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Theory of damped quantum rotation in nuclear magnetic resonance spectra. III. Nuclear permutation symmetry of the line shape equation

机译:核磁共振光谱中阻尼量子旋转的理论。三,线形方程的核置换对称性

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The damped quantum rotation (DQR) theory describes manifestations in nuclear magnetic resonance spectra of the coherent and stochastic dynamics of N-fold molecular rotors composed of indistinguishable particles. The standard jump model is only a limiting case of the DQR approach; outside this limit, the stochastic motions of such rotors have no kinematic description. In this paper, completing the previous two of this series, consequences of nuclear permutation symmetry for the properties of the DQR line shape equation are considered. The systems addressed are planar rotors, such as aromatic hydrocarbons’ rings, occurring inside of molecular crystals oriented in the magnetic field. Under such conditions, oddfold rotors can have nontrivial permutation symmetries only for peculiar orientations while evenfold ones always retain their intrinsic symmetry element, which is rotation by 180° about the N-fold axis; in specific orientations the latter can gain two additional symmetry elements. It is shown that the symmetry selection rules applicable to the classical rate processes in fluids, once recognized as having two diverse aspects, macroscopic and microscopic, are also rigorously valid for the DQR processes in the solid state. However, formal justification of these rules is different because the DQR equation is based on the Pauli principle, which is ignored in the jump model. For objects like the benzene ring, exploitation of these rules in imulations of spectra using the DQR equation can be of critical significance for the feasibility of the calculations. Examples of such calculations for the proton system of the benzene ring in a general orientation are provided. It is also shown that, because of the intrinsic symmetries of the evenfold rotors, many of the DQR processes, which such rotors can undergo, are unobservable in NMR spectra.
机译:阻尼量子旋转(DQR)理论描述了在核磁共振波谱中由不可区分的粒子组成的N折叠分子转子的相干和随机动力学的表现形式。标准跳跃模型只是DQR方法的一个限制情况;在该极限之外,这种转子的随机运动没有运动学描述。本文完成了本系列的前两个部分,考虑了核排列对称性对DQR线形方程的性质的影响。所解决的系统是平面转子,例如芳烃环,出现在磁场中定向的分子晶体内部。在这种情况下,奇数转子只能对特殊的方向具有非平凡的排列对称性,而偶数转子则始终保持其固有的对称性,即绕N轴旋转180°。在特定方向上,后者可以获得两个额外的对称元素。结果表明,适用于流体中经典速率过程的对称选择规则,一旦被认为具有宏观和微观两个不同方面,也对固态的DQR过程严格地有效。但是,这些规则的形式合理性是不同的,因为DQR方程基于Pauli原理,在跳跃模型中将其忽略。对于像苯环这样的物体,在使用DQR方程的光谱模拟中利用这些规则对于计算的可行性至关重要。提供了用于一般取向的苯环的质子系统的这种计算的示例。还表明,由于偶数折叠转子的固有对称性,在NMR光谱中无法观察到许多此类转子可能经历的DQR过程。

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