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NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

3.2K
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...
3.2K
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.5K
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,...
1.5K
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

1.5K
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...
1.5K
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

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

1.7K
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...
1.7K
Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)01:22

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

1.5K
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...
1.5K
Manipulation and Analysis01:21

Manipulation and Analysis

300
GIS manipulation and analysis functions are vital for decision-making and planning. These activities range from data retrieval tasks, such as selecting information based on specific criteria, to advanced analytical techniques that address complex spatial problems.One critical GIS analysis method is overlaying, which combines multiple data layers to examine impacts. For example, overlaying a river-dammed lake boundary with road networks can identify affected infrastructure. Another common...
300

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Related Experiment Video

Updated: Jan 30, 2026

Preparation and Characterization of C60/Graphene Hybrid Nanostructures
08:40

Preparation and Characterization of C60/Graphene Hybrid Nanostructures

Published on: May 15, 2018

10.0K

Single spin localization and manipulation in graphene open-shell nanostructures.

Jingcheng Li1, Sofia Sanz2, Martina Corso2,3

  • 1CIC nanoGUNE, 20018, Donostia-San Sebastián, Spain.

Nature Communications
|January 16, 2019
PubMed
Summary
This summary is machine-generated.

Researchers observed and controlled individual magnetic moments in graphene nanostructures. This intrinsic π-paramagnetism opens possibilities for graphene in spintronics applications.

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Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Nanotechnology

Background:

  • Graphene's potential for spintronics relies on achieving magnetism.
  • Theoretical models predict magnetism in specific graphene structures due to electron interactions.
  • Experimental verification of graphene magnetism is challenging.

Purpose of the Study:

  • To experimentally observe and manipulate individual magnetic moments in graphene nanostructures.
  • To investigate the origin and properties of magnetism in graphene open-shell systems.
  • To demonstrate the intrinsic π-paramagnetism of graphene.

Main Methods:

  • Utilized scanning tunneling spectroscopy (STS) to detect localized electron spins.
  • Employed the Kondo effect to identify single electron spins at zigzag sites.
  • Quantified spin-spin exchange interactions using inelastic electron excitations (singlet-triplet transitions).
  • Performed theoretical simulations to model electron correlations and spin-polarized states.

Main Results:

  • Observed and manipulated individual magnetic moments in graphene open-shell nanostructures on a gold surface.
  • Detected single electron spins localized at specific zigzag sites via the Kondo effect.
  • Found that nearby spins couple to a singlet ground state, with quantified exchange interactions.
  • Demonstrated that hydrogen adatoms quench magnetic moments and induce half-integer spin switching.

Conclusions:

  • Graphene nanostructures exhibit intrinsic π-paramagnetism.
  • Electron correlations are responsible for spin-polarized radical states in these structures.
  • The ability to control magnetic moments in graphene opens avenues for spintronic devices.