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Related Concept Videos

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: 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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Atomic Nuclei: Nuclear Spin State Population Distribution01:14

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Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
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Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

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In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis,  the precessing magnetic moments are randomly oriented around the z-axis.
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Atomic Nuclei: Nuclear Spin State Overview01:03

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NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...
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A state interaction spin-orbit coupling density matrix renormalization group method.

Elvira R Sayfutyarova1, Garnet Kin-Lic Chan1

  • 1Department of Chemistry, Princeton University, Princeton, New Jersey 08540, USA.

The Journal of Chemical Physics
|June 24, 2016
PubMed
Summary
This summary is machine-generated.

We introduce a novel state interaction spin-orbit (SISO) coupling method using density matrix renormalization group (DMRG) and spin-orbit mean-field (SOMF) for accurate electronic structure calculations. This method precisely determines spin-orbit coupling effects in atoms and molecular complexes.

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Area of Science:

  • Quantum Chemistry
  • Computational Physics
  • Electronic Structure Theory

Background:

  • Accurate calculation of spin-orbit coupling (SOC) is crucial for understanding electronic properties of atoms and molecules.
  • Existing methods may face challenges with computational cost or accuracy for complex systems.
  • Density matrix renormalization group (DMRG) is a powerful tool for strongly correlated systems.

Purpose of the Study:

  • To develop and implement a novel State Interaction Spin-Orbit (SISO) coupling method.
  • To integrate DMRG wavefunctions with the spin-orbit mean-field (SOMF) operator for enhanced accuracy.
  • To benchmark the DMRG-SISO scheme against established methods for atomic and molecular systems.

Main Methods:

  • Implementation of a spin-adapted algorithm for computing transition density matrices between matrix product states.
  • Application of the DMRG-SISO scheme to calculate zero-field splitting (ZFS) in copper and gold atoms.
  • Computation of SOC effects on the spin-ladder states of an iron-sulfur dimer complex.

Main Results:

  • Accurate benchmark calculations for the zero-field splitting of copper and gold atoms were performed.
  • Comparison with complete active space self-consistent-field (CASSCF) and second-order complete active space perturbation theory (CASPT2) showed good agreement.
  • The study determined the splitting of the lowest quartet and sextet states for the iron-sulfur dimer complex.

Conclusions:

  • The developed DMRG-SISO scheme provides accurate results for spin-orbit coupling effects.
  • The method shows significant potential for studying electronic structures of complex molecular systems.
  • The magnitude of ZFS for higher states in the iron-sulfur dimer approaches a substantial fraction of the Heisenberg exchange parameter.