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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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Entropy01:18

Entropy

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The first law of thermodynamics is quantitatively formulated via an equation relating the internal energy of a system, the heat exchanged by it, and the work done on it. A quantitative formulation of the second law of thermodynamics leads to defining a state function, the entropy.
When an ideal gas expands isothermally, the disorder in the gas increases. From the molecular perspective, the gas molecules have more volume to move around in.
Consider an infinitesimal step in the expansion, which...
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Atomic Nuclei: Nuclear Relaxation Processes01:23

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In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis,  the precessing magnetic moments are randomly oriented around the z-axis.
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Phase Transitions: Vaporization and Condensation02:39

Phase Transitions: Vaporization and Condensation

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The physical form of a substance changes on changing its temperature. For example, raising the temperature of a liquid causes the liquid to vaporize (convert into vapor). The process is called vaporization—a surface phenomenon. Vaporization occurs when the thermal motion of the molecules overcome the intermolecular forces, and the molecules (at the surface) escape into the gaseous state. When a liquid vaporizes in a closed container, gas molecules cannot escape. As these gas phase molecules...
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Atomic Spectroscopy: Effects of Temperature01:27

Atomic Spectroscopy: Effects of Temperature

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Atomization, converting samples into gas-phase atoms and ions, is essential for atomic spectroscopy. The flame temperature required for atomization affects the efficiency of the atomic spectroscopic methods by increasing the atomization efficiency and the relative population of the excited and ground states.
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Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

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Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
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Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
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Cooling Atomic Gases With Disorder.

Thereza Paiva1, Ehsan Khatami2, Shuxiang Yang3

  • 1Departamento de Física dos Sólidos, Instituto de Física, Universidade Federal do Rio de Janeiro, 21945-970 Rio de Janeiro, Rio de Janeiro, Brazil.

Physical Review Letters
|December 27, 2015
PubMed
Summary
This summary is machine-generated.

Researchers propose a novel method using disordered potentials and constant entropy trajectories to achieve low temperatures in cold atomic gases. This approach enables the exploration of magnetism and superconductivity in fermionic atom lattices, approaching the Néel temperature for the 3D Hubbard model.

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Area of Science:

  • Quantum simulation
  • Condensed matter physics
  • Cold atomic gases

Background:

  • Cold atomic gases emulate phenomena like Bose-Einstein condensation and the quantum Hall effect.
  • Achieving low temperatures for magnetism and superconductivity in fermionic atom lattices is challenging.

Purpose of the Study:

  • To propose a method for producing low-temperature cold atomic gases.
  • To enable the study of magnetism and exotic superconductivity in fermionic atom lattices.
  • To explore incompletely understood quantum phases.

Main Methods:

  • Preparing cold atomic gases in a disordered potential.
  • Utilizing a constant entropy trajectory to transition to a nondisordered state.
  • Employing quantum Monte Carlo simulations.

Main Results:

  • The proposed method can approach the Néel temperature of the three-dimensional Hubbard model.
  • Simulations show feasibility for experimentally achievable parameters.
  • The required randomness is in a regime where atom transport and equilibration are robust.

Conclusions:

  • The proposed method offers a viable pathway to low-temperature regimes for studying quantum magnetism and superconductivity.
  • This technique facilitates the investigation of exotic phases in fermionic atom systems.
  • Quantum Monte Carlo simulations validate the approach for future experimental exploration.