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Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

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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...
1.7K
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

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

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

2.0K
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...
2.0K
Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

2.3K
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...
2.3K
NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

3.9K
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...
3.9K
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...
1.7K

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Related Experiment Video

Updated: Apr 16, 2026

All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics
11:33

All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics

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Spin-current nano-oscillator based on nonlocal spin injection.

V E Demidov1, S Urazhdin2, A Zholud2

  • 1Department of Physics and Center for Nonlinear Science, University of Muenster, 48149 Muenster, Germany.

Scientific Reports
|February 27, 2015
PubMed
Summary

Nonlocal spin injection can create pure spin currents and induce coherent magnetization dynamics. This enables novel microwave nano-sources for spintronics and magnonics with tunable frequencies and high stability.

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Area of Science:

  • Physics
  • Materials Science
  • Electrical Engineering

Background:

  • Nonlocal spin injection generates pure spin currents.
  • Pure spin currents are crucial for spintronic and magnonic devices.
  • Efficient spin current generation is key for advanced nano-scale applications.

Purpose of the Study:

  • To demonstrate that nonlocal spin injection can induce coherent magnetization dynamics.
  • To explore the potential of this phenomenon for creating novel microwave nano-sources.
  • To investigate the characteristics of these nano-sources for spintronic and magnonic applications.

Main Methods:

  • Experimental demonstration of nonlocal spin injection.
  • Induction and observation of coherent magnetization dynamics.
  • Characterization of microwave nano-source properties, including linewidth and tunability.
  • Spatially resolved measurements of dynamical magnetization.
  • Development of a quasilinear dynamical model for analysis.

Main Results:

  • Nonlocal spin injection successfully induces coherent magnetization dynamics.
  • The induced dynamics can be utilized for microwave nano-sources.
  • These nano-sources exhibit narrow oscillation linewidths.
  • Frequency tunability over a wide range is achieved using a static magnetic field.
  • Spatially resolved measurements reveal a large oscillation area, enhancing stability against thermal fluctuations.

Conclusions:

  • Nonlocal spin injection is a viable mechanism for generating coherent magnetization dynamics.
  • This phenomenon offers a pathway to novel, stable, and tunable microwave nano-sources.
  • The developed dynamical model accurately describes the observed oscillation characteristics.
  • The findings have significant implications for the future of spintronic and magnonic devices.