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Related Concept Videos

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.
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...
¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are slanted or...
Atomic Nuclei: Nuclear Spin01:08

Atomic Nuclei: Nuclear Spin

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...
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...
Atomic Radii and Effective Nuclear Charge03:08

Atomic Radii and Effective Nuclear Charge

The elements in groups of the periodic table exhibit similar chemical behavior. This similarity occurs because the members of a group have the same number and distribution of electrons in their valence shells.

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In Situ Monitoring of Diffusion of Guest Molecules in Porous Media Using Electron Paramagnetic Resonance Imaging
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Published on: September 2, 2016

Accurate ab Initio Spin Densities.

Katharina Boguslawski, Konrad H Marti, Ors Legeza

    Journal of Chemical Theory and Computation
    |June 19, 2012
    PubMed
    Summary
    This summary is machine-generated.

    This study introduces a new method using density-matrix renormalization group (DMRG) to calculate spin density distributions for complex molecules. This approach accurately describes electronic structures requiring large active spaces.

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    Published on: January 25, 2020

    Area of Science:

    • Quantum Chemistry
    • Computational Chemistry
    • Materials Science

    Background:

    • Accurate electronic structure calculations are crucial for understanding molecular properties.
    • Molecules with large active spaces pose significant challenges for traditional computational methods.
    • Spin density distributions provide key insights into molecular electronic behavior.

    Purpose of the Study:

    • To develop a robust method for calculating spin density distributions in molecules with large active spaces.
    • To enhance the accuracy and applicability of the density-matrix renormalization group (DMRG) algorithm.
    • To provide a computationally feasible approach for complex electronic structure problems.

    Main Methods:

    • Utilizing the density-matrix renormalization group (DMRG) algorithm to compute spin density matrix elements.
    • Employing a sampling-reconstruction scheme for analytic convergence of spin density distributions.
    • Reconstructing complete-active-space configuration-interaction (CASCI) wave functions from matrix product states.

    Main Results:

    • The DMRG-based approach successfully calculates spin density distributions for challenging molecular systems.
    • The sampling-reconstruction scheme provides an accurate convergence criterion.
    • Reconstructed CASCI wave functions offer detailed insights into electron distribution (alpha and beta electrons).

    Conclusions:

    • The presented methodology offers a powerful tool for studying the electronic structure of complex molecules.
    • This approach overcomes limitations of standard methods for systems requiring large active spaces.
    • The technique provides valuable chemical insights into electron behavior and spin properties.