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J Phys Chem B. 2022 Feb 17;126(6):1202-1211. doi: 10.1021/acs.jpcb.1c10131. Epub 2022 Feb 5.

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Chempluschem. 2016 Aug;81(8):836-841. doi: 10.1002/cplu.201600176. Epub 2016 May 25.
2
Capture of nitrogen dioxide and conversion to nitric acid in a porous metal-organic framework.在多孔金属有机骨架中捕获二氧化氮并将其转化为硝酸。
Nat Chem. 2019 Dec;11(12):1085-1090. doi: 10.1038/s41557-019-0356-0. Epub 2019 Nov 22.
3
Reducing bias in the analysis of solution-state NMR data with dynamics detectors.利用动力学探测器减少溶液态 NMR 数据分析中的偏倚。
J Chem Phys. 2019 Jul 21;151(3):034102. doi: 10.1063/1.5111081.
4
Separating out the middle.分离中间部分。
Nat Mater. 2019 Sep;18(9):910-911. doi: 10.1038/s41563-019-0437-x.
5
Stochastic modeling of macromolecules in solution. I. Relaxation processes.溶液中大分子的随机建模。I. 弛豫过程。
J Chem Phys. 2019 May 14;150(18):184107. doi: 10.1063/1.5077065.
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Stochastic modeling of macromolecules in solution. II. Spectral densities.溶液中大分子的随机建模。II. 谱密度。
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Solid-state NMR reveals a comprehensive view of the dynamics of the flexible, disordered N-terminal domain of amyloid-β fibrils.固态 NMR 揭示了淀粉样β纤维中柔性、无规的 N 端结构域动力学的全面视图。
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Phenyl-Ring Dynamics in Amyloid Fibrils and Proteins: The Microscopic-Order-Macroscopic-Disorder Perspective.芳环动力学在淀粉样纤维和蛋白质中的研究:微观有序-宏观无序的观点。
J Phys Chem B. 2018 Sep 20;122(37):8675-8684. doi: 10.1021/acs.jpcb.8b06330. Epub 2018 Sep 10.
10
MOMD Analysis of NMR Line Shapes from Aβ-Amyloid Fibrils: A New Tool for Characterizing Molecular Environments in Protein Aggregates.NMR 线谱的 MOMD 分析:一种用于鉴定蛋白聚集物中分子环境的新工具。
J Phys Chem B. 2018 May 10;122(18):4793-4801. doi: 10.1021/acs.jpcb.8b02181. Epub 2018 May 2.

固态核磁共振结构动力学:应用于互锁分子有机框架的统一 MOMD 视角。

Structural Dynamics by NMR in the Solid State: The Unified MOMD Perspective Applied to Organic Frameworks with Interlocked Molecules.

机构信息

The Mina and Everard Goodman Faculty of Life Sciences, Bar-Ilan University, Ramat-Gan 52900 Israel.

Baker Laboratory of Chemistry and Chemical Biology, Cornell University, Ithaca, New York 14853-1301, United States.

出版信息

J Phys Chem B. 2020 Jul 23;124(29):6225-6235. doi: 10.1021/acs.jpcb.0c03687. Epub 2020 Jul 14.

DOI:10.1021/acs.jpcb.0c03687
PMID:32584038
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7666760/
Abstract

The microscopic-order-macroscopic-disorder (MOMD) approach for NMR lineshape analysis has been applied to the University of Windsor Dynamic Materials (UWDM) of types 1, 2, α-3, β-3, and 5, which are metal-organic frameworks (MOFs) comprising mobile mechanically interlocked molecules (MIMs). The mobile MIM components are selectively deuterated crown ether macrocycles - 24C6, 22C6, and B24C6. Their motion is described in MOMD by an effective/collective dynamic mode characterized by a diffusion tensor, , a restricting/ordering potential, , expanded in the Wigner rotation matrix elements, , and features of local geometry. Experimental H lineshapes are available over 220 K (on average) and in some cases 320 K. They are reproduced with axial , given by the terms and , and established local geometry. For UWDM of types 1, β-3, and 5, where the macrocycle resides in a relatively loose space, is in the 1-3 , in the (1.0-2.5) × 10 s, and in the (0.4-2.5) × 10 s range; the deuterium atom is bonded to a carbon atom with tetrahedral coordination character. For UWDM of types 2 and α-3, where the macrocycle resides in a much tighter space, a substantial change in the symmetry of and the coordination character of the H-bonded carbon are detected at higher temperatures. The activation energies for and are characteristic of each system. The MOMD model is general; effective/collective dynamic modes are treated. The characteristics of motion, ordering, and geometry are physically well-defined; they differ from case to case in extent and symmetry but not in essence. Physical clarity and consistency provide new insights. A previous interpretation of the same experimental data used models consisting of collections of independent simple motions. These models are specific to each case and temperature. Within their scope, generating consistent physical pictures and comparing cases are difficult; possible collective modes are neglected.

摘要

用于 NMR 线宽分析的微观-宏观-无序 (MOMD) 方法已应用于温莎大学动态材料 (UWDM) 1 型、2 型、α-3 型、β-3 型和 5 型,这些材料是由可移动的机械互锁分子 (MIM) 组成的金属有机骨架 (MOF)。可移动的 MIM 成分是选择性氘化的冠醚大环 - 24C6、22C6 和 B24C6。它们的运动在 MOMD 中由以扩散张量 、 为特征的有效/集体动态模式来描述, 是在 Wigner 旋转矩阵元素 中展开的限制/有序势, 并具有局部几何特征。实验 H 线宽可在 220 K(平均)以上,在某些情况下可达 320 K。它们通过轴向 来重现, 由项 和 给出,以及已建立的局部几何形状。对于 UWDM 1 型、β-3 型和 5 型,大环位于相对宽松的空间中, 在 1-3 范围内, 在(1.0-2.5)×10 s 范围内, 在(0.4-2.5)×10 s 范围内;氘原子与具有四面体配位特征的碳原子键合。对于 UWDM 2 型和 α-3 型,大环位于更紧凑的空间中,在较高温度下检测到 和氢键合碳原子的对称性以及配位特征发生了实质性变化。 和 的活化能是每个系统的特征。MOMD 模型是通用的;处理有效/集体动态模式。运动、有序和几何的特征在物理上是明确定义的;它们在程度和对称性上因情况而异,但在本质上没有区别。物理清晰度和一致性提供了新的见解。对相同实验数据的先前解释使用了由独立简单运动集合组成的模型。这些模型是特定于每个案例和温度的。在其范围内,生成一致的物理图像和比较案例是困难的;可能的集体模式被忽略了。