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Related Concept Videos

Chirality at Nitrogen, Phosphorus, and Sulfur02:30

Chirality at Nitrogen, Phosphorus, and Sulfur

Chirality is most prevalent in carbon-based tetrahedral compounds, but this important facet of molecular symmetry extends to sp3-hybridized nitrogen, phosphorus and sulfur centers, including trivalent molecules with lone pairs. Here, the lone pair behaves as a functional group in addition to the other three substituents to form an analogous tetrahedral center that can be chiral.
A consequence of chirality is the need for enantiomeric resolution. While this is theoretically possible for all...
Isotopes01:12

Isotopes

Elements have a set number of protons that determines their atomic number (Z). For example, all atoms with eight protons are oxygen; however, the number of neutrons can vary for atoms of the same element. The sum of the number of protons and the number of neutrons is the mass number (A). Atoms with the same atomic number but different mass numbers are called isotopes. Elements can have multiple isotopes, for example, carbon-12, carbon-13, and carbon-14.
An element's atomic mass, or weight, is a...
Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

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. This...
¹H NMR: Long-Range Coupling01:27

¹H NMR: Long-Range Coupling

The coupling interactions of nuclei across four or more bonds are usually weak, with J values less than 1 Hz. While these are usually not observed in spectra, the presence of multiple bonds along the coupling pathway can result in observable long-range coupling.
In alkenes, spin information is communicated via σ–π overlap, as seen in allylic (four-bond) and homoallylic (five-bond) couplings. These coupling interactions are stronger when the σ bond is parallel to the alkene π orbitals.
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.
¹³C NMR: ¹H–¹³C Decoupling01:04

¹³C NMR: ¹H–¹³C Decoupling

The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...

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Coulomb Explosion Imaging as a Tool to Distinguish Between Stereoisomers
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Published on: August 18, 2017

Isotopic chains around oxygen from evolved chiral two- and three-nucleon interactions.

A Cipollone1, C Barbieri, P Navrátil

  • 1Department of Physics, University of Surrey, Guildford GU2 7XH, United Kingdom.

Physical Review Letters
|August 27, 2013
PubMed
Summary

This study introduces a new method for nuclear physics calculations, incorporating three-body interactions to accurately predict isotope binding energies. The approach shows strong agreement with experimental data for oxygen and nitrogen isotopes.

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Area of Science:

  • Nuclear Physics
  • Quantum Many-Body Theory

Background:

  • Traditional nuclear models often simplify interactions, limiting accuracy for complex systems.
  • Accurate predictions of nuclear properties are crucial for understanding stellar evolution and nuclear reactions.

Purpose of the Study:

  • To extend self-consistent Green's function theory to include three-body interactions.
  • To apply this enhanced formalism to isotopic chains around oxygen.
  • To investigate the impact of three-nucleon forces on nuclear binding energies and driplines.

Main Methods:

  • Developed a formalism based on the third-order algebraic diagrammatic construction for two-body Hamiltonians.
  • Incorporated system-dependent one- and two-body interactions derived from three-body forces.
  • Applied the method to study chiral two- and three-nucleon forces at low momentum cutoffs.

Main Results:

  • Accurately reproduced binding energies for nitrogen, oxygen, and fluorine isotopes.
  • Demonstrated the predictive power of the formalism, especially for neutron-rich isotopes.
  • Successfully reproduced experimental driplines for oxygen and nitrogen isotopes.
  • Enabled calculation of form factors for nucleon transfer on doubly magic systems.

Conclusions:

  • The inclusion of three-body interactions significantly improves the accuracy of nuclear binding energy predictions.
  • The developed formalism provides a robust framework for studying nuclear structure and reactions.
  • This approach offers valuable insights into the behavior of neutron-rich nuclei and nuclear forces.