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When an object is in equilibrium, it is either at rest or moving with a constant velocity. There are two types of equilibrium: static and dynamic. Static equilibrium occurs when an object is at rest, while dynamic equilibrium occurs when an object is moving with a constant velocity. In both cases, there must be a balance of forces acting on the object.
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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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Newton's first law of motion states that a body at rest remains at rest, or if in motion, remains in motion at constant velocity, unless acted on by a net external force. It also states that there must be a cause for any change in velocity (a change in either magnitude or direction) to occur. This cause is a net external force. For example, consider what happens to an object sliding along a rough horizontal surface. The object quickly grinds to a halt, due to the net force of friction. If...
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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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Related Experiment Video

Updated: Jun 30, 2025

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
11:21

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

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Single-quasiparticle eigenstate thermalization.

Piotr Tokarczyk1, Lev Vidmar2,3, Patrycja Łydżba1

  • 1Institute of Theoretical Physics, Wroclaw University of Science and Technology, 50-370 Wrocław, Poland.

Physical Review. E
|March 16, 2024
PubMed
Summary
This summary is machine-generated.

We introduce single-quasiparticle eigenstate thermalization for quantum chaotic Hamiltonians breaking U(1) symmetry. This explains the equilibration of observables in many-body systems after a quantum quench.

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Last Updated: Jun 30, 2025

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Area of Science:

  • Condensed Matter Physics
  • Quantum Chaos
  • Many-Body Systems

Background:

  • Quantum chaotic quadratic Hamiltonians exhibit single-particle eigenstate thermalization.
  • Previous studies focused on Hamiltonians with U(1) symmetry.

Purpose of the Study:

  • Investigate quantum chaotic Hamiltonians that break U(1) symmetry.
  • Introduce and study single-quasiparticle eigenstate thermalization.
  • Analyze the impact of disorder on near-zero modes and density of states.

Main Methods:

  • Focus on spinless fermion Hamiltonians in 3D with local hopping, pairing, and on-site disorder.
  • Introduce and analyze single-quasiparticle eigenstate thermalization.
  • Numerically simulate quantum quenches to observe equilibration of observables.

Main Results:

  • Defined single-quasiparticle eigenstate thermalization for U(1)-breaking systems.
  • Identified disorder-induced near-zero modes causing a density of states peak.
  • Demonstrated numerical equilibration of observables in many-body eigenstates after a quantum quench.

Conclusions:

  • Single-quasiparticle eigenstate thermalization explains observable equilibration in U(1)-breaking systems.
  • Findings extend the concept of eigenstate thermalization to a broader class of quantum chaotic systems.