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Related Concept Videos

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

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

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...
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...
Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

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. This...
¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

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 slanted or...
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...

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High-Temperature and High-Pressure In situ Magic Angle Spinning Nuclear Magnetic Resonance Spectroscopy
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Compensated DRAMA sequence for homonuclear dipolar recoupling under magic-angle spinning.

Fang-Chieh Chou1, Tim W T Tsai, Hsin-Kuan Lee

  • 1Department of Chemistry, National Taiwan University, No. 1, Section 4, Roosevelt Road, Taipei, Taiwan.

Solid State Nuclear Magnetic Resonance
|December 8, 2009
PubMed
Summary

The enhanced DRAMA-XY4 pulse sequence improves homonuclear dipolar recoupling for spin 1/2 systems. This method compensates for chemical shift anisotropy and resonance offsets, enabling efficient 31P double-quantum excitation.

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11:44

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Published on: November 12, 2016

Area of Science:

  • Solid-state Nuclear Magnetic Resonance (NMR) spectroscopy
  • Quantum information processing
  • Materials science

Background:

  • Homonuclear dipolar recoupling is crucial for structural studies in solid-state NMR.
  • The DRAMA sequence was a significant development for double-quantum excitation in spin 1/2 systems.
  • Limitations of the original DRAMA sequence include sensitivity to chemical shift anisotropy and resonance offsets, hindering practical applications.

Purpose of the Study:

  • To enhance the practicability and robustness of the DRAMA sequence for homonuclear dipolar recoupling.
  • To improve the efficiency of double-quantum excitation in spin 1/2 systems under challenging conditions.
  • To compensate for detrimental effects of chemical shift anisotropy and resonance offsets.

Main Methods:

  • Modification of the basic DRAMA sequence by incorporating four pi pulses with XY-4 phases (DRAMA-XY4).
  • Application of Average Hamiltonian theory to analyze the performance and compensation capabilities of the new sequence.
  • Numerical simulations and experimental validation using 31P NMR on hydroxyapatite samples.

Main Results:

  • The DRAMA-XY4 sequence demonstrates significantly enhanced performance compared to the basic DRAMA sequence.
  • Effective compensation of chemical shift anisotropy was achieved.
  • Satisfactory 31P double-quantum excitation was observed within a resonance offset range of [-4, 4] kHz.

Conclusions:

  • The incorporation of XY-4 phases into the DRAMA sequence (DRAMA-XY4) greatly improves its utility for homonuclear dipolar recoupling.
  • DRAMA-XY4 offers a robust method for efficient double-quantum excitation, overcoming key limitations of the original DRAMA sequence.
  • This enhanced sequence is suitable for practical applications in solid-state NMR, particularly for 31P studies within specified resonance offset limits.