Jove
Visualize
Contact Us
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 Concept Videos

Electron Paramagnetic Resonance (EPR) Spectroscopy: Organic Radicals01:17

Electron Paramagnetic Resonance (EPR) Spectroscopy: Organic Radicals

2.4K
Ideally, an unpaired electron shows a single peak in the EPR spectrum due to the transition between the two spin energy states. However, coupling interactions can occur between the spins of the unpaired electron and any neighboring spin-active nuclei. This hyperfine coupling results in hyperfine splitting, where the EPR signal is split into multiplets. The signals split into 2nI + 1 peaks, where n is the number of equivalent nuclei and I is the nuclear spin. These splitting patterns provide...
2.4K
NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences01:17

NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences

779
A pulse is a short burst of radio waves distributed over a range of frequencies that simultaneously excites all the nuclei in the sample. Upon passing a radio frequency pulse along the x-axis, the nuclei absorb energy corresponding to their Larmor frequencies and achieve resonance. This shifts the net magnetization vector from the z-axis toward the transverse plane. This angle of rotation of the magnetization vector, or the flip angle, is proportional to the duration and intensity of the pulse.
779
NMR Spectrometers: Resolution and Error Correction01:14

NMR Spectrometers: Resolution and Error Correction

679
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...
679
Double Resonance Techniques: Overview01:12

Double Resonance Techniques: Overview

191
Double resonance techniques in Nuclear Magnetic Resonance (NMR) spectroscopy involve the simultaneous application of two different frequencies or radiofrequency pulses to manipulate and observe two distinct nuclear spins. One important application of double resonance is spin decoupling, which selectively suppresses coupling with one type of nucleus while observing the NMR signal from another nucleus, simplifying the spectrum and enhancing resolution.
Spin decoupling is usually achieved by...
191
¹H NMR: Interpreting Distorted and Overlapping Signals01:02

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...
1.0K
Atomic Nuclei: Magnetic Resonance01:05

Atomic Nuclei: Magnetic Resonance

639
The number of nuclear spins aligned in the lower energy state is slightly greater than those in the higher energy state. In the presence of an external magnetic field, as the spins precess at the Larmor frequency, the excess population results in a net magnetization oriented along the z axis. When a pulse or a short burst of radio waves at the Larmor frequency is applied along the x axis, the coupling of frequencies causes resonance and flips the nuclear spins of the excess population from the...
639

You might also read

Related Articles

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

Sort by
Same author

Multinuclear Solid-State NMR and NMR Crystallography of Solid Forms of Creatine and Creatinine.

Molecular pharmaceutics·2026
Same author

Precursor-Dependent Routing of Aromatic Amino Acids Determines Lignin Structure in Grasses by Sensitivity-Enhanced Solid-State NMR.

Journal of the American Chemical Society·2026
Same author

Exchange coupling-assisted <sup>13</sup>C dynamic nuclear polarization in microdiamonds at 14 T.

Physical chemistry chemical physics : PCCP·2026
Same author

Isotropic Hyperfine Interactions Drive Cross-Effect Dynamic Nuclear Polarization.

The journal of physical chemistry letters·2025
Same author

Clustering and Heterogeneous P1 Distributions in Diamond Govern DNP Mechanisms at 6.9 and 13.8 T.

The journal of physical chemistry letters·2025
Same author

Distinct echinocandin responses of Candida albicans and Candida auris cell walls revealed by solid-state NMR.

Nature communications·2025

Related Experiment Video

Updated: Jun 14, 2025

High-Temperature and High-Pressure In situ Magic Angle Spinning Nuclear Magnetic Resonance Spectroscopy
08:55

High-Temperature and High-Pressure In situ Magic Angle Spinning Nuclear Magnetic Resonance Spectroscopy

Published on: October 9, 2020

5.5K

High-field pulsed EPR spectroscopy under magic angle spinning.

Orit Nir-Arad1, Alexander B Fialkov1, David H Shlomi1

  • 1School of Chemistry, Tel-Aviv University, 6997801 Tel-Aviv, Israel.

Science Advances
|August 30, 2024
PubMed
Summary

This study presents the first pulsed electron paramagnetic resonance (EPR) experiments using magic angle spinning (MAS) at high magnetic fields. These advancements enable new investigations into electron spin dynamics crucial for dynamic nuclear polarization (DNP) mechanisms.

More Related Videos

Site Directed Spin Labeling and EPR Spectroscopic Studies of Pentameric Ligand-Gated Ion Channels
11:19

Site Directed Spin Labeling and EPR Spectroscopic Studies of Pentameric Ligand-Gated Ion Channels

Published on: July 4, 2016

10.6K
Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
09:00

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser

Published on: June 28, 2018

9.9K

Related Experiment Videos

Last Updated: Jun 14, 2025

High-Temperature and High-Pressure In situ Magic Angle Spinning Nuclear Magnetic Resonance Spectroscopy
08:55

High-Temperature and High-Pressure In situ Magic Angle Spinning Nuclear Magnetic Resonance Spectroscopy

Published on: October 9, 2020

5.5K
Site Directed Spin Labeling and EPR Spectroscopic Studies of Pentameric Ligand-Gated Ion Channels
11:19

Site Directed Spin Labeling and EPR Spectroscopic Studies of Pentameric Ligand-Gated Ion Channels

Published on: July 4, 2016

10.6K
Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
09:00

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser

Published on: June 28, 2018

9.9K

Area of Science:

  • Physics
  • Chemistry
  • Spectroscopy

Background:

  • Electron paramagnetic resonance (EPR) is typically performed at low magnetic fields.
  • Magic angle spinning (MAS) and high magnetic fields enhance sensitivity and resolution in Nuclear Magnetic Resonance (NMR) and Dynamic Nuclear Polarization (DNP).
  • Investigating DNP mechanisms requires understanding electron spin dynamics under DNP-relevant conditions, which has been experimentally limited.

Purpose of the Study:

  • To perform the first pulsed EPR experiments under magic angle spinning (MAS) at high magnetic fields.
  • To overcome instrumental challenges that have historically prevented MAS-EPR at high fields.
  • To provide experimental data on electron spin dynamics under conditions relevant to DNP.

Main Methods:

  • Development and implementation of a dedicated, homebuilt MAS-EPR probehead.
  • Conducting pulsed EPR experiments under MAS at a high magnetic field (7 tesla).
  • Recording and analyzing pulsed MAS-EPR spectra of P1 center diamond defects.
  • Utilizing time-domain simulations to interpret spectral changes.

Main Results:

  • Demonstration of successful pulsed EPR experiments under MAS at high magnetic field.
  • Observation of unique effects of MAS on EPR line shape, intensity, and signal dephasing.
  • P1 center diamond defect spectra recorded at 7 tesla revealed MAS-induced spectral alterations.
  • Time-domain simulations accurately reproduced observed line shape changes and intensity trends.

Conclusions:

  • Pulsed MAS-EPR at high magnetic fields is now feasible, overcoming significant instrumental hurdles.
  • MAS significantly influences EPR spectral characteristics, including line shape, intensity, and dephasing.
  • This technique provides crucial experimental insights into electron spin dynamics relevant for DNP mechanism studies.