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

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

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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...
1.5K
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.4K
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,...
1.4K
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

1.4K
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...
1.4K
Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)01:22

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

1.4K
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...
1.4K
NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

2.9K
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...
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The Pauli Exclusion Principle03:06

The Pauli Exclusion Principle

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The arrangement of electrons in the orbitals of an atom is called its electron configuration. We describe an electron configuration with a symbol that contains three pieces of information:
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Related Experiment Video

Updated: Jan 4, 2026

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
11:21

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

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Dynamical Spin-Orbit Coupling of a Quantum Gas.

Ronen M Kroeze1,2, Yudan Guo1,2, Benjamin L Lev1,2,3

  • 1Department of Physics, Stanford University, Stanford, California 94305, USA.

Physical Review Letters
|November 9, 2019
PubMed
Summary

We demonstrate dynamic spin-orbit coupling (SOC) in Bose-Einstein condensates using Raman transitions and cavity fields. This leads to a novel spinor-helix polariton condensate with potential for exotic quantum states.

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Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
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Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser

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Nanofabrication of Gate-defined GaAs/AlGaAs Lateral Quantum Dots
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Nanofabrication of Gate-defined GaAs/AlGaAs Lateral Quantum Dots

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Related Experiment Videos

Last Updated: Jan 4, 2026

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Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
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Nanofabrication of Gate-defined GaAs/AlGaAs Lateral Quantum Dots
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Nanofabrication of Gate-defined GaAs/AlGaAs Lateral Quantum Dots

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Area of Science:

  • Quantum optics
  • Atomic physics
  • Condensed matter physics

Background:

  • Bose-Einstein condensates (BECs) are quantum states of matter with unique properties.
  • Spin-orbit coupling (SOC) is crucial for emergent quantum phenomena.
  • Controlling SOC dynamically in quantum systems is a significant challenge.

Purpose of the Study:

  • To realize and investigate dynamical one-dimensional spin-orbit coupling (SOC) in a Bose-Einstein condensate.
  • To explore the formation of novel light-matter states through superradiance and backaction.
  • To pave the way for creating exotic quantum states like topological superfluids.

Main Methods:

  • Utilizing Raman transitions driven by classical pump fields and a quantum dynamical cavity field.
  • Inducing SOC via spin-correlated momentum impulses on atoms.
  • Observing emergent SOC through spin-resolved atomic momentum imaging and cavity field emission analysis.

Main Results:

  • Achieved dynamical 1D SOC in a BEC confined within an optical cavity.
  • Observed a superradiant Dicke phase transition above a critical pump power.
  • Created a spinor-helix polariton condensate with emergent spin-spatial ordering.

Conclusions:

  • The study successfully demonstrates a novel method for realizing dynamical SOC in quantum gas cavity QED systems.
  • The observed spinor-helix polariton condensate is a new type of light-matter quasi-particle.
  • This work opens avenues for exploring Meissner-like effects, topological superfluids, and quantum Hall states.