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The de Broglie Wavelength02:32

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In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
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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.
In the case of a non-isolated system, the change in the internal energy is zero only if the process is cyclic. A thermodynamic process is considered cyclic if the system undergoes a series of changes and returns to its initial state. 
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Entropy Change in Reversible Processes01:10

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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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The Bohr Model02:18

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Following the work of Ernest Rutherford and his colleagues in the early twentieth century, the picture of atoms consisting of tiny dense nuclei surrounded by lighter and even tinier electrons continually moving about the nucleus was well established. This picture was called the planetary model since it pictured the atom as a miniature “solar system” with the electrons orbiting the nucleus like planets orbiting the sun. The simplest atom is hydrogen, consisting of a single proton as...
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First Law: Particles in One-dimensional Equilibrium01:10

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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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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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Related Experiment Video

Updated: Jul 1, 2025

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
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Ergodicity breaking from Rydberg clusters in a driven-dissipative many-body system.

Dongsheng Ding1,2, Zhengyang Bai3, Zongkai Liu1,2

  • 1Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, Anhui 230026, China.

Science Advances
|March 4, 2024
PubMed
Summary

Rydberg atoms demonstrate a shift from ergodic to ergodicity-breaking dynamics, showing long-time oscillations due to Rydberg excitation clusters. This reveals their potential for studying quantum many-body systems and phase transitions.

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Area of Science:

  • Quantum many-body physics
  • Atomic physics
  • Condensed matter physics

Background:

  • Probing ergodicity breaking in quantum systems is difficult due to dissipation damaging quantum coherence.
  • Rydberg atoms offer a platform to study exotic phases and non-ergodic dynamics, where interactions can overcome dissipation.

Purpose of the Study:

  • To experimentally investigate ergodicity breaking dynamics in driven-dissipative Rydberg atomic gases.
  • To identify the features and underlying mechanisms of broken ergodicity in these systems.

Main Methods:

  • Utilizing Rydberg atoms in a driven-dissipative setup.
  • Observing dynamics at room temperature, highlighting the role of strong Rydberg interactions.
  • Experimentally tuning atomic densities to verify collective effects.

Main Results:

  • Experimental evidence of a transition from ergodic to ergodicity-breaking dynamics.
  • Observation of long-time phase oscillations, indicative of broken ergodicity.
  • Attribution of broken ergodicity to Rydberg excitation clusters forming limit cycles and broken symmetry.

Conclusions:

  • Rydberg many-body systems are suitable for probing ergodicity breaking dynamics, including limit cycles.
  • These systems provide a platform for benchmarking nonequilibrium phase transitions.
  • Collective effects in Rydberg systems are crucial for observing broken symmetry and non-ergodic behavior.