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Related Concept Videos

Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

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...
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...
The Pauli Exclusion Principle03:06

The Pauli Exclusion Principle

The arrangement of electrons in the orbitals of an atom is called its electron configuration. We describe an electron configuration with a symbol that contains three pieces of information:
Double Resonance Techniques: Overview01:12

Double Resonance Techniques: Overview

Double resonance techniques in Nuclear Magnetic Resonance (NMR) spectroscopy involve the simultaneous application of two different frequencies or radiofrequency pulses to manipulate and observe two distinct nuclear spins. One important application of double resonance is spin decoupling, which selectively suppresses coupling with one type of nucleus while observing the NMR signal from another nucleus, simplifying the spectrum and enhancing resolution.
Spin decoupling is usually achieved by...
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

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 have a...
Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

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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Site Directed Spin Labeling and EPR Spectroscopic Studies of Pentameric Ligand-Gated Ion Channels
11:19

Site Directed Spin Labeling and EPR Spectroscopic Studies of Pentameric Ligand-Gated Ion Channels

Published on: July 4, 2016

Treating molecules in arbitrary spin states using the parametric two-electron reduced-density-matrix method.

Christine A Schwerdtfeger1, David A Mazziotti

  • 1Department of Chemistry and The James Franck Institute, The University of Chicago, Chicago, Illinois 60637, USA.

The Journal of Chemical Physics
|July 27, 2012
PubMed
Summary
This summary is machine-generated.

The M parametric two-electron reduced density matrix (2-RDM) method accurately describes molecules in various spin states, capturing more electron correlation energy than coupled cluster methods with lower computational cost.

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Area of Science:

  • Quantum Chemistry
  • Computational Chemistry
  • Electronic Structure Theory

Background:

  • Parametric variational 2-RDM methods minimize electronic energy using parameterized 2-RDMs.
  • The M 2-RDM parametrization offers a computationally efficient approach to electronic structure calculations.

Purpose of the Study:

  • Extend the M parametric 2-RDM method to handle molecules in arbitrary spin states.
  • Evaluate the accuracy and efficiency of the extended method for describing molecular properties.

Main Methods:

  • Utilized approximate N-representability conditions to derive the M parametric 2-RDM method for arbitrary spin states.
  • Compared results with the K parametric 2-RDM method and various wavefunction methods.

Main Results:

  • The M method accurately describes bond breaking in open-shell molecules (e.g., triplet B2, OH+) even with strong correlation.
  • Achieved higher correlation energy capture than coupled cluster with single and double excitations (CCSD) at a lower computational cost.
  • Computed 2-RDMs demonstrated near N-representability across different geometries.

Conclusions:

  • The extended M parametric 2-RDM method provides a robust and efficient tool for studying molecules in diverse spin states.
  • This approach offers a promising alternative for electronic structure calculations, particularly for systems with strong electron correlation.