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Acryloylnitrenes: Spectroscopic Characterization, Spin Multiplicities, and Rearrangement to Vinyl Isocyanates

机译:丙烯酰基:光谱表征,旋转多样性和对乙烯基异氰酸酯的重排

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摘要

The simplest acryloylnitrene, CH2=CHC(O)N (1b), and two halogenated derivatives, CH2=CFC(O)N (2b) and CH2=CBrC(O)N (3b), were generated through the 266 nm laser photolysis of the corresponding azide precursors in solid N-2-matrices at 15 K. The IR spectroscopic characterization of these new acylnitrenes is supported by N-15-labeling and quantum chemical calculations at the B3LYP/6-311++G(3df,3pd) level of theory. For the three nitrenes 1b, 2b, and 3b, two conformers exhibiting syn and anti configurations between the C=C and C=O bonds with respect to the C-C bonds have been identified. Consistent with the CBS-QB3 calculated singlet-triplet energy gaps (Delta E-ST < 0 kcal mol(-1)), the IR spectral analysis suggests that all these acryloylnitrenes adopt oxazirine-like structures with closed-shell singlet spin multiplicity. Upon subsequent green light (532 nm) irradiation, these acryloylnitrenes rearrange to form vinyl isocyanates CH2=CXNCO (X = H, F, Br), for which the IR spectra have also been obtained. According to the calculations on the alpha,beta-fluorinated acryloylnitrenes at the CBS-QB3 level, their spin multiplicities can be switched from singlet CH2=CFC(O)N (DEBT = -0.86 kcal mol(-1)) to triplet CF2=CFC(O)N (Delta E-ST = +0.61 kcal mol(-1)), whereas CFH=CFC(O)N is magnetically bistable due to a rather small Delta E-ST (+0.09 kcal mol(-1)).
机译:通过266nm激光光解产生最简单的丙烯酰基丙烯,CH2 = CHC(O)N(1b)和两个卤化衍生物CH2 = CFC(O)N(2b)和CH 2 = CBRC(O)N(3b)在15K的固体N-2族基质中的相应叠氮化物前体。通过B3LYP / 6-311 ++ G的N-15标记和量子化学计算支持这些新的酰基尼的IR光谱表征(3DF,3PD )理论水平。对于三个1B,2B和3B,已经鉴定了在C = C和C = O键之间表现出SYN和抗构型相对于C-C键之间的两个相实剂。与CBS-QB3计算出的单次三联能间隙一致(Delta E-ST <0 KCAL(-1)),IR光谱分析表明所有这些丙烯酰基均采用封闭壳单旋转多样性的恶化的类似恶化的结构。在随后的绿光(532nm)照射时,这些丙烯酰肾上腺素重新排列以形成乙烯基异氰酸酯CH 2 = CXNCO(X = H,F,BR),其也得到了IR光谱。根据CBS-QB3水平的α,β-氟化丙烯酰基的计算,它们的旋转多样性可以从单次CH 2 = CFC(O)N(债务= -0.86kcal(-1))转换为Triollet CF2 = CFC(O)N(Delta E-St = + 0.61 kcal mol(-1)),而CFH = CFC(O)N由于相当小的ΔE-ST(+0.09kcal摩尔(-1)而导致磁体双稳态)。

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