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NMR 揭示多晶卟吩中同位素和相效应对质子互变异构的影响。

Isotope and phase effects on the proton tautomerism in polycrystalline porphycene revealed by NMR.

机构信息

Institut für Chemie und Biochemie, Takustrasse 3, Freie Universität Berlin, D-14195 Berlin, Germany.

出版信息

J Phys Chem A. 2009 Mar 12;113(10):2193-206. doi: 10.1021/jp8079414.

DOI:10.1021/jp8079414
PMID:19093846
Abstract

Using high resolution solid state (15)N and (2)H spectroscopy and longitudinal relaxometry we have studied the tautomerism of porphycene in the solid state, corresponding to a double proton transfer in two cooperative hydrogen bonds. The tautomerism is degenerate above 225 K but the degeneracy is lifted below this temperature, indicating a phase transition. Thus, the high-temperature phase is characterized by a dynamic proton disorder and the low-temperature phase by a dynamic proton order. (15)N magnetization transfer experiments obtained under cross polarization (CP) and magic angle spinning (MAS) conditions reveal the presence of two nonequivalent molecules A and B in the unit cell of phase II, exhibiting slightly different equilibrium constants of the tautomerism. Rate constants of the tautomerism in phase I could be obtained by the analysis of the longitudinal (15)N and (2)H relaxation times. The former, obtained at 9.12 MHz, exhibit a T(1) minimum around 270 K and are consistent with proton transfer induced dipolar (1)H-(15)N relaxation mechanism. The latter, obtained at 46.03 MHz, exhibit a minimum around 330 K and arise from quadrupole relaxation. Within the margin of error, the rate constants of the HH and of the HD/DD tautomerism are the same, exhibiting a barrier of about 30 kJ mol(-1), as expected for an overbarrier reaction in a configuration with two compressed hydrogen bonds. By contrast, in the low-temperature phase a switch of the DD transfer kinetics into the nanosecond time scale is observed, exhibiting a non-Arrhenius temperature dependence which is typical for tunneling. This increase of the rate constants by lowering the temperature is discussed in terms of a switch from a concerted HH transfer in phase I to a stepwise transfer in phase II, where intermolecular interactions lower the energy of one of the cis-intermediates.

摘要

使用高分辨率固态 (15)N 和 (2)H 波谱和纵向弛豫率,我们研究了卟吩在固态中的互变异构,这对应于两个协同氢键中的双重质子转移。互变异构在 225 K 以上是简并的,但在低于此温度时简并被解除,表明发生了相变。因此,高温相的特征是质子动态无序,低温相的特征是质子动态有序。在交叉极化 (CP) 和魔角旋转 (MAS) 条件下获得的 (15)N 磁化转移实验表明,在 II 相的晶胞中存在两个非等价的分子 A 和 B,它们的互变异构平衡常数略有不同。通过分析纵向 (15)N 和 (2)H 弛豫时间,可以获得 I 相互变异构的速率常数。在 9.12 MHz 下获得的前者在 270 K 左右表现出 T(1)最小值,并且与质子转移诱导的偶极 (1)H-(15)N 弛豫机制一致。在 46.03 MHz 下获得的后者在 330 K 左右表现出最小值,这是由四极弛豫引起的。在误差范围内,HH 和 HD/DD 互变异构的速率常数相同,表现出约 30 kJ mol(-1)的势垒,这与具有两个压缩氢键的构型中的过势垒反应一致。相比之下,在低温相中,DD 转移动力学切换到纳秒时间尺度,表现出非 Arrhenius 温度依赖性,这是隧道的典型特征。通过降低温度来增加速率常数的现象可以通过从 I 相的协同 HH 转移切换到 II 相的分步转移来解释,其中分子间相互作用降低了一个顺式中间体的能量。

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