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A pure, perfectly crystalline solid possessing no kinetic energy (that is, at a temperature of absolute zero, 0 K) may be described by a single microstate, as its purity, perfect crystallinity,and complete lack of motion means there is but one possible location for each identical atom or molecule comprising the crystal (W = 1). According to the Boltzmann equation, the entropy of this system is zero.
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Understanding the stability of equilibrium configurations is a fundamental part of mechanical engineering. In any system, there are three distinct types of equilibrium: stable, neutral, and unstable.
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Entropy02:39

Entropy

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Salt particles that have dissolved in water never spontaneously come back together in solution to reform solid particles. Moreover, a gas that has expanded in a vacuum remains dispersed and never spontaneously reassembles. The unidirectional nature of these phenomena is the result of a thermodynamic state function called entropy (S). Entropy is the measure of the extent to which the energy is dispersed throughout a system, or in other words, it is proportional to the degree of disorder of a...
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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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Entropy and the Second Law of Thermodynamics01:20

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The second law of thermodynamics can be stated quantitatively using the concept of entropy. Entropy is the measure of disorder of the system.
The relation  between entropy and disorder can be illustrated with the example of the phase change of ice to water. In ice, the molecules are located at specific sites giving a solid state, whereas, in a liquid form, these molecules are much freer to move. The molecular arrangement has therefore become more randomized. Although the change in average...
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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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Updated: May 26, 2025

Visually Based Characterization of the Incipient Particle Motion in Regular Substrates: From Laminar to Turbulent Conditions
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Many-Body Adiabatic Passage: Instability, Chaos, and Quantum Classical Correspondence.

Anant Vijay Varma1,2, Amichay Vardi2,3, Doron Cohen1

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Interactions and entanglement significantly impact adiabatic passage in interacting bosons. This study reveals classical and quantum chaos in Bose-Hubbard chains using stimulated Raman adiabatic passage, confirmed across multiple simulation methods.

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Area of Science:

  • Quantum physics
  • Condensed matter physics
  • Quantum chaos

Background:

  • Adiabatic passage is crucial for quantum control but is sensitive to interactions and entanglement.
  • Bose-Hubbard chains are a key model for studying interacting bosons and quantum phenomena.
  • Chaos in quantum systems, particularly in interacting many-body systems, remains an active area of research.

Purpose of the Study:

  • To investigate the influence of interactions and entanglement on adiabatic passage in Bose-Hubbard chains.
  • To explore the emergence of classical and quantum chaos in these systems under stimulated Raman adiabatic passage protocols.
  • To compare the manifestation of chaos across different theoretical treatments.

Main Methods:

  • Simulations of stimulated Raman-adiabatic-passage-like schemes in Bose-Hubbard chains.
  • Analysis of low-dimensional chaos (three-site chain) and high-dimensional chaos (more than three sites).
  • Utilizing mean-field classical treatment, truncated Wigner semiclassical treatment, and full many-body quantum simulations.

Main Results:

  • Adiabatic passage dynamics in Bose-Hubbard chains exhibit clear fingerprints of classical and quantum chaos.
  • Chaos is observed in both low-dimensional (three-site) and high-dimensional (many-site) chaotic regimes.
  • These chaotic signatures are consistently found across mean-field, semiclassical, and full quantum simulations.

Conclusions:

  • Interactions and entanglement fundamentally alter adiabatic passage in interacting bosons, leading to chaotic dynamics.
  • Stimulated Raman adiabatic passage protocols can effectively reveal classical and quantum chaos in Bose-Hubbard models.
  • The observed chaos is robust and consistently detectable through various theoretical and computational approaches.