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Related Concept Videos

Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

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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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The Quantum-Mechanical Model of an Atom02:45

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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.
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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...
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The difference between the calculated and experimentally measured masses is known as the mass defect of the atom. In the case of helium-4, the mass defect indicates a “loss” in mass of 4.0331 amu – 4.0026 amu = 0.0305 amu. The loss in mass accompanying the formation of an atom from protons, neutrons, and electrons is due to the conversion of that mass into energy that is evolved as the atom forms. The nuclear binding energy is the energy produced when the atoms’ nucleons...
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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.
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Gradient Echo Quantum Memory in Warm Atomic Vapor
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Accurate nuclear quantum statistics on machine-learned classical effective potentials.

Iryna Zaporozhets1,2,3, Félix Musil1, Venkat Kapil4,5,6

  • 1Department of Physics, Freie Universität Berlin, Arnimallee 12, 14195 Berlin, Germany.

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|October 1, 2024
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Summary
This summary is machine-generated.

This study introduces a machine-learned potential to reduce computational costs for simulating nuclear quantum effects (NQEs) in molecular dynamics. The method accurately captures NQEs in various systems, enabling efficient simulations of complex molecular properties.

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Area of Science:

  • Computational chemistry
  • Molecular dynamics
  • Machine learning in science

Background:

  • Nuclear quantum effects (NQEs) significantly influence hydrogen-bound systems, including biomolecules.
  • Simulating NQEs using path integral molecular dynamics (PIMD) is computationally expensive, especially for complex systems at low temperatures.

Purpose of the Study:

  • To develop a computationally efficient method for incorporating NQEs in molecular simulations.
  • To reduce the computational burden of PIMD by employing machine learning techniques.

Main Methods:

  • Leveraging deep learning and multiscale coarse-graining.
  • Developing a machine-learned potential to represent corrections to classical potentials.
  • Validating the approach on four distinct systems: Morse potential, Zundel cation, single water molecule, and bulk water.

Main Results:

  • The machine-learned potential accurately represents corrections to classical potentials, significantly reducing computational cost.
  • The framework accurately computes position-dependent static properties, showing excellent agreement with PIMD calculations.
  • The approach effectively captures strong NQEs in the tested systems.

Conclusions:

  • The developed framework offers a computationally feasible way to simulate NQEs in molecular systems.
  • This work paves the way for transferable machine-learned potentials for accurate NQE simulations across diverse molecular systems.