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

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

1.9K
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...
1.9K
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.6K
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,...
1.6K
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

1.6K
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.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
1.6K
NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

3.6K
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...
3.6K
Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)01:22

Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)

1.7K
Vicinal or three-bond coupling is commonly observed between protons attached to adjacent carbons. Here, nuclear spin information is primarily transferred via electron spin interactions between adjacent C‑H bond orbitals. This generally favors the antiparallel arrangement of spins, so 3J values are usually positive.
The extent of coupling depends on the C‑C bond length, the two H‑C‑C angles, any electron-withdrawing substituents, and the dihedral angle between the involved orbitals. The...
1.7K
Nuclear Overhauser Enhancement (NOE)01:06

Nuclear Overhauser Enhancement (NOE)

1.6K
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...
1.6K

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Related Experiment Video

Updated: Mar 28, 2026

Hyperpolarized Xenon for NMR and MRI Applications
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Hyperpolarized Xenon for NMR and MRI Applications

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Synchronous Spin-Exchange Optical Pumping.

A Korver1, D Thrasher1, M Bulatowicz1

  • 1Department of Physics, University of Wisconsin-Madison, Madison, Wisconsin 53706, USA.

Physical Review Letters
|January 2, 2016
PubMed
Summary
This summary is machine-generated.

This study introduces a novel precision Nuclear Magnetic Resonance (NMR) method using hyperpolarized gases. The technique significantly reduces NMR shifts caused by alkali spin-exchange fields, enabling highly accurate measurements.

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Area of Science:

  • Atomic, Molecular, and Optical Physics
  • Quantum Information Science
  • Magnetic Resonance Imaging

Background:

  • Precision Nuclear Magnetic Resonance (NMR) is crucial for various scientific fields.
  • NMR measurements are often limited by shifts and broadening caused by external fields, particularly alkali spin-exchange fields.
  • Existing methods struggle to mitigate these detrimental effects effectively.

Purpose of the Study:

  • To develop and demonstrate a new approach for precision NMR using hyperpolarized gases.
  • To mitigate NMR frequency shifts induced by alkali spin-exchange fields.
  • To investigate and overcome novel NMR broadening effects.

Main Methods:

  • Implementation of an NMR bias field using a sequence of alkali (Rubidium-Rb) 2π pulses.
  • Optical pumping of Rb polarization transverse to the bias field.
  • Modulation of Rb polarization at the noble-gas (Xenon-Xe) NMR resonance to build up precessing transverse Xe polarization via spin-exchange collisions.

Main Results:

  • Demonstrated a novel method for precision NMR with hyperpolarized gases.
  • Successfully mitigated NMR shifts due to the alkali spin-exchange field.
  • Achieved a 2500× suppression of spin-exchange frequency shifts.
  • Projected NMR frequency uncertainties below 10 nHz/sqrt[Hz] at the photon shot-noise limit.

Conclusions:

  • The developed approach significantly enhances precision in NMR measurements.
  • This technique effectively suppresses detrimental spin-exchange field effects, paving the way for new applications.
  • The results indicate a path towards achieving unprecedented NMR frequency uncertainties.