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¹H NMR: Long-Range Coupling01:27

¹H NMR: Long-Range Coupling

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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...
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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...
1.3K
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.2K
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,...
1.2K
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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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...
1.2K
Crystal Field Theory - Octahedral Complexes02:58

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Crystal Field Theory
To explain the observed behavior of transition metal complexes (such as colors), a model involving electrostatic interactions between the electrons from the ligands and the electrons in the unhybridized d orbitals of the central metal atom has been developed. This electrostatic model is crystal field theory (CFT). It helps to understand, interpret, and predict the colors, magnetic behavior, and some structures of coordination compounds of transition metals.
CFT focuses on...
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A Benchmark and Basis-Set Extrapolation Study of Hyperfine Coupling Constants from the Random Phase Approximation and

Daniel Graf1, Lu Liu1, Florian Siekmann1

  • 1Theoretical Chemistry, Department of Chemistry, Ludwig-Maximilians-Universität München (LMU), D-81377 Munich, Germany.

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|April 23, 2026
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Summary
This summary is machine-generated.

Accurately calculating hyperfine coupling constants (HFCCs) is now more feasible. New σ-functionals offer high accuracy comparable to advanced methods but with reduced computational cost for HFCCs.

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Area of Science:

  • Computational Chemistry
  • Quantum Chemistry
  • Spectroscopy

Background:

  • Accurate computation of hyperfine coupling constants (HFCCs) is crucial for linking theoretical predictions with experimental data.
  • Current high-accuracy methods for HFCCs are often computationally expensive, limiting their application.
  • Developing cost-effective and accurate computational methods for HFCCs is an ongoing challenge.

Purpose of the Study:

  • To present and evaluate the theory for calculating HFCCs using σ-functionals.
  • To compare the accuracy and computational cost of σ-functionals against established high-accuracy methods.
  • To investigate the impact of atomic-orbital basis sets on HFCC calculations and enable systematic extrapolations.

Main Methods:

  • Implementation of HFCC calculations using σ-functionals.
  • Comparison of σ-functional results with coupled-cluster singles doubles and perturbative triples (CCSD(T)) and domain-based local pair-natural orbital coupled-cluster singles doubles (DLPNO-CCSD) benchmarks.
  • Assessment of different atomic-orbital basis sets (pcH, pcJ) and their suitability for HFCC computations.
  • Systematic complete basis-set (CBS) extrapolations for HFCCs.

Main Results:

  • The best-performing σ-functional achieves accuracy comparable to DLPNO-CCSD for HFCCs.
  • σ-functionals offer significantly reduced computational demand compared to DLPNO-CCSD.
  • The pcH and pcJ basis-set families are well-suited for RPA, σ-functional, and CCSD(T) HFCC calculations.
  • Basis-set extrapolated CCSD(T) HFCCs provide reliable reference values.

Conclusions:

  • σ-functionals represent a promising and computationally efficient approach for accurate HFCC calculations.
  • The developed methods and basis-set recommendations facilitate reliable HFCC benchmarks.
  • This work provides new reference values for HFCCs, aiding future theoretical and experimental studies.