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¹H NMR: Long-Range Coupling01:27

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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.
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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.
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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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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.
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The mathematical expression known as the wave function, ψ, contains information about each orbital and the wavelike properties of electrons in an isolated atom. When atoms are bound together in a molecule, the wave functions combine to produce new mathematical descriptions that have different shapes. This process of combining the wave functions for atomic orbitals is called hybridization and is mathematically accomplished by the linear combination of atomic orbitals. The new orbitals that...
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Correlation effects beyond coupled cluster singles and doubles approximation through Fock matrix dressing.

Rahul Maitra1, Takahito Nakajima1

  • 1Computational Molecular Science Research Team, RIKEN Advanced Institute for Computational Science, Kobe 650-0047, Japan.

The Journal of Chemical Physics
|December 3, 2017
PubMed
Summary
This summary is machine-generated.

We developed a new coupled cluster theory method that includes higher-level excitations. This approach accurately captures more electron correlation effects with minimal computational cost, improving quantum chemistry calculations.

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Area of Science:

  • Quantum Chemistry
  • Computational Chemistry
  • Theoretical Chemistry

Background:

  • Coupled cluster theory is a powerful method for electronic structure calculations.
  • Standard coupled cluster with singles and doubles (CCSD) neglects higher excitations, limiting accuracy for some systems.
  • Accurately including triple and higher excitations is computationally expensive.

Purpose of the Study:

  • To present an accurate single-reference coupled cluster theory that incorporates higher excitations.
  • To improve upon conventional coupled cluster with singles and doubles (CCSD) approximations.
  • To provide a computationally economical method for capturing correlation effects beyond CCSD.

Main Methods:

  • A novel 'dressing' of the Fock operator matrix within a singles and doubles framework.
  • The dressing is derived from a second-order perturbative approximation of a similarity transformed Hamiltonian.
  • This method induces higher-rank excitations through local renormalization of orbital lines.

Main Results:

  • The dressed Fock operator effectively simulates triple and higher excitations.
  • The method recovers significant correlation effects beyond the singles and doubles approximation.
  • The additional computational cost is economically scaled with n^5.

Conclusions:

  • This Fock matrix dressing approach offers a natural improvement over conventional CCSD.
  • The method is conceptually simple, easily generalizable to multi-reference schemes, and suitable for strong degeneracy.
  • It serves as a lowest-order perturbative approximation to iterative n-body excitation inclusive coupled cluster schemes.