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Entropy02:39

Entropy

30.8K
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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Third Law of Thermodynamics02:38

Third Law of Thermodynamics

19.4K
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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Entropy and the Second Law of Thermodynamics01:20

Entropy and the Second Law of Thermodynamics

3.1K
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...
3.1K
Second Law of Thermodynamics02:49

Second Law of Thermodynamics

24.3K
In the quest to identify a property that may reliably predict the spontaneity of a process, a promising candidate has been identified: entropy. Processes that involve an increase in entropy of the system (ΔS > 0) are very often spontaneous; however, examples to the contrary are plentiful. By expanding consideration of entropy changes to include the surroundings, a significant conclusion regarding the relation between this property and spontaneity may be reached. In thermodynamic...
24.3K
Entropy Change in Reversible Processes01:10

Entropy Change in Reversible Processes

2.7K
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.
The statement can be further generalized to prove that entropy is a state function. Take a cyclic process between any two points on a p-V diagram.
2.7K
The Second Law of Thermodynamics01:14

The Second Law of Thermodynamics

5.5K
In the quest to identify a property that may reliably predict the spontaneity of a process, a promising candidate has been identified: entropy. Scientists refer to the measure of randomness or disorder within a system as entropy. High entropy means high disorder and low energy. To better understand entropy, think of a student’s bedroom. If no energy or work were put into it, the room would quickly become messy. It would exist in a very disordered state, one of high entropy. Energy must be...
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Related Experiment Video

Updated: Sep 4, 2025

A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference
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A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference

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Universal Feature of Charged Entanglement Entropy.

Pablo Bueno1, Pablo A Cano2, Ángel Murcia3

  • 1CERN, Theoretical Physics Department, CH-1211 Geneva 23, Switzerland.

Physical Review Letters
|July 22, 2022
PubMed
Summary
This summary is machine-generated.

Charged Rényi entropies generalize entanglement entropy using a chemical potential. For conformal field theories, the leading correction to entanglement entropy is quadratic in this potential, universally controlled by specific coefficients.

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Area of Science:

  • Quantum Field Theory
  • Statistical Mechanics
  • String Theory

Background:

  • Rényi entropies generalize entanglement entropy and can be extended to include global symmetries.
  • These 'charged Rényi entropies' depend on a chemical potential conjugate to the charge within the entangling region.
  • For n=1, this yields a concept of charged entanglement entropy.

Purpose of the Study:

  • To prove that the leading correction to uncharged entanglement entropy in general d(>=3)-dimensional conformal field theories (CFTs) is universally controlled.
  • To establish the dependence of this correction on the chemical potential and specific CFT coefficients.
  • To connect these findings with holographic calculations and properties of twist operators.

Main Methods:

  • Derivation for general d-dimensional CFTs using universal identities related to twist operator magnetic response.
  • Analytic holographic calculations in higher-curvature gravities and for free fields in d=4.
  • Application of basic thermodynamic relations.

Main Results:

  • The leading correction to entanglement entropy across a spherical surface in CFTs is quadratic in the chemical potential.
  • This correction is positive definite and universally controlled by coefficients C_J and a_2.
  • These coefficients characterize current correlators and energy flux.

Conclusions:

  • The study provides a universal formula for the leading correction to entanglement entropy in CFTs.
  • The results are consistent with holographic models and offer insights into quantum information in curved spacetimes.
  • This work establishes a fundamental relationship between entanglement, symmetries, and gravitational phenomena in CFTs.