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Related Concept Videos

Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

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 have a...
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

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,...
Valence Bond Theory02:42

Valence Bond Theory

Coordination compounds and complexes exhibit different colors, geometries, and magnetic behavior, depending on the metal atom/ion and ligands from which they are composed. In an attempt to explain the bonding and structure of coordination complexes, Linus Pauling proposed the valence bond theory, or VBT, using the concepts of hybridization and the overlapping of the atomic orbitals. According to VBT, the central metal atom or ion (Lewis acid) hybridizes to provide empty orbitals of suitable...
Valence Bond Theory02:45

Valence Bond Theory

Overview of Valence Bond Theory
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

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

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...
Fermi Level Dynamics01:12

Fermi Level Dynamics

The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
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Updated: May 17, 2026

Spin Saturation Transfer Difference NMR (SSTD NMR): A New Tool to Obtain Kinetic Parameters of Chemical Exchange Processes
11:44

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Published on: November 12, 2016

Spin-Adapted Restricted Open-Shell Hartree-Fock and Its Dynamic Correlation Extension.

Maru Song1, Luca Bonfirraro1, Ignacio Fdez Galván2

  • 1Max Planck Institute for Solid State Research, Stuttgart 70569, Germany.

Journal of Chemical Theory and Computation
|May 15, 2026
PubMed
Summary
This summary is machine-generated.

A new computational method, configuration-state-function restricted open-shell Hartree-Fock (CSF-ROHF), optimizes electronic configurations efficiently. Incorporating dynamic correlation significantly improves accuracy for complex molecular systems.

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Area of Science:

  • Quantum Chemistry
  • Computational Chemistry
  • Electronic Structure Theory

Background:

  • Accurate electronic structure calculations are crucial for understanding molecular properties.
  • Restricted open-shell Hartree-Fock (ROHF) methods offer a balance between accuracy and computational cost.
  • Challenges remain in optimizing electronic configurations and capturing dynamic correlation effects.

Purpose of the Study:

  • To implement and evaluate a spin-adapted configuration-state-function restricted open-shell Hartree-Fock (CSF-ROHF) method in OpenMolcas.
  • To assess the computational efficiency and convergence behavior of the CSF-ROHF approach.
  • To develop and validate a computationally inexpensive protocol for incorporating dynamic correlation to improve CSF-ROHF accuracy.

Main Methods:

  • Development of a spin-adapted CSF-ROHF implementation using the Graphical Unitary Group Approach and Generalized Active Space algorithms.
  • Analysis of CSF-ROHF convergence properties, emphasizing the role of initial orbital ordering.
  • Introduction of a second-order, spin-adapted perturbation strategy with the Stochastic-SplitGAS algorithm to include dynamic correlation.

Main Results:

  • The CSF-ROHF method enables orbital optimization of single electronic configurations at near mean-field cost.
  • Computational efficiency was demonstrated on {[Ni(H2O)4]nOn-1(H2O)2}2+ model systems.
  • CSF-ROHF showed limitations for iron-sulfur cluster spin gaps, but perturbation theory correction yielded excellent agreement with high-level methods.

Conclusions:

  • The developed CSF-ROHF method provides an efficient route for electronic structure calculations.
  • Initial orbital ordering is critical for successful CSF-ROHF optimization.
  • Perturbative correction significantly enhances the accuracy of CSF-ROHF, offering a cost-effective approach for complex systems.