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Related Concept Videos

Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

1.1K
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.
1.1K
Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

697
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 Radii and Effective Nuclear Charge03:08

Atomic Radii and Effective Nuclear Charge

52.1K
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.
52.1K
The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

42.7K
Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
42.7K
¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

1.1K
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...
1.1K
Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

1.1K
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...
1.1K

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Second-Order Self-Consistent Field Algorithms: From Classical to Quantum Nuclei.

Robin Feldmann1, Alberto Baiardi1, Markus Reiher1

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|January 26, 2023
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Summary
This summary is machine-generated.

This study introduces a new framework for self-consistent field (SCF) orbital optimization using differential geometry. The augmented Roothaan-Hall (ARH) algorithm improves convergence for challenging electronic and nuclear-electronic calculations.

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Area of Science:

  • Computational chemistry
  • Quantum chemistry
  • Theoretical chemistry

Background:

  • Self-consistent field (SCF) methods are fundamental in quantum chemistry.
  • Convergence issues in SCF calculations, especially for strongly correlated systems and nuclear-electronic problems, hinder accurate molecular modeling.
  • Existing first-order optimization strategies often struggle with stability and efficiency.

Purpose of the Study:

  • To develop a general framework for deriving Newton SCF orbital optimization algorithms.
  • To extend the augmented Roothaan-Hall (ARH) algorithm to unrestricted electronic and nuclear-electronic calculations.
  • To demonstrate ARH's effectiveness in improving convergence and computational efficiency.

Main Methods:

  • Leveraging concepts from differential geometry to derive SCF orbital optimization algorithms.
  • Extending the augmented Roothaan-Hall (ARH) algorithm.
  • Applying ARH to unrestricted electronic calculations (e.g., iron-sulfur clusters) and nuclear-electronic calculations (e.g., protonated water clusters).

Main Results:

  • The ARH algorithm provides a balance between stability and computational cost for difficult SCF problems.
  • ARH successfully overcomes slow orbital convergence in strongly correlated electronic systems.
  • ARH significantly accelerates convergence in nuclear-electronic calculations, even for small molecules.

Conclusions:

  • The differential geometry-based framework offers a robust approach to SCF algorithm development.
  • The extended ARH algorithm is a powerful tool for tackling challenging convergence problems in computational chemistry.
  • ARH enhances the efficiency and applicability of SCF methods for complex molecular systems.