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

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

1.6K
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...
1.6K
NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

3.0K
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...
3.0K
¹H NMR Signal Multiplicity: Splitting Patterns01:13

¹H NMR Signal Multiplicity: Splitting Patterns

6.5K
When protons A and X are coupled, their nuclear spin energy levels are slightly modified. This is because the energy required to excite proton A to a spin state parallel to proton X is slightly different from the energy required for it to become anti-parallel to spin X. Consequently, there are two possible excitation frequencies for A (A1 and A2), depending on the spin state of X, and vice versa. The mutual nature of coupling implies that the difference between frequencies A1 and A2, indicated...
6.5K
¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

1.5K
Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
1.5K
¹H NMR: Long-Range Coupling01:27

¹H NMR: Long-Range Coupling

2.6K
The coupling interactions of nuclei across four or more bonds are usually weak, with J values less than 1 Hz. While these are usually not observed in spectra, the presence of multiple bonds along the coupling pathway can result in observable long-range coupling.
In alkenes, spin information is communicated via σ–π overlap, as seen in allylic (four-bond) and homoallylic (five-bond) couplings. These coupling interactions are stronger when the σ bond is parallel to the alkene...
2.6K
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

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Related Experiment Video

Updated: Jan 16, 2026

Generation and Coherent Control of Pulsed Quantum Frequency Combs
06:42

Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

9.6K

Nonreciprocal quantum synchronization.

Deng-Gao Lai1, Adam Miranowicz2,3, Franco Nori2,4

  • 1RIKEN Center for Quantum Computing (RQC), RIKEN Wako-shi, Saitama, Japan. denggaolai@foxmail.com.

Nature Communications
|September 26, 2025
PubMed
Summary
This summary is machine-generated.

This study demonstrates directional quantum synchronization of phonons, a novel quantum resource. The method shows robustness against imperfections and noise, paving the way for advanced quantum technologies.

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Last Updated: Jan 16, 2026

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Area of Science:

  • Quantum physics
  • Quantum information science
  • Optomechanics

Background:

  • Nonreciprocal physics is crucial for classical and quantum resources.
  • Nonreciprocal quantum synchronization of phonons remains unexplored.
  • Existing methods are sensitive to imperfections and noise.

Purpose of the Study:

  • To demonstrate nonreciprocal quantum synchronization of phonons.
  • To reveal the robustness of this quantum resource against practical device imperfections and thermal noise.
  • To establish a foundation for generating robust nonreciprocal quantum resources.

Main Methods:

  • Harnessing the synergy of the Sagnac and magnon-Kerr effects.
  • Utilizing light or magnetic fields to control phonon synchronization.
  • Investigating the impact of fabrication imperfections and thermal noise.

Main Results:

  • Achieved directional quantum synchronization of phonons.
  • Demonstrated counterintuitive robustness against random fabrication imperfections and thermal noise.
  • Observed unique nonreciprocity in quantum synchronization based on direction.

Conclusions:

  • The proposed method enables nonreciprocal quantum synchronization of phonons.
  • The approach overcomes limitations of previous proposals by enhancing resonator resilience.
  • Lays the groundwork for creating robust nonreciprocal quantum resources.