丙-1-酮的形成。1a、b在乙腈中的激光闪光光解(308nm)显示由于分别形成自由基4a和4b而产生瞬态吸收(λmax≈310nm),在环境温度下其寿命约为14微秒。TD-DFT计算(B3LYP/6-31+G(d))表明,叠氮化物1a中三重态酮(T1K(n,π*)和T2K(π,π*))的第一和第二激发态几乎简并,分别比基态(S0)高约74和76kcal/mol。类似地,叠氮化物1b的T1K和T2K分别比S0高75和82kcal/mol。在叠氮化物1a和1b中,计算得出的C-N键断裂的过渡态分别比S0高71和74kcal/mol。对于叠氮化物1a和1b,计算得出的C-N键断裂的键解离能分别为55和58kcal/mol,使得在环境温度下从叠氮化物1中的T1K可以实现C-N键的断裂。相比之下,叠氮化物1在14K的氩气基质中的辐照通过从T2K的分子内能量转移导致相应的三重态烷基氮烯(1-n)的形成。1-n的表征得到了同位素标记、红外光谱和分子模拟的支持。