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Related Concept Videos

NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences01:17

NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences

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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.
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NMR Spectrometers: Resolution and Error Correction01:14

NMR Spectrometers: Resolution and Error Correction

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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...
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NMR Spectrometers: Overview01:20

NMR Spectrometers: Overview

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NMR spectrometers consist of a strong magnet, a radiofrequency transmitter, and a detector attached to a computer console for recording spectra of samples containing NMR-active nuclei. In first-generation NMR instruments called continuous-wave spectrometers, the resonance frequencies of the nuclei are determined by frequency-sweep or field-sweep methods. The magnetic field strength is fixed and the rf signal is swept in the former, while the radiofrequency signal is fixed and the magnetic field...
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Double Resonance Techniques: Overview01:12

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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...
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¹³C NMR: ¹H–¹³C Decoupling01:04

¹³C NMR: ¹H–¹³C Decoupling

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The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
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Chemical Shift: Internal References and Solvent Effects01:17

Chemical Shift: Internal References and Solvent Effects

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In an NMR sample, precise measurement of the absolute absorption frequencies of nuclei is difficult. A standard internal reference compound is added, and the frequency difference between the reference signal and sample signals is measured.
The internal reference compound generally used in NMR spectroscopy is tetramethylsilane (TMS). TMS is preferred because it is chemically inert, soluble in NMR solvents, and easily removable. Also, the highly shielded methyl protons in TMS yield an intense...
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Author Spotlight: Exploring Intrinsically Disordered Protein Dynamics Through NMR Relaxation Experiments
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Seedless: on-the-fly pulse calculation for NMR experiments.

Charles J Buchanan1,2, Gaurav Bhole3,4, Gogulan Karunanithy2,5

  • 1Kavli Institute of Nanoscience Discovery, Dorothy Crowfoot Hodgkin Building, Oxford, UK.

Nature Communications
|August 7, 2025
PubMed
Summary
This summary is machine-generated.

Seedless software calculates optimized radio frequency (RF) pulses for Nuclear Magnetic Resonance (NMR) experiments. This tool enhances signal-to-noise ratio and control of magnetisation for improved sensitivity in various NMR applications.

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Area of Science:

  • Nuclear Magnetic Resonance (NMR) spectroscopy
  • Pulse sequence optimization
  • Magnetic Resonance Imaging (MRI)

Background:

  • NMR signal loss occurs due to non-uniform excitation across chemical shifts and radio frequency (RF) inhomogeneity.
  • Existing methods struggle to compensate for these effects, limiting sensitivity and control.

Purpose of the Study:

  • To introduce Seedless, a computational tool for calculating RF pulses that counteract signal loss.
  • To enhance magnetisation control and boost signal-to-noise ratio in NMR experiments.
  • To enable on-the-fly optimization of NMR pulses tailored to specific samples and hardware.

Main Methods:

  • Utilizes an optimized GRadient Ascent Pulse Engineering (GRAPE) implementation for rapid pulse calculation.
  • Applies one of four selected transforms to identified chemical shift bands.
  • Demonstrates effectiveness using imaging experiments across 1D, 2D, and 3D applications.

Main Results:

  • Seedless calculates compensating pulses in seconds, enabling on-the-fly optimization.
  • Demonstrated increases in coil volume and signal-to-noise ratio in imaging experiments.
  • Achieved significant sensitivity gains in diverse chemical and biological NMR applications.

Conclusions:

  • Seedless offers a versatile method to improve NMR sensitivity across all pulse sequences.
  • The tool's ability to tailor pulses to specific samples and hardware enhances experimental outcomes.
  • On-the-fly pulse optimization via Seedless advances NMR capabilities for research and diagnostics.