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Related Concept Videos

NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences01:17

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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 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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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.
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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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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.
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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...
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Radiofrequency fields in MAS solid state NMR probes.

Zdeněk Tošner1, Armin Purea2, Jochem O Struppe3

  • 1Munich Center for Integrated Protein Science (CIPS-M) at Department of Chemistry, Technical University of Munich, Lichtenbergstr. 4, 85747 Garching, Germany; Department of Chemistry, Technical University of Munich, Lichtenbergstr. 4, 85747 Garching, Germany; Department of Chemistry, Faculty of Science, Charles University, Hlavova 8, 12842 Prague 2, Czech Republic.

Journal of Magnetic Resonance (San Diego, Calif. : 1997)
|September 26, 2017
PubMed
Summary
This summary is machine-generated.

Dynamic radiofrequency (RF) field variations in solenoid coils during magic angle spinning (MAS) impact NMR experiments. Understanding these RF inhomogeneities is crucial for accurate pulse calibration and robust experimental design.

Keywords:
Cross-polarizationMagic angle spinningNutation experimentRadiofrequency amplitude and phase modulationRadiofrequency field inhomogeneitySolenoid coilSolid state NMR

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Area of Science:

  • Solid-state Nuclear Magnetic Resonance (NMR) Spectroscopy
  • Physical Chemistry
  • Analytical Chemistry

Background:

  • Solenoid coils are essential components in NMR spectrometers, generating radiofrequency (RF) fields for experiments.
  • The static distribution of RF fields along the coil axis is well-understood, but dynamic inhomogeneities are less characterized.
  • Sample rotation, particularly during magic angle spinning (MAS), introduces complex RF field modulations.

Purpose of the Study:

  • To analyze the dynamic radiofrequency (RF) field distribution within a solenoid coil during sample rotation.
  • To investigate the impact of RF inhomogeneities on NMR pulse sequences, specifically pulse calibration and cross-polarization experiments.
  • To review and propose methods for mapping RF fields for imaging applications.

Main Methods:

  • Extensive numerical simulations were employed to model RF field dynamics.
  • Analysis focused on the effects of radial RF inhomogeneities induced by sample rotation.
  • Methods for RF field mapping using B0 gradients were reviewed, including nutation, cross-polarization, and spin-lock experiments.

Main Results:

  • Dynamic radial RF inhomogeneities and phase modulations occur during MAS, especially in coil end regions (±25% amplitude, ±30° phase variation).
  • RF inhomogeneity significantly affects pulse calibration and ramped cross-polarization (CP) experiments across various MAS rates.
  • RF field mapping techniques provide direct visualization of amplitude distribution and channel correlations.

Conclusions:

  • Understanding dynamic RF field distribution is critical for optimizing NMR spectrometer performance.
  • Knowledge of RF inhomogeneities enables the design of more robust NMR pulse sequences and experimental protocols.
  • RF field mapping techniques offer valuable tools for characterizing coil performance and calibrating experiments.