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Related Concept Videos

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

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

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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...
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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...
1.2K
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

1.1K
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...
1.1K
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,...
1.1K
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
¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

1.2K
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...
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Hyperfine Coupling Constants in Local Exact Two-Component Theory.

Yannick J Franzke1, Jason M Yu2

  • 1Fachbereich Chemie, Philipps-Universität Marburg, Hans-Meerwein-Straße 4, 35032 Marburg, Germany.

Journal of Chemical Theory and Computation
|December 20, 2021
PubMed
Summary
This summary is machine-generated.

We developed an efficient computational method for electron-nucleus hyperfine coupling using the exact two-component (X2C) theory. This approach accurately predicts molecular properties, matching experimental data for transition-metal and rare-earth compounds.

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Area of Science:

  • Quantum chemistry
  • Relativistic effects in molecules
  • Computational materials science

Background:

  • Accurate calculation of electron-nucleus hyperfine coupling is crucial for understanding molecular properties.
  • Relativistic effects become significant for heavy elements, necessitating advanced theoretical frameworks.
  • Existing methods for hyperfine coupling can be computationally expensive, especially for large systems.

Purpose of the Study:

  • To present a highly efficient implementation of the electron-nucleus hyperfine coupling matrix within the one-electron exact two-component (X2C) theory.
  • To address the computational cost associated with the exact derivative of the X2C Hamiltonian by employing the diagonal local approximation to the unitary decoupling transformation (DLU).
  • To validate the accuracy and efficiency of the DLU-X2C method for various chemical systems.

Main Methods:

  • Implementation of the complete derivative of the X2C Hamiltonian, considering derivatives of the unitary decoupling transformation.
  • Application of the diagonal local approximation to the unitary decoupling transformation (DLU) to reduce computational expense.
  • Employment of the finite nucleus model and the (modified) screened nuclear spin-orbit approach for two-electron picture-change effects.
  • Fully integral direct and OpenMP-parallelized implementation for high performance.
  • Extensive benchmark studies on Hamiltonian, basis set, and density functional approximations for transition-metal compounds.

Main Results:

  • The DLU approximation introduces negligible error, with the DLU-X2C Hamiltonian accurately reproducing four-component relativistic results.
  • Functionals with high Hartree-Fock exchange (e.g., CAM-QTP-02, ωB97X-D) and the pure density functional r2SCAN show favorable performance.
  • Fully uncontracted or contracted quadruple-ζ basis sets are necessary for accurate calculations.
  • The method was successfully applied to large systems, including [Pt(C6Cl5)4]- and four rare-earth single-molecule magnets.
  • Results from the spin-orbit DLU-X2C Hamiltonian show excellent agreement with experimental findings for Pt, La, Lu, and Tb molecules.

Conclusions:

  • The DLU-X2C method provides a computationally efficient and accurate approach for calculating electron-nucleus hyperfine coupling.
  • The developed implementation is robust and capable of handling complex molecules and materials.
  • The findings support the use of specific density functionals and basis sets for reliable relativistic calculations.