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NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

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

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

1.1K
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...
1.1K
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.1K
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,...
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¹H NMR: Long-Range Coupling01:27

¹H NMR: Long-Range Coupling

2.0K
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...
2.0K
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

1.0K
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...
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Exploring hyperfine coupling in molecular qubits.

Joan Cardona1, Àlex Solé1,2, Pablo Mella3

  • 1Departament de Química Inorgànica i Orgànica, Institut de Recerca de Química Teòrica i Computacional, Universitat de Barcelona Diagonal 645 08028 Barcelona Spain eliseo.ruizatqi.ub.edu.

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Summary
This summary is machine-generated.

This study benchmarks density functional theory (DFT) methods for predicting hyperfine coupling constants in molecular qubits. It reveals how molecular design can tune these interactions for improved quantum technologies.

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Area of Science:

  • Quantum chemistry
  • Materials science
  • Computational physics

Background:

  • Molecular qubits are crucial for quantum sensing and computing, but their performance is limited by challenges in optimization.
  • Hyperfine coupling significantly influences molecular qubit properties, yet a complete understanding of its mechanisms across various systems is lacking.

Purpose of the Study:

  • To benchmark density functional theory (DFT) methodologies for accurately predicting hyperfine coupling constants in molecular qubits containing VIV and CuII.
  • To systematically analyze the contributions of dipolar, isotropic, and spin-orbit interactions to hyperfine coupling.
  • To investigate the impact of coordination sphere and molecular geometry on these contributions.

Main Methods:

  • Utilized DFT calculations to assess various computational methodologies.
  • Analyzed the decomposition of hyperfine coupling into different contributions.
  • Modeled diverse molecular systems with varying coordination environments and geometries.

Main Results:

  • Identified optimal DFT methodologies for predicting hyperfine coupling constants in VIV and CuII-based molecular qubits.
  • Demonstrated that molecular design can precisely tune hyperfine coupling, either minimizing overall interaction or enhancing it along specific axes.
  • Quantified the influence of coordination sphere and molecular geometry on dipolar, isotropic, and spin-orbit contributions.

Conclusions:

  • Provides crucial insights into structure-property relationships governing hyperfine coupling in molecular qubits.
  • Offers guidance on selecting appropriate computational methods (density functional, basis sets, relativistic corrections) for accurate hyperfine coupling predictions.
  • Highlights the potential of rational molecular design for optimizing molecular qubit performance in quantum technologies.