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Related Concept Videos

Echo01:06

Echo

1.0K
The human ear cannot distinguish between two sources of sound if they happen to reach within a specific time interval, typically 0.1 seconds apart. More than this, and they are perceived as separate sources.
Imagine the sound is reflected back to the ears. Assuming that the source is very close to the human, the difference between hearing the two sounds—the emitted sound and the reflected sound—may be more than the minimum time for perceiving distinct sounds. If this is the case,...
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Catalytically Perfect Enzymes01:07

Catalytically Perfect Enzymes

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The theory of catalytically perfect enzymes was first proposed by W.J. Albery and J. R. Knowles in 1976. These enzymes catalyze biochemical reactions at high-speed. Their catalytic efficiency values range from 108-109 M-1s-1. These enzymes are also called 'diffusion-controlled' as the only rate-limiting step in the catalysis is that of the substrate diffusion into the active site. Examples include triose phosphate isomerase, fumarase, and superoxide dismutase.
 
Most enzymes...
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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...
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Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.5K
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,...
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Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

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

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

1.7K
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...
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Study of Protein Dynamics via Neutron Spin Echo Spectroscopy
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Towards perfect NMR: Spin-echo versus perfect-echo building blocks.

Teodor Parella1

  • 1Servei de Ressonància Magnètica Nuclear, Universitat Autònoma de Barcelona, Barcelona, Catalonia, Spain.

Magnetic Resonance in Chemistry : MRC
|June 22, 2018
PubMed
Summary

Researchers explored novel nuclear magnetic resonance (NMR) techniques to enhance spectral quality. They reviewed "perfect-echo" building blocks as alternatives to spin-echo, aiming for undistorted signals in NMR spectroscopy.

Keywords:
NMR building blocksNMR pulse sequence designperfect BIRDperfect INEPTperfect WATERGATEperfect spin-echoperfect-echospin-echo

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Area of Science:

  • Analytical Chemistry
  • Spectroscopy
  • Physical Chemistry

Background:

  • Improving the quality of nuclear magnetic resonance (NMR) spectra is crucial for accurate molecular analysis.
  • Existing NMR methods can suffer from distortions, phase anomalies, and undesired J modulations, complicating data interpretation.
  • The concept of "perfect NMR" aims to achieve undistorted, pure in-phase signals with ideal lineshapes.

Purpose of the Study:

  • To review alternative NMR building blocks to the conventional spin-echo sequence.
  • To introduce and discuss the "perfect-echo" module for enhanced NMR spectral quality.
  • To describe methods for minimizing or removing dispersive contributions in NMR experiments.

Main Methods:

  • Review of alternative NMR building blocks based on a general double spin-echo (SE) module, termed "perfect-echo".
  • Description of several implementations designed to mitigate unwanted dispersive contributions.
  • Illustration of methods using examples relevant to homonuclear and heteronuclear NMR experiments on small molecules.

Main Results:

  • The "perfect-echo" module offers a viable alternative to traditional spin-echo sequences for improving NMR spectral quality.
  • Implemented methods effectively minimize or remove dispersive artifacts, leading to cleaner spectral lineshapes.
  • The described techniques are applicable to both homonuclear and heteronuclear NMR, demonstrating broad utility.

Conclusions:

  • The "perfect-echo" concept provides a robust strategy for achieving higher quality NMR spectra.
  • These advanced NMR pulse sequences are valuable tools for obtaining undistorted, pure absorption signals.
  • The reviewed methods offer practical solutions for enhancing spectral resolution and simplifying the analysis of small molecules.