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Related Concept Videos

Group Polarization01:01

Group Polarization

Group polarization is the strengthening of an original group attitude following the discussion of views within a group (Teger & Pruitt, 1967). That is, if a group initially favors a viewpoint, after discussion the group consensus is likely a stronger endorsement of the viewpoint. Conversely, if the group was initially opposed to a viewpoint, group discussion would likely lead to stronger opposition.
¹H NMR: Complex Splitting01:13

¹H NMR: Complex Splitting

A proton M that is coupled to a proton X results in doublet signals for M. However, NMR-active nuclei can be simultaneously coupled to more than one nonequivalent nucleus. When M is coupled to a second proton A, such as in styrene oxide, each peak in the doublet is split into another doublet.
Splitting diagrams or splitting tree diagrams are routinely used to depict such complex couplings. While drawing splitting diagrams, the splitting with the larger coupling constant is usually applied first.
Potential Due to a Polarized Object01:29

Potential Due to a Polarized Object

A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
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.
Structure of Benzene: Kekulé Model01:07

Structure of Benzene: Kekulé Model

In 1865, August Kekule suggested the structure of benzene according to the structural theory of organic chemistry based on the three assertions—formula of benzene is C6H6, all the hydrogens of benzene are equivalent, and each carbon must have four bonds due to its tetravalency.
He proposed that benzene has a cyclic structure of six carbon atoms attached to one hydrogen atom each, with three alternating pi bonds.
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...

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A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference
07:56

A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference

Published on: September 5, 2019

Linear complex polarization propagator in a four-component Kohn-Sham framework.

Sebastien Villaume1, Trond Saue, Patrick Norman

  • 1Department of Physics, Chemistry and Biology, Linköping University, SE-581 83 Linköping, Sweden.

The Journal of Chemical Physics
|August 17, 2010
PubMed
Summary
This summary is machine-generated.

A new algorithm solves complex linear response equations for advanced spectroscopy. This method accurately calculates electric dipole dispersion coefficients for rubidium and cesium dimers.

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Area of Science:

  • Computational chemistry
  • Quantum mechanics
  • Spectroscopy

Background:

  • Linear response theory is crucial for understanding molecular properties.
  • Existing methods face challenges with complex frequency arguments and relaxation channels.
  • Polarization propagator approaches require robust equation solvers.

Purpose of the Study:

  • To present a novel algorithm for solving linear response equations in the random phase approximation.
  • To enable calculations involving complex frequency arguments and nonstimulated relaxation.
  • To validate the algorithm's stability and robustness in spectroscopic applications.

Main Methods:

  • Developed a complex-valued algorithm for linear response equations.
  • Implemented the algorithm within a four-component relativistic, noncollinear, density functional theory framework.
  • Applied the method to calculate electric dipole dispersion coefficients (C(6)) for diatomic molecules.

Main Results:

  • Demonstrated the algorithm's stability and robustness across visible, ultraviolet, and X-ray spectroscopies.
  • Successfully computed C(6) coefficients for rubidium (Rb2) and cesium (Cs2) dimers.
  • Obtained highly accurate C(6) values: 14.0x10^3 a.u. for Rb2 and 21.9x10^3 a.u. for Cs2.

Conclusions:

  • The presented algorithm is a stable and robust solver for complex linear response equations.
  • The method accurately determines electric dipole dispersion coefficients for molecular dimers.
  • This work advances computational methods for spectroscopic analysis and intermolecular interactions.