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Lecture 5 Ideal Gases of Bosons and Fermions

Lecture 5 Ideal Gases of Bosons and Fermions

Lecture 5 Ideal Gases of Bosons and Fermions. Dhani Herdiwijaya v1.0. We have considered systems with a fixed number of particles at low particle densities , n << n Q . We allowed these systems to exchange only energy with the environment/reservoir

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556 views • 43 slides
4. The rotating mean field

4. The rotating mean field

4. The rotating mean field. The mean field is a functional of the single particle states determined by an averaging procedure. The mean field concept. A nucleon moves in the mean field generated by all nucleons. The nucleons move independently.

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336 views • 24 slides
The Gibbs Factor

The Gibbs Factor

Lecture 23. Systems with a Variable Number of Particles. Ideal Gases of Bosons and Fermions (Ch. 7).

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453 views • 20 slides
The Gibbs Factor

The Gibbs Factor

Lecture 23. Systems with a Variable Number of Particles. Ideal Gases of Bosons and Fermions (Ch. 7).

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513 views • 20 slides
Treatment of Correlation Effects in Electron Momentum Density: Natural Orbital Functional Theory

Treatment of Correlation Effects in Electron Momentum Density: Natural Orbital Functional Theory

Treatment of Correlation Effects in Electron Momentum Density: Natural Orbital Functional Theory. B. Barbiellini Northeastern University. Overview . Beyond the IPA: many-body wave function ?. Is the concept of one-electron orbital still meaningful ?

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406 views • 18 slides
Lecture 21. Grand canonical ensemble (Ch. 7)

Lecture 21. Grand canonical ensemble (Ch. 7)

Lecture 21. Grand canonical ensemble (Ch. 7). Reservoir R U 0 - ?. Boltzmann statistics ( T, V, N ) :. System S ?. Plan : we want to generalize this result to the case where both energy and particles can be exchanged with the environment. Reservoir U R , N R , T , ?. System E , N.

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151 views • 14 slides

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