Jove
Visualize
Contact Us

Related Concept Videos

¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

1.7K
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...
1.7K
NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

3.6K
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...
3.6K
NMR Spectrometers: Resolution and Error Correction01:14

NMR Spectrometers: Resolution and Error Correction

1.1K
When magnetic nuclei in a sample achieve resonance and undergo relaxation, the signal detected in NMR is an approximately exponential free induction decay. Fourier transform of an exponential decay yields a Lorentzian peak in the frequency domain. Lorentzian peaks in an NMR spectrum are defined by their amplitude, full width at half maximum, and position, where the peak width is governed by the spin-spin relaxation time alone. In real experiments, however, the applied magnetic field is rendered...
1.1K
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.6K
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,...
1.6K
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

1.6K
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...
1.6K
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)

1.9K
Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
1.9K

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Breakdown of Disorder-Suppressed Floquet Heating under Two-Frequency Driving.

Physical review letters·2026
Same author

Gas-phase spectroscopy of H<sub>2</sub>O@C<sub>60</sub><sup>+</sup> and H<sub>2</sub>O@C<sub>60</sub>H<sup>+</sup> in the mid-infrared: the challenges of searching for endohedral fullerenes in space.

Physical chemistry chemical physics : PCCP·2026
Same author

Spinor double-quantum excitation in the solution NMR of near-equivalent spin-1/2 pairs.

The Journal of chemical physics·2026
Same author

Terahertz spectroscopy study of the confining potential for methane in the endofullerene CH4@C60.

The Journal of chemical physics·2025
Same author

Singlet NMR in a case of high molecular symmetry.

The Journal of chemical physics·2025
Same author

<sup>1</sup>H-enhanced <sup>103</sup>Rh NMR spectroscopy and relaxometry of <sup>103</sup>Rh(acac)<sub>3</sub> in solution.

Magnetic resonance (Gottingen, Germany)·2025
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Experiment Video

Updated: Mar 25, 2026

Author Spotlight: Exploring Intrinsically Disordered Protein Dynamics Through NMR Relaxation Experiments
09:25

Author Spotlight: Exploring Intrinsically Disordered Protein Dynamics Through NMR Relaxation Experiments

Published on: November 1, 2024

2.9K

Error Compensation without a Time Penalty: Robust Spin-Lock-Induced Crossing in Solution NMR.

Mohamed Sabba1, Christian Bengs1, Urvashi D Heramun1

  • 1School of Chemistry and Chemical Engineering, University of Southampton, Southampton SO17 1BJ, United Kingdom.

The Journal of Physical Chemistry Letters
|March 23, 2026
PubMed
Summary

A new compensated spin-lock-induced crossing (cSLIC) method improves nuclear magnetic resonance (NMR) for complex spin systems. This technique enhances accuracy in singlet NMR and hyperpolarized NMR experiments without extending experiment time.

More Related Videos

Spin Saturation Transfer Difference NMR SSTD NMR: A New Tool to Obtain Kinetic Parameters of Chemical Exchange Processes
11:44

Spin Saturation Transfer Difference NMR SSTD NMR: A New Tool to Obtain Kinetic Parameters of Chemical Exchange Processes

Published on: November 12, 2016

18.7K
Practical Aspects of Sample Preparation and Setup of 1H R1&#961; Relaxation Dispersion Experiments of RNA
08:17

Practical Aspects of Sample Preparation and Setup of 1H R1ρ Relaxation Dispersion Experiments of RNA

Published on: July 9, 2021

5.3K

Related Experiment Videos

Last Updated: Mar 25, 2026

Author Spotlight: Exploring Intrinsically Disordered Protein Dynamics Through NMR Relaxation Experiments
09:25

Author Spotlight: Exploring Intrinsically Disordered Protein Dynamics Through NMR Relaxation Experiments

Published on: November 1, 2024

2.9K
Spin Saturation Transfer Difference NMR SSTD NMR: A New Tool to Obtain Kinetic Parameters of Chemical Exchange Processes
11:44

Spin Saturation Transfer Difference NMR SSTD NMR: A New Tool to Obtain Kinetic Parameters of Chemical Exchange Processes

Published on: November 12, 2016

18.7K
Practical Aspects of Sample Preparation and Setup of 1H R1&#961; Relaxation Dispersion Experiments of RNA
08:17

Practical Aspects of Sample Preparation and Setup of 1H R1ρ Relaxation Dispersion Experiments of RNA

Published on: July 9, 2021

5.3K

Area of Science:

  • Nuclear Magnetic Resonance (NMR) Spectroscopy
  • Quantum Information Science
  • Chemical Physics

Background:

  • The spin-lock-induced crossing (SLIC) is a standard technique in solution Nuclear Magnetic Resonance (NMR).
  • Strongly coupled nuclear spin systems present challenges for traditional NMR methods.
  • Existing SLIC protocols can be sensitive to radio-frequency field imperfections.

Purpose of the Study:

  • To introduce a modified SLIC procedure, termed compensated SLIC (cSLIC), for improved NMR of strongly coupled spin systems.
  • To enhance the robustness of SLIC against radio-frequency field amplitude variations.
  • To apply cSLIC to singlet NMR and parahydrogen-enhanced hyperpolarized NMR experiments.

Main Methods:

  • Development of the compensated-SLIC (cSLIC) sequence utilizing a repetitive element with two distinct radio-frequency field amplitudes.
  • Implementation of effective compensation mechanisms for radio-frequency field amplitude deviations.
  • Validation through numerical simulations and experimental execution on relevant NMR systems.

Main Results:

  • The cSLIC scheme effectively compensates for radio-frequency field amplitude errors.
  • Compensation is achieved without increasing the total duration of the SLIC sequence.
  • Demonstrated advantageous properties of cSLIC in simulations and experiments for challenging NMR scenarios.

Conclusions:

  • The cSLIC technique offers a significant improvement over standard SLIC for strongly coupled spin systems.
  • This method enhances the reliability and applicability of NMR for specialized techniques like singlet NMR and hyperpolarized NMR.
  • cSLIC provides a robust and efficient solution for overcoming experimental imperfections in NMR.