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Experimentally, if object A is in equilibrium with object B, and object B is in equilibrium with object C, then object A is in equilibrium with object C. That statement of transitivity is called the "zeroth law of thermodynamics." For example, a cold metal block and a hot metal block are both placed on a metal plate at room temperature. Eventually, the cold block and the plate will be in thermal equilibrium. In addition, the hot block and the plate will be in thermal equilibrium.
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In the Carnot engine, which achieves the maximum efficiency between two reservoirs of fixed temperatures, the total change in entropy is zero. The observation can be generalized by considering any reversible cyclic process consisting of many Carnot cycles. Thus, it can be stated that the total entropy change of any ideal reversible cycle is zero.
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A thermodynamic system with zero heat exchange and work is an isolated system. For these systems, the internal energy remains constant.
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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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Whether solid, liquid, or gas, a substance's state depends on the order and arrangement of its particles (atoms, molecules, or ions). Particles in the solid pack closely together, generally in a pattern. The particles vibrate about their fixed positions but do not move or squeeze past their neighbors. In liquids, although the particles are closely spaced, they are randomly arranged. The position of the particles are not fixed—that is, they are free to move past their neighbors to...
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Related Experiment Video

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Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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Ergodicity Breaking Transition in Zero Dimensions.

Jan Šuntajs1, Lev Vidmar1

  • 1Department of Theoretical Physics, J. Stefan Institute, SI-1000 Ljubljana, Slovenia and Department of Physics, Faculty of Mathematics and Physics, University of Ljubljana, SI-1000 Ljubljana, Slovenia.

Physical Review Letters
|August 26, 2022
PubMed
Summary
This summary is machine-generated.

Researchers studied a quantum many-body system model to understand ergodicity breaking transitions. Numerical results confirmed the transition, offering insights into quantum system dynamics.

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Area of Science:

  • Quantum physics
  • Condensed matter theory
  • Statistical mechanics

Background:

  • Ergodicity breaking transitions are crucial in quantum many-body systems.
  • Toy models are essential for understanding complex quantum phenomena.
  • A variant model by De Roeck and Huveneers describes avalanche mechanisms in spin chains.

Purpose of the Study:

  • To establish and investigate a toy model exhibiting an ergodic to nonergodic transition.
  • To confirm the existence of this transition in the thermodynamic limit.
  • To benchmark properties characteristic of ergodicity breaking in finite systems.

Main Methods:

  • Studying a zero-dimensional model coupling an ergodic quantum dot with spin-1/2 particles.
  • Utilizing spectral form factor calculations for exact numerical analysis.
  • Comparing numerical results with theoretical predictions.

Main Results:

  • Exact numerical results from spectral form factor calculations show strong agreement with theoretical predictions.
  • The study unambiguously confirms the existence of an ergodicity breaking transition.
  • Key properties signaling the transition in finite systems were identified and benchmarked.

Conclusions:

  • The investigated model provides a valid framework for studying ergodicity breaking transitions.
  • The findings validate theoretical predictions and offer a tool for analyzing finite-size effects.
  • This work contributes to the fundamental understanding of ergodicity in quantum systems.