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Double Resonance Techniques: Overview01:12

Double Resonance Techniques: Overview

820
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...
820
¹H NMR Signal Multiplicity: Splitting Patterns01:13

¹H NMR Signal Multiplicity: Splitting Patterns

7.0K
When protons A and X are coupled, their nuclear spin energy levels are slightly modified. This is because the energy required to excite proton A to a spin state parallel to proton X is slightly different from the energy required for it to become anti-parallel to spin X. Consequently, there are two possible excitation frequencies for A (A1 and A2), depending on the spin state of X, and vice versa. The mutual nature of coupling implies that the difference between frequencies A1 and A2, indicated...
7.0K
Insensitive Nuclei Enhanced by Polarization Transfer (INEPT)01:15

Insensitive Nuclei Enhanced by Polarization Transfer (INEPT)

1.1K
Insensitive Nuclei Enhanced by Polarization Transfer (INEPT) is an advanced Nuclear Magnetic Resonance (NMR) technique specifically designed to detect and enhance the signals of low-abundance nuclei, such as carbon-13 and nitrogen-15, in small molecules. The fundamental principle behind INEPT is the transfer of polarization from a more abundant and highly polarizable nucleus, typically hydrogen-1, to the low-abundance nucleus of interest. This process effectively boosts the NMR signal of the...
1.1K
NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

3.3K
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...
3.3K
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
¹³C NMR: Distortionless Enhancement by Polarization Transfer (DEPT)01:20

¹³C NMR: Distortionless Enhancement by Polarization Transfer (DEPT)

1.8K
When proton-coupled carbon-13 spectra are simplified by a broadband proton decoupling technique, structural information about the coupled protons is lost. Distortionless enhancement by polarization transfer (DEPT) is a technique that provides information on the number of hydrogens attached to each carbon in a molecule. While the DEPT experiment utilizes complex pulse sequences, the pulse delay and flip angle are specifically manipulated. The resulting signals have different phases depending on...
1.8K

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Related Experiment Video

Updated: Feb 27, 2026

A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference
07:56

A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference

Published on: September 5, 2019

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Sensitivity enhancement by multiple-contact cross-polarization under magic-angle spinning.

J Raya1, J Hirschinger1

  • 1Institut de Chimie, UMR 7177 CNRS, Université de Strasbourg, Strasbourg, France.

Journal of Magnetic Resonance (San Diego, Calif. : 1997)
|June 30, 2017
PubMed
Summary
This summary is machine-generated.

Multiple-contact cross-polarization (MC-CP) enhances polarization in solid-state NMR. This method offers higher efficiency than optimized techniques, especially when magic-angle spinning frequencies match heteronuclear couplings.

Keywords:
Cross-polarizationMagic-angle spinningSolid-state NMRSpin diffusion

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High-Temperature and High-Pressure In situ Magic Angle Spinning Nuclear Magnetic Resonance Spectroscopy
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Area of Science:

  • Solid-state Nuclear Magnetic Resonance (NMR) spectroscopy.
  • Advanced pulse sequence development for enhanced sensitivity.

Background:

  • Cross-polarization (CP) is crucial for sensitivity enhancement in solid-state NMR.
  • Magic-angle spinning (MAS) is vital for high-resolution spectra of powder samples.
  • Existing methods like Hartmann-Hahn CP (HHCP) and adiabatic passage HHCP (APHH-CP) have limitations.

Purpose of the Study:

  • To analytically describe and evaluate the Multiple-Contact Cross-Polarization (MC-CP) technique.
  • To compare MC-CP performance against established CP methods under MAS conditions.
  • To determine optimal conditions and limitations for MC-CP experiments.

Main Methods:

  • Application of MC-CP to ferrocene and l-alanine powder samples.
  • Analytical description using density matrix formalism.
  • Combination of two-step memory function and Anderson-Weiss approximation for approximate solutions.

Main Results:

  • MC-CP achieves higher polarization at short contact times than optimized APHH-CP when MAS frequency is near heteronuclear dipolar coupling.
  • MC-CP exhibits broader Hartmann-Hahn (HH) sideband conditions compared to single-contact HHCP.
  • Rotor-asynchronous equilibrations can restore efficient centerband HH condition polarization transfer.

Conclusions:

  • MC-CP is a robust technique, particularly advantageous when standard APHH-CP is challenging.
  • The broader sideband conditions of MC-CP offer flexibility in experimental setup.
  • Understanding repolarization boundary conditions is key for successful MC-CP implementation.