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Related Concept Videos

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...
Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...
Nuclear Overhauser Enhancement (NOE)01:06

Nuclear Overhauser Enhancement (NOE)

Irradiation of a spin-active nucleus causes an increase or decrease in the signal intensity of neighboring nuclei that are not necessarily chemically bonded or involved in J-coupling. This phenomenon, called the nuclear Overhauser enhancement (NOE), results from through-space interactions between the nuclear spins. The NOE effect decreases with increasing internuclear distance and is generally not observed beyond 4 angstroms. In NOE, dipole-dipole interactions between neighboring spin-active...
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...
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Molecular and Ionic Solids

Crystalline solids are divided into four types: molecular, ionic, metallic, and covalent network based on the type of constituent units and their interparticle interactions.
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Preparation of Fungal and Plant Materials for Structural Elucidation Using Dynamic Nuclear Polarization Solid-State NMR
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Dynamic Nuclear Polarization in the solid state: a transition between the cross effect and the solid effect.

Daphna Shimon1, Yonatan Hovav, Akiva Feintuch

  • 1Department of Chemical Physics, Weizmann Institute of Science, Rehovot, Israel.

Physical Chemistry Chemical Physics : PCCP
|March 16, 2012
PubMed
Summary
This summary is machine-generated.

Proton Dynamic Nuclear Polarization (DNP) experiments reveal temperature-dependent contributions of the Solid Effect (SE) and Cross Effect (CE) mechanisms. Lowering temperatures below 20 K enhances SE-DNP while diminishing CE-DNP in TEMPOL-doped samples.

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Area of Science:

  • Magnetic Resonance Spectroscopy
  • Physical Chemistry

Background:

  • Dynamic Nuclear Polarization (DNP) enhances nuclear magnetic resonance (NMR) signals by transferring polarization from electron spins to nuclei.
  • In solid-state DNP, enhancement mechanisms include the Solid Effect (SE), Cross Effect (CE), and Thermal Mixing (TM).

Purpose of the Study:

  • To determine the dominant DNP mechanisms responsible for proton signal enhancement in TEMPOL-doped frozen solutions.
  • To investigate the influence of temperature and microwave power on SE-DNP and CE-DNP contributions.

Main Methods:

  • Proton DNP experiments were performed using a hybrid Electron Paramagnetic Resonance (EPR)-NMR spectrometer.
  • Measurements included electron and nuclear spin-lattice relaxation rates, enhancement buildup times, and microwave-swept DNP spectra.
  • A theoretical model was employed to analyze DNP spectra and quantify SE-DNP and CE-DNP contributions.

Main Results:

  • Observed variations in DNP spectral lineshapes indicated changes in the relative contributions of SE-DNP and CE-DNP with temperature and microwave power.
  • Analysis revealed that lowering the temperature below 20 K increased the SE-DNP contribution and decreased the CE-DNP contribution.
  • The Thermal Mixing (TM) mechanism was found to be negligible in this study.

Conclusions:

  • The study successfully quantified the contributions of SE-DNP and CE-DNP mechanisms to proton signal enhancement.
  • Temperature plays a critical role in modulating the balance between SE-DNP and CE-DNP, with implications for optimizing DNP experiments.