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Related Concept Videos

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

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

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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...
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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.
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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NMR Spectroscopy: Spin–Spin Coupling01:08

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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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Valence Bond Theory02:42

Valence Bond Theory

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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...
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Current density functional framework for spin-orbit coupling: Extension to periodic systems.

Yannick J Franzke1, Christof Holzer2

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|May 8, 2024
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Summary
This summary is machine-generated.

Spin-orbit coupling necessitates new meta-generalized gradient approximations that include current density. This study generalizes spin-orbit current density functional theory for periodic systems, impacting calculations of material properties.

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Area of Science:

  • Quantum Chemistry
  • Condensed Matter Physics
  • Materials Science

Background:

  • Spin-orbit coupling (SOC) is crucial for understanding electronic properties in materials.
  • Current density in the ground state necessitates advanced density functional approximations.
  • Existing meta-generalized gradient approximations (meta-GGAs) do not fully account for SOC-induced current densities.

Purpose of the Study:

  • To generalize the spin-orbit current density functional theory (SOC-CDFT) formalism.
  • To extend the formalism to non-magnetic and magnetic periodic systems of arbitrary dimensions.
  • To implement analytical derivatives for calculating geometry gradients and stress tensors.

Main Methods:

  • Generalization of meta-generalized gradient approximations to include current density.
  • Development of a formalism for spin-orbit current density functional theory in periodic systems.
  • Implementation of analytical derivatives for geometry optimization and stress tensor calculations.

Main Results:

  • The generalized SOC-CDFT formalism is applicable to periodic systems.
  • Analytical derivatives enable efficient structural property calculations.
  • The impact of current density on band gaps, lattice constants, magnetic transitions, and Rashba splittings is quantified.

Conclusions:

  • The developed SOC-CDFT provides a more accurate description of electronic properties in periodic systems.
  • Current density plays a significant role in various material properties, sometimes exceeding differences between standard DFT approximations.
  • This work offers a robust theoretical framework for studying SOC effects in condensed matter systems.