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Related Concept Videos

¹H NMR: Long-Range Coupling01:27

¹H NMR: Long-Range Coupling

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

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

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...
¹H NMR Signal Multiplicity: Splitting Patterns01:13

¹H NMR Signal Multiplicity: Splitting Patterns

When protons A and X are coupled, their nuclear spin energy levels are slightly modified. This is because the energy required to excite proton A to a spin state parallel to proton X is slightly different from the energy required for it to become anti-parallel to spin X. Consequently, there are two possible excitation frequencies for A (A1 and A2), depending on the spin state of X, and vice versa. The mutual nature of coupling implies that the difference between frequencies A1 and A2, indicated...
¹H NMR: Complex Splitting01:13

¹H NMR: Complex Splitting

A proton M that is coupled to a proton X results in doublet signals for M. However, NMR-active nuclei can be simultaneously coupled to more than one nonequivalent nucleus. When M is coupled to a second proton A, such as in styrene oxide, each peak in the doublet is split into another doublet.
Splitting diagrams or splitting tree diagrams are routinely used to depict such complex couplings. While drawing splitting diagrams, the splitting with the larger coupling constant is usually applied first.
Ligand Binding and Linkage00:49

Ligand Binding and Linkage

Allosteric proteins have more than one ligand binding site; the binding of a ligand to any of these sites influences the binding of ligands to the other sites. When a protein is allosteric, its binding sites are called coupled or linked.  In the case of enzymes, the site that binds to the substrate is known as the active site and the other site is known as the regulatory site. When a ligand binds to the regulatory site, this leads to conformational changes in the protein that can influence the...

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Approximately size extensive local Multireference Singles and Doubles Configuration Interaction.

David B Krisiloff1, Emily A Carter

  • 1Department of Chemistry, Princeton University, Princeton, NJ 08544, USA.

Physical Chemistry Chemical Physics : PCCP
|February 24, 2012
PubMed
Summary
This summary is machine-generated.

A new computational method improves the accuracy of electronic structure calculations for large molecules. This local, approximately size-extensive Multi-reference Configuration Interaction (MRCI) method significantly reduces computational cost and energy errors.

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Area of Science:

  • Quantum Chemistry
  • Computational Chemistry
  • Theoretical Chemistry

Background:

  • Multi-reference Configuration Interaction (MRCI) is a highly accurate method for small molecules.
  • Traditional MRCI methods have high computational costs and are not size-extensive, limiting their application to larger systems.
  • Existing methods struggle with accurate electronic structure predictions for molecules beyond a certain size.

Purpose of the Study:

  • To develop a computationally efficient and size-extensive MRCI method applicable to larger molecules.
  • To address the limitations of traditional MRCI in terms of computational scaling and energy errors.
  • To enable accurate electronic structure and reaction energetics predictions for medium-to-large molecules.

Main Methods:

  • Developed a local (L) MRCI approach combined with Cholesky decomposition (CD) for efficient integral processing.
  • Implemented integral screening and truncation of long-range electron correlation in a local orbital basis.
  • Investigated a priori and a posteriori size extensivity corrections, including Multi-reference Averaged Coupled-Pair Functional (MRACPF) and Davidson-Silver/Pople schemes.

Main Results:

  • Achieved a computational cost scaling of O(N(3)) with a small prefactor, significantly reducing computational expense.
  • Demonstrated that CD-LMRACPF provides superior accuracy compared to Davidson-type corrections.
  • Successfully applied the CD-LMRACPF method to molecules with up to 50 heavy atoms.

Conclusions:

  • The developed CD-LMRACPF method offers a computationally feasible and accurate approach for electronic structure calculations of larger molecules.
  • This method overcomes the limitations of traditional MRCI, enabling high-accuracy predictions for systems previously intractable.
  • The advancements pave the way for more sophisticated theoretical studies in chemistry and materials science involving larger molecular systems.