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Related Concept Videos

Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

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

Atomic Nuclei: Nuclear Spin State Population Distribution

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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.
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Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

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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.
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Atomic Nuclei: Nuclear Spin01:08

Atomic Nuclei: Nuclear Spin

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All atomic particles possess an intrinsic angular momentum, or 'spin'. Electrons, protons, and neutrons each have a spin value of ½, although protons and neutrons in nuclei may have higher half-integer spins owing to energetic factors.
Atomic nuclei have a net nuclear spin, , which can have an integer or half-integer value. In atomic nuclei, the spins of protons are paired against each other but not with neutrons, and vice versa. Consequently, an even number of protons does not contribute...
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Nuclear Overhauser Enhancement (NOE)01:06

Nuclear Overhauser Enhancement (NOE)

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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...
1.3K
NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

3.4K
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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Dissolution Dynamic Nuclear Polarization Instrumentation for Real-time Enzymatic Reaction Rate Measurements by NMR
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Effect of electron spin dynamics on solid-state dynamic nuclear polarization performance.

Ting Ann Siaw1, Matthias Fehr, Alicia Lund

  • 1Department of Chemical Engineering, University of California Santa Barbara, Santa Barbara, CA 93106, USA. songi@chem.ucsb.edu.

Physical Chemistry Chemical Physics : PCCP
|June 27, 2014
PubMed
Summary
This summary is machine-generated.

Generic mono-nitroxide radicals can achieve solid-state dynamic nuclear polarization (ssDNP) comparable to bi-radicals at low temperatures. This finding expands the use of ssDNP for material characterization by optimizing experimental conditions.

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Area of Science:

  • Solid-state dynamic nuclear polarization (ssDNP)
  • Nuclear Magnetic Resonance (NMR) spectroscopy
  • Material characterization

Background:

  • Solid-state dynamic nuclear polarization (ssDNP) enhanced NMR is a powerful tool for material characterization.
  • Broad adoption requires the use of generic mono-nitroxide radicals as spin probes.
  • Understanding ssDNP efficiency factors is crucial for optimizing experimental conditions.

Purpose of the Study:

  • To advance the mechanistic understanding of ssDNP at liquid helium temperatures (4-40 K).
  • To investigate the effect of electron spin dynamics on ssDNP performance.
  • To determine the factors influencing the efficiency of mono- and bi-radicals as spin probes.

Main Methods:

  • Examined ssDNP performance at liquid helium temperatures (4-40 K) and 7 T.
  • Analyzed nuclear spin polarization (Pn) and signal buildup time as a function of electron spin relaxation rates.
  • Modulated electron spin relaxation rates by varying mono- and bi-radical spin concentrations.

Main Results:

  • Mono- and bi-radicals yielded comparable nuclear spin polarization at 4 K and 7 T, contrasting with higher temperatures.
  • Observed maximum Pn at intermediate spin concentrations for both radical types.
  • Demonstrated that comparable polarization arises from a similar integral EPR saturation factor.

Conclusions:

  • Generic mono-nitroxide probes can achieve competitive ssDNP performance to custom bi-radicals at low temperatures.
  • Mechanistic insights rationalize ssDNP performance based on electron spin dynamics and radical concentration.
  • This expands the application scope of ssDNP for studying functional materials and solids.