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Related Concept Videos

NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

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The spin state of an NMR-active nucleus can have a slight effect on its immediate electronic environment. This effect propagates through the intervening bonds and affects the electronic environments of NMR-active nuclei up to three bonds away; occasionally, even farther. This phenomenon is called spin–spin coupling or J-coupling. Coupling interactions are mutual and result in small changes in the absorption frequencies of both nuclei involved. While nuclei of the same element are involved...
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Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

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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 Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

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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...
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Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

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

1.7K
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...
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Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)01:22

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

1.5K
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...
1.5K
Atomic Nuclei: Nuclear Spin01:08

Atomic Nuclei: Nuclear Spin

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All atomic particles possess an intrinsic angular momentum, or 'spin'. Electrons, protons, and neutrons each have a spin value of ½, although protons and neutrons in nuclei may have higher half-integer spins owing to energetic factors.
Atomic nuclei have a net nuclear spin, , which can have an integer or half-integer value. In atomic nuclei, the spins of protons are paired against each other but not with neutrons, and vice versa. Consequently, an even number of protons does not contribute to...
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Study of Protein Dynamics via Neutron Spin Echo Spectroscopy
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A general spin-complete spin-flip configuration interaction method.

Joani Mato1, Mark S Gordon

  • 1Department of Chemistry, Iowa State University, Ames, IA 50011, USA. mark@si.msg.chem.iastate.edu.

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|January 11, 2018
PubMed
Summary
This summary is machine-generated.

A new spin-flip configuration interaction (SF-CI) method, SF-ORMAS, accurately models complex electronic structures. This method extends existing techniques to study bond breaking, diradicals, and excitations, enhancing computational chemistry capabilities.

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Area of Science:

  • Quantum Chemistry
  • Computational Chemistry
  • Theoretical Chemistry

Background:

  • Accurate electronic structure calculations are crucial for understanding chemical phenomena.
  • Existing methods may struggle with systems exhibiting significant static correlation, such as diradicals or bond breaking processes.
  • The development of versatile computational methods is essential for advancing chemical research.

Purpose of the Study:

  • Introduce a novel, general spin-correct spin-flip configuration interaction (SF-CI) method.
  • Extend the occupation-restricted multiple active spaces (ORMAS) CI method to incorporate spin-flip excitations.
  • Provide a flexible computational tool for studying diverse chemical systems with varying multiplicities.

Main Methods:

  • Developed the spin-flip occupation-restricted multiple active spaces (SF-ORMAS) method within the GAMESS computational chemistry package.
  • Employed a single reference, high-spin restricted open-shell determinant as the starting point.
  • Incorporated spin-flipped excitations to generate wave functions of desired multiplicity.
  • Included dynamic correlation effects via perturbation theory.

Main Results:

  • Demonstrated the efficacy of SF-ORMAS for single and multiple bond breaking scenarios.
  • Successfully characterized diradical systems using the new methodology.
  • Applied the method to calculate vertical excitations in linear alkenes.
  • Computed the singlet-triplet energy gap for silicon trimer.

Conclusions:

  • The SF-ORMAS method offers a versatile and accurate approach for electronic structure calculations.
  • The flexibility in active space design allows tailored application to specific chemical problems.
  • The method successfully addresses challenges in systems with significant static correlation and varying spin states.