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Related Concept Videos

Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...
Atomic Nuclei: Nuclear Spin01:08

Atomic Nuclei: Nuclear Spin

All atomic particles possess an intrinsic angular momentum, or 'spin'. Electrons, protons, and neutrons each have a spin value of ½, although protons and neutrons in nuclei may have higher half-integer spins owing to energetic factors.
Atomic nuclei have a net nuclear spin, , which can have an integer or half-integer value. In atomic nuclei, the spins of protons are paired against each other but not with neutrons, and vice versa. Consequently, an even number of protons does not contribute to...
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must have a...
Atomic Nuclei: Nuclear Magnetic Moment00:59

Atomic Nuclei: Nuclear Magnetic Moment

All atomic nuclei are positively charged. When they have a nonzero spin, they behave like rotating charges. As a consequence of their charge and spin, these nuclei generate a magnetic field (B). This, in turn, gives rise to a magnetic moment (μ), which is randomly oriented in the absence of an external magnetic field. When an external magnetic field (B0) is applied, the magnetic moment vectors can align with the field or against it in 2 + 1 orientations. A hydrogen nucleus, which is just a...
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

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 in...

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Related Experiment Video

Updated: May 27, 2026

In Situ Monitoring of Diffusion of Guest Molecules in Porous Media Using Electron Paramagnetic Resonance Imaging
06:34

In Situ Monitoring of Diffusion of Guest Molecules in Porous Media Using Electron Paramagnetic Resonance Imaging

Published on: September 2, 2016

A first-principles description of proton-driven spin diffusion.

Jean-Nicolas Dumez1, Meghan E Halse, Mark C Butler

  • 1Université de Lyon (ENS Lyon/CNRS/UCB Lyon1), Centre de RMN à très hauts champs, 5 rue de la Doua, 69100 Villeurbanne, France.

Physical Chemistry Chemical Physics : PCCP
|November 17, 2011
PubMed
Summary
This summary is machine-generated.

We developed a new simulation method for proton-driven spin diffusion. This approach accurately predicts carbon-13 polarization transfer in solid-state nuclear magnetic resonance experiments using crystal structure data.

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Area of Science:

  • Solid-state Nuclear Magnetic Resonance (NMR) spectroscopy
  • Computational chemistry
  • Quantum mechanics

Background:

  • Proton-driven spin diffusion is a key mechanism for polarization transfer in solid-state NMR.
  • Accurate simulation of this process is crucial for interpreting experimental data and understanding molecular dynamics.
  • Previous methods often required empirical adjustments or were computationally intensive.

Purpose of the Study:

  • To design a novel computational approach for simulating proton-driven spin diffusion.
  • To quantitatively describe experimental observations of carbon-13 polarization transfer.
  • To validate the simulation method using crystal geometry without adjustable parameters.

Main Methods:

  • Development of a reduced Liouville space representation for spin dynamics.
  • Implementation of the simulation approach based on first principles.
  • Application to a powder sample undergoing magic-angle spinning.

Main Results:

  • The reduced Liouville space approach accurately reproduces experimentally observed carbon-13 polarization transfer.
  • Quantitative agreement is achieved directly from crystal geometry.
  • No adjustable parameters were required for the simulation.

Conclusions:

  • The developed simulation method provides a powerful and accurate tool for studying spin diffusion in solid-state NMR.
  • This approach simplifies the interpretation of complex NMR experiments.
  • It opens new avenues for structure determination and dynamic studies using NMR.