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Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

957
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,...
957
π Electron Effects on Chemical Shift: Overview01:27

π Electron Effects on Chemical Shift: Overview

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An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0,...
1.1K
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

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

1000
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...
1000
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 Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

911
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...
911
Energy Associated With a Charge Distribution01:21

Energy Associated With a Charge Distribution

1.5K
The work done to bring a charge through a distance r is given by the potential difference between the initial and the final position. To assemble a collection of point charges, the total work done can be expressed in terms of the product of each pair of charges divided by their separation distance, defined with respect to a suitable origin. Solving this expression gives the energy stored in a point charge distribution.
1.5K

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Related Experiment Video

Updated: Jun 25, 2025

Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids
08:04

Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids

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Electronic Couplings and Conversion Dynamics between Localized and Charge Transfer Excitations from Many-Body Green's

Gianluca Tirimbò1,2, Björn Baumeier1,2

  • 1Department of Mathematics and Computer Science, Eindhoven University of Technology, P.O. Box 513, 5600 MB Eindhoven, The Netherlands.

Journal of Chemical Theory and Computation
|May 21, 2024
PubMed
Summary

We explored electronic coupling between localized and charge-transfer excitations using GW-Bethe-Salpeter equation theory. Different methods minimally impacted couplings in small systems but showed variations in large, disordered organic materials.

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Area of Science:

  • Computational Chemistry
  • Materials Science
  • Quantum Mechanics

Background:

  • Understanding electronic coupling is crucial for designing organic electronic materials.
  • Localized excitations (LEs) and charge-transfer (CT) excitations play key roles in charge dynamics.
  • Many-body Green's functions theory within the GW approximation and Bethe-Salpeter equation (GW-BSE) is a powerful tool for electronic structure calculations.

Purpose of the Study:

  • To investigate the determination of electronic coupling between LE and CT excitations.
  • To assess the influence of different diabatization methods and GW-BSE model choices on LE-CT couplings.
  • To evaluate LE-CT couplings in large-scale, disordered organic semiconductor morphologies.

Main Methods:

  • Many-body Green's functions theory using the GW approximation and Bethe-Salpeter equation (GW-BSE).
  • Application to a small molecule dimer system and a large-scale low-donor morphology (rubrene and fullerene).
  • Coupled GW-BSE-molecular mechanics calculations for disordered systems.
  • Comparison of Edmiston-Ruedenberg, Generalize Mulliken-Hush, and fragment charge difference diabatization formalisms.

Main Results:

  • Diabatization methods and GW-BSE model choices minimally affected LE-CT couplings in small systems.
  • Significant differences in LE-CT couplings were observed for disordered organic systems using different diabatization methods.
  • These differences impacted intermediate-time state populations in a kinetic model but not final populations.

Conclusions:

  • The choice of diabatization method becomes important for accurate LE-CT coupling calculations in complex, disordered organic materials.
  • GW-BSE calculations coupled with molecular mechanics provide a robust framework for studying electronic couplings in such systems.
  • Understanding these couplings is essential for predicting and controlling charge conversion dynamics in organic electronics.