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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 involved orbitals. The...
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Spin–Spin Coupling Constant: Overview01:08

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

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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

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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: One-Bond Coupling01:17

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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,...
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Atomic Nuclei: Nuclear Spin State Population Distribution01:14

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Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
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Nuclear Spin-Spin Coupling Constants from Auxiliary Density Functional Theory.

Bernardo Zuniga-Gutierrez1, Luis G Cota2, Jesús N Pedroza-Montero3

  • 1Departamento de Química, Centro Universitario de Ciencias Exactas e Ingeniería, Blvd. Marcelino García Barragán 1421, C.P. 44430 Guadalajara, Jalisco, México.

Journal of Chemical Theory and Computation
|March 30, 2026
PubMed
Summary
This summary is machine-generated.

New auxiliary density functional theory (ADFT) methods accurately calculate nuclear spin-spin coupling constants (NSSCCs). This approach is efficient for large systems, enabling routine calculations of nanosystems with over 1000 atoms.

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Area of Science:

  • Quantum chemistry
  • Computational physics
  • Theoretical chemistry

Background:

  • Indirect spin-spin coupling constants (NSSCCs) are crucial for interpreting NMR spectra.
  • Accurate and efficient calculation of NSSCCs is computationally demanding.
  • Auxiliary Density Functional Theory (ADFT) offers a promising framework for electronic structure calculations.

Purpose of the Study:

  • To present working equations for calculating NSSCCs using ADFT.
  • To introduce an implementation based on auxiliary density perturbation theory (ADPT).
  • To demonstrate the computational efficiency and scalability of the new method.

Main Methods:

  • Calculation of NSSCC contributions (Fermi-contact, spin-dipole, spin-orbit terms) as analytic second-order ADFT energy derivatives.
  • Utilizing auxiliary density perturbation theory (ADPT) for perturbed density matrix elements.
  • Employing analytic kernel implementations for Local Density Approximation (LDA) and Generalized Gradient Approximation (GGA) for improved performance.

Main Results:

  • ADPT-calculated NSSCCs show comparable accuracy to Kohn-Sham DFT and favorable agreement with post-Hartree-Fock results.
  • Validation against experimental data for small molecules confirms the reliability of the ADPT NSSCC implementation.
  • Benchmark calculations on amylose chains demonstrate efficient parallel scaling.

Conclusions:

  • The developed ADPT NSSCC method provides accurate results comparable to established methods.
  • The implementation is computationally efficient and scales well for parallel architectures.
  • This approach enables routine calculation of NSSCCs for large nanosystems exceeding 1000 atoms.