Lectures: Difference between revisions
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== Lecture 5: Degenerate fermions in equilibrium == | == Lecture 5: Degenerate fermions in equilibrium == | ||
*Example: Pressure of ideal Fermi | *Example: Pressure of ideal Fermi. | ||
*Example: Heat capacity of electrons in solids. | *Example: Heat capacity of electrons in solids. | ||
*Example: Pauli paramagnetism. | *Example: Pauli paramagnetism. |
Revision as of 15:39, 18 February 2011
Lecture 1: Failure of classical statistical mechanics
- Example: Planck theory of black-body radiation.
Additional references
Lecture 2: Mixed states in quantum mechanics and the density operator
- Example: Proper mixed states in spintronics.
- Example: Improper mixed states in decoherence of qubits and von Neumann entropy.
- Example: Proper mixed states for quantum systems in thermal equilibrium and density matrix for microcanonical, canonical, and grand canonical ensembles via correspondence with classical statistical mechanics.
- Example: Density matrix and quantum partition function for a single particle in a box in the quantum canonical ensemble.
- Example: Density matrix and quantum partition function for a linear harmonic oscillator in the quantum canonical ensemble.
Additional references
- J. K. Gamble and J. F. Lindner, Demystifying decoherence and the master equation of quantum Brownian motion, Am. J. Phys. 77, 244 (2009). [PDF]
- A. Ekert and P. L. Knight, Entangled quantum systems and the Schmidt decomposition, Am. J. Phys. 63, 415 (1995). [PDF]
Lecture 3: Many-particle wave functions and the Hilbert space of identical particles
- Example: Wave functions of 3 fermions and 3 bosons.
Lecture 4: Quantum partition function for many-particle systems in equilibrium
- Example: Quantum partition function for two bosons and two fermions and comparison with classical statistical mechanics.
- Example: "Effective force" between noninteracting bosons and fermions due to Pauli principle.
- Quantum partition function for non-interacting bosons and fermions in the grand canonical ensemble.
Additional references
- W. J. Mullin and G. Blaylock, Quantum statistics: Is there an effective fermion repulsion or boson attraction?, Am. J. Phys. 71, 1223 (2003). [PDF]
- G. Cook and R. H. Dickerson, Understanding the chemical potential, Am. J. Phys. 63, 737 (1995). [PDF]
Lecture 5: Degenerate fermions in equilibrium
- Example: Pressure of ideal Fermi.
- Example: Heat capacity of electrons in solids.
- Example: Pauli paramagnetism.
- Example: Landau diamagnetism.
- Example: Stoner ferromagnetism.
- Example: Neutron stars and black holes.
Lecture 6: Degenerate bosons in equilibrium
- Example: Heat capacity of phonons in solids.
- Example: Cosmic microwave background radiation.
- Example: Magnons in the Heisenberg model of magnetism.
Lecture 7: Bose-Einstein condensation
- Example: BEC for free noninteracting bosons.
- Example: BEC for trapped ultracold atom gases.
Additional references
- W. J. Mullin, The loop-gas approach to Bose–Einstein condensation for trapped particles, Am. J. Phys. 68, 120 (2000). [PDF]
Lecture 8: Magnetic systems
- Example: Noninteracting spins.
- Thermodynamics of magnetism.
- Example: Partition function of the Ising model in one-dimension.
- Example: Onsager solution and computer simulations of the Ising model in two-dimensions.
Lecture 9: Phase transitions
- Example: Phase diagrams of liquid-gas and paramagnet-ferromagnet systems.
- Thermodynamic equation of state near phase transitions.
Lecture 10: Mean-field theory of phase transitions
- Example: Mean-field theory of the Ising model of magnetism.
- Example: Mean-field theory of the Heisenberg model of magnetism and upper critical dimensionality.
- Example: Landau theory and the origin of its failure for two-dimensional Ising model.
Lecture 11: Critical phenomena and renormalization group (RG)
- Universality and scaling relations
- Example: Percolation as geometrical phase transition.
- Example: RG for percolation.
- Example: RG for 1D Ising model.
- Example: Niemeijer-van Leeuwen RG in real space for 2D Ising model.
- Additional references:
- M. E. Fisher, Renormalization group theory: Its basis and formulation in statistical physics, Rev. Mod. Phys. 70, 653 (1998). [PDF]
Lecture 12: Boltzmann (semiclassical) theory of linear response
- Example: Conductivity of massless Dirac fermions in 2D graphene.
Lecture 13: Kubo (quantum) theory of linear response
- Example: Conductivity of electrons in metals.
Lecture 14: Bogoliubov theory of superfluidity
Lecture 15: Introduction to quantum phase transitions
Additional references
- S. Sachdev and B. Keimer, Quantum criticality, Physics Today 64(2), 29 (2011). [PDF]