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Related Concept Videos

Fermi Level01:18

Fermi Level

The Fermi-Dirac function is represented by an S-shaped curve indicating the probability of an energy state being occupied by an electron at a given temperature. The Fermi level is the energy level at which there is a fifty percent chance of finding an electron, and it is positioned between the lower-energy valence band and the higher-energy conduction band.
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
Second Uniqueness Theorem01:16

Second Uniqueness Theorem

Consider a region consisting of several individual conductors with a definite charge density in the region between these conductors. The second uniqueness theorem states that if the total charge on each conductor and the charge density in the in-between region are known, then the electric field can be uniquely determined.
In contrast, consider that the electric field is non-unique and apply Gauss's law in divergence form in the region between the conductors and the integral form to the surface...
Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

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.
Fermi Level Dynamics01:12

Fermi Level Dynamics

The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
The Zeroth Law of Thermodynamics01:14

The Zeroth Law of Thermodynamics

Systems in mechanical equilibrium exert equal pressure on the separating wall. Similarly, systems in thermal equilibrium share a common thermodynamic property: temperature.Temperature is a measure of the average kinetic energy of particles within a system. More generally, it reflects the internal energy state of the system. The higher the temperature, the more energy a system has, given that other variables, such as volume and pressure, remain constant. However, temperature is not a form of...
Entropy and the Second Law of Thermodynamics01:20

Entropy and the Second Law of Thermodynamics

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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Related Experiment Video

Updated: Jul 16, 2026

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
11:21

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

Universality in a 2-component fermi system at finite temperature.

Gautam Rupak1

  • 1Institute for Nuclear Theory, University of Washington, Seattle, Washington 98195, USA.

Physical Review Letters
|March 16, 2007
PubMed
Summary

Thermodynamic properties of Fermi systems near unitarity are universal. Calculations show the third virial coefficient is a universal number, relevant for neutron matter and atomic experiments.

Area of Science:

  • Quantum physics
  • Thermodynamics
  • Statistical mechanics

Background:

  • Understanding Fermi systems near the unitarity limit is crucial for nuclear physics and ultracold atomic gases.
  • Virial expansions are key for describing thermodynamic properties of dilute systems at high temperatures.
  • Universality in these properties suggests model-independent behavior.

Purpose of the Study:

  • To calculate the third virial coefficient (b3(T)) for a Fermi system at the unitarity limit.
  • To derive the energy density using virial expansion up to the third coefficient.
  • To explore the universality of thermodynamic properties in such systems.

Main Methods:

  • Model-independent finite temperature calculations.
  • Analysis of the virial expansion coefficients in the high-temperature Boltzmann regime.

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Related Experiment Videos

Last Updated: Jul 16, 2026

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
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Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

Angle-resolved Photoemission Spectroscopy At Ultra-low Temperatures
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Angle-resolved Photoemission Spectroscopy At Ultra-low Temperatures

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  • Focus on the unitarity limit where the 2-body scattering length approaches +/-infinity.
  • Main Results:

    • The third virial coefficient at the unitarity limit, b3(infinity), is found to be approximately 1.11, a universal number.
    • The energy density is derived up to the third virial expansion.
    • Demonstrated universality of virial coefficients for dilute Fermi systems.

    Conclusions:

    • The calculated universal value of b3(infinity) provides a benchmark for theoretical and experimental studies.
    • Findings are applicable to dilute neutron matter and can be experimentally verified in ultracold Fermi gases near Feshbach resonances.