通过随机步行在相位空间中揭示相位和时间合对NMR放松率的影响
1Carlson School of Chemistry and Biochemistry, Clark University, Worcester, Massachusetts 01610, USA.
Physical review. E
|October 18, 2023
概括
阶段时间合通过修改光谱密度频率,显著影响核磁共振 (NMR) 放松. 这种新模型成功地适应了传统理论失败的实验数据,揭示了更快的细分运动动态.
科学领域:
- 物理 物理学 物理
- 化学 化学 化学
- 材料科学 材料科学 材料科学
背景情况:
- 阶段时间合是旋转系统中的自然现象.
- 它对核磁共振 (NMR) 放松的影响挑战了现有的理论,如二次量子扰动理论.
研究的目的:
- 扩展相扩散方法,以考虑NMR放松中的相时合效应.
- 研究相时合对NMR放松率和动态的影响.
主要方法:
- 利用未合的相扩散和合的随机走路.
- 使用旋转随机场的瞬间投影来确定累积相位.
- 在静态和旋转框架中导出相位扩散系数.
主要成果:
- 阶段时间合将光谱密度角频率 (ω) 修改为明显频率 (ηω),其中 η 是阶段时间合常数.
- 最强合 (η=2) 与传统结果 (η=1) 不一致.
- 修改后的放松时间表达式与传统模型不同,适合用于聚乙烯混合物的实验性NMR数据.
结论:
- 阶段时间合对于准确的NMR放松分析至关重要,特别是对于复杂的系统.
- 开发的模型更好地适应实验数据,表明细分运动比先前估计的更快.
相关概念视频
Atomic Nuclei: Types of Nuclear Relaxation
310
Nuclear relaxation restores the equilibrium population imbalance and can occur via spin–lattice or spin–spin mechanisms, which are first-order exponential decay processes.
In spin–lattice or longitudinal relaxation, the excited spins exchange energy with the surrounding lattice as they return to the lower energy level. Among several mechanisms that contribute to spin–lattice relaxation, magnetic dipolar interactions are significant. Here, the excited nucleus transfers...
In spin–lattice or longitudinal relaxation, the excited spins exchange energy with the surrounding lattice as they return to the lower energy level. Among several mechanisms that contribute to spin–lattice relaxation, magnetic dipolar interactions are significant. Here, the excited nucleus transfers...
310
¹H NMR of Conformationally Flexible Molecules: Temporal Resolution
868
At room temperature, the chair conformer of cyclohexane undergoes rapid ring flipping between two equivalent chair conformers at a rate of approximately 105 times per second. These two chair conformers are in equilibrium. The rapid ring flipping results in the interconversion of the axial proton to an equatorial proton and an equatorial to the axial proton. Such interconversions are too rapid and cannot be detected on the NMR timescale. Hence, the NMR spectrometer cannot distinguish between the...
868
¹H NMR: Interpreting Distorted and Overlapping Signals
1.0K
Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
1.0K
¹H NMR: Long-Range Coupling
1.8K
The coupling interactions of nuclei across four or more bonds are usually weak, with J values less than 1 Hz. While these are usually not observed in spectra, the presence of multiple bonds along the coupling pathway can result in observable long-range coupling.
In alkenes, spin information is communicated via σ–π overlap, as seen in allylic (four-bond) and homoallylic (five-bond) couplings. These coupling interactions are stronger when the σ bond is parallel to the alkene...
In alkenes, spin information is communicated via σ–π overlap, as seen in allylic (four-bond) and homoallylic (five-bond) couplings. These coupling interactions are stronger when the σ bond is parallel to the alkene...
1.8K
NMR Spectroscopy: Spin–Spin Coupling
1.4K
The spin state of an NMR-active nucleus can have a slight effect on its immediate electronic environment. This effect propagates through the intervening bonds and affects the electronic environments of NMR-active nuclei up to three bonds away; occasionally, even farther. This phenomenon is called spin–spin coupling or J-coupling. Coupling interactions are mutual and result in small changes in the absorption frequencies of both nuclei involved. While nuclei of the same element are involved...
1.4K
Atomic Nuclei: Nuclear Relaxation Processes
660
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
660


