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

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

1.3K
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...
1.3K
¹H NMR: Long-Range Coupling01:27

¹H NMR: Long-Range Coupling

2.4K
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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Valence Bond Theory and Hybridized Orbitals02:38

Valence Bond Theory and Hybridized Orbitals

26.7K
According to valence bond theory, a covalent bond results when: (1) an orbital on one atom overlaps an orbital on a second atom, and (2) the single electrons in each orbital combine to form an electron pair. The strength of a covalent bond depends on the extent of overlap of the orbitals involved. Maximum overlap is possible when the orbitals overlap on a direct line between the two nuclei.
A σ bond (single bond in a Lewis structure) is a covalent bond in which the electron density is...
26.7K
Molecular Orbital Theory II03:51

Molecular Orbital Theory II

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Molecular Orbital Energy Diagrams
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Molecular Orbital Theory I02:35

Molecular Orbital Theory I

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

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

1.5K
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...
1.5K

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Related Experiment Video

Updated: Dec 14, 2025

Computation of Atmospheric Concentrations of Molecular Clusters from ab initio Thermochemistry
12:11

Computation of Atmospheric Concentrations of Molecular Clusters from ab initio Thermochemistry

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A state-specific multireference coupled-cluster method based on the bivariational principle.

Tilmann Bodenstein1, Simen Kvaal1

  • 1Hylleraas Centre for Quantum Molecular Sciences, Department of Chemistry, University of Oslo, P.O. Box 1033 Blindern, N-0315 Oslo, Norway.

The Journal of Chemical Physics
|July 17, 2020
PubMed
Summary
This summary is machine-generated.

A new multireference coupled-cluster (MRCC) method, bivariational MRCC (bivar-MRCC), offers a computationally affordable approach. This state-specific method provides results comparable to existing techniques, making it accessible for broader applications.

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Area of Science:

  • Quantum chemistry
  • Computational chemistry
  • Theoretical chemistry

Background:

  • Multireference coupled-cluster (MRCC) methods are crucial for accurately describing complex electronic structures.
  • Existing state-specific MRCC methods often face challenges with computational cost and complexity.
  • Arponen's bivariational principle offers a novel theoretical framework for developing new quantum chemical methods.

Purpose of the Study:

  • To introduce and formulate a new state-specific multireference coupled-cluster (MRCC) method based on Arponen's bivariational principle, termed bivariational MRCC (bivar-MRCC).
  • To assess the computational feasibility and accuracy of the bivar-MRCC method through pilot implementation and benchmark calculations.
  • To explore the potential of bivar-MRCC as a practical tool for a wider range of users in quantum chemistry.

Main Methods:

  • Development of the bivariational MRCC (bivar-MRCC) method, employing independent parameterizations for the wave function (ket) and its complex conjugate (bra).
  • Incorporation of formal bra and ket references as bivariational parameters to mitigate reference bias.
  • Pilot implementation and extensive benchmark calculations on standard quantum chemistry problems to validate the method's performance.

Main Results:

  • The bivar-MRCC method demonstrates manifest multiplicative separability of the state and additive separability of the energy.
  • The method preserves polynomial scaling of the working equations, contributing to its computational efficiency.
  • Benchmark calculations show that bivar-MRCC results are comparable to those obtained from established state-specific multireference methods.

Conclusions:

  • The bivariational MRCC (bivar-MRCC) method presents a computationally efficient and accurate approach for state-specific electronic structure calculations.
  • Its straightforward formulation and modest computational complexity make it a practical alternative to existing MRCC methods.
  • The bivar-MRCC method has the potential to become a valuable and accessible tool for researchers in computational and theoretical chemistry.