Statistical Mechanics II
Landau–Ginzburg theory, the scaling hypothesis and the renormalisation group.
What this course covers
- Statistical mechanics as microscopic-macroscopic bridge
- Collective behavior from interactions
- Statistical field theories and universality
- Normal modes and lattice vibrations
- Phonon dispersion and low-k linear behavior
- Universal low-temperature heat capacity from phonons
- Coarse graining and the continuum displacement field
- Constructing an effective elastic field theory from symmetry
- Isotropic elasticity in higher dimensions
- Elasticity as a statistical field theory
- Longitudinal and transverse modes in isotropic solids
- Low-temperature heat capacity and universality
- Phase transitions and the liquid-gas critical point
- Critical exponents (α, β, γ, δ)
- Critical opalescence and diverging correlation length
- Landau-Ginzburg effective field theory
- Landau-Ginzburg field theory construction
- Saddle-point (mean-field) approximation
- Mean-field critical exponents
- Spontaneous symmetry breaking
- Goldstone modes
- Landau-Ginzburg theory for superfluidity
- Phase fluctuation cost and Gaussian modes
- d-dimensional Coulomb potential
- Mermin-Wagner theorem and lower critical dimension
- Landau-Ginzburg free energy functional
- Scattering experiments and structure factor
- Gaussian fluctuations around the mean-field state
- Longitudinal vs. transverse susceptibility
- Fourier-space decomposition and mode independence
- Lorentzian scattering line shape and critical scattering
- Real-space correlation function and correlation length
- Divergence of the correlation length at T_c
- Scaling relation between γ, ν, and η (Fisher relation)
- Comparison of mean-field exponents with experiment
- Statistical field theory for phase transitions
- Critical exponent alpha and heat capacity singularities
- Saddle point approximation for the partition function
- Systematic expansion beyond saddle point
- Fourier decomposition of fluctuation fields
- Upper critical dimension d=4
- Failure of mean-field theory below d=4
- Ginzburg criterion for validity of mean-field theory
- Critical points and universality
- Failure of mean-field (saddle-point) exponents
- Scaling hypothesis for the free energy
- Gap exponent and crossover between singularities
- Exponent identities from the scaling hypothesis
- Scaling hypothesis for the correlation length
- Josephson (hyperscaling) relation
- Fisher identity and the exponent η
- Scale invariance at the critical point
- Critical points and universal scaling exponents
- Scale invariance and power-law correlations
- Renormalization group procedure: three steps
- RG transformation of probability weights
- RG flow equations and linearization near fixed point
- Deriving thermodynamic scaling from RG exponents
- General RG framework: parameter space and fixed points
- Eigenvalues, eigendirections, and relevant vs. irrelevant operators
- Basin of attraction and universality
- Number of relevant directions and experimental tunability
- Landau-Ginzburg statistical field theory
- Fourier representation and mode decoupling
- Gaussian model partition function and free energy
- Singular behavior and upper critical dimension
- Scaling form of the free energy and critical exponents
- Coarse-graining step of the RG procedure
- Rescaling and field renormalization steps
- RG eigenvalues and relevant vs. irrelevant operators
- Multiple fixed points and choice of rescaling factor z
- Relevance of the m⁴ term and need for perturbative RG
- Statistical field theory and partition function
- Landau-Ginzburg Gaussian model
- Fourier mode decomposition of the field
- Gaussian propagator and two-point correlator
- Wick's theorem for Gaussian averages
- Perturbation theory for interacting field theory
- Connected (cumulant) contractions via Wick's theorem
- Symmetry constraints on the two-point correlator
- Perturbative correction to susceptibility and shift of Tc
- Breakdown of perturbation theory below four dimensions
- Perturbation theory for partition functions
- Divergence of perturbation theory below four dimensions
- Momentum-shell coarse graining
- Perturbative expansion in the interaction vertex
- Wick's theorem and diagrammatic contractions
- Renormalization of the parameter t at first order
- Rescaling steps of the renormalization group
- Differential RG flow equations
- Fixed points and eigenvalue analysis
- Wilson-Fisher fixed point and epsilon expansion
- Partition function via statistical field theory
- Renormalization group coarse graining step
- Cumulant expansion of the effective Hamiltonian
- Diagrammatic representation of perturbation terms
- RG rescaling and renormalization steps
- Differential RG flow equations
- Gaussian fixed point and flow topology above d=4
- Need for epsilon expansion below d=4
- Second-order cumulant diagrams and u² corrections
- Wilson-Fisher (O(N)) fixed point
- Critical exponents from the O(N) fixed point
- Universal critical exponents near phase transitions
- Statistical field theory and order parameter symmetry
- Failure of saddle-point and perturbation theory below four dimensions
- Scaling hypothesis and exponent identities
- Kadanoff's renormalization group idea and fixed points
- Wilson's perturbative RG: integrating out shell modes
- RG flow equations for t and u
- Gaussian versus O(n) fixed points
- Computing critical exponents from RG eigenvalues
- Epsilon expansion and asymptotic series
- Lattice models and microscopic degrees of freedom
- Ising model
- O(N) spin models (XY and Heisenberg)
- Potts model and permutation symmetry
- Approaches to solving lattice models
- Position-space renormalization group in 1D
- RG recursion relations and fixed points for 1D Ising
- Correlation length and susceptibility near the 1D fixed point
- Why exact decimation fails in higher dimensions
- Transfer matrix method and exact solvability in 1D
- Renormalization group in 1D Ising model
- Challenges of RG on 2D lattices
- Niemeijer–van Leeuwen cumulant approximation
- Majority rule and cell-spin averaging
- Recursion relation and fixed point (triangular lattice)
- Critical exponents y_t and y_h from cell RG
- Migdal–Kadanoff bond-moving approximation
- Transfer matrix formulation of 1D models
- Absence of phase transitions in 1D via Perron–Frobenius
- Finite-size crossover and 2D phase transitions
- Ising model as universal spin model
- Low-temperature series expansion
- Energy and heat capacity from series
- Extracting critical exponents via ratio method
- Alternating signs and variable transformations
- High-temperature expansion and graph representation
- 1D Ising model: exact solution via graphs
- Ising model definition and setup
- Low-temperature expansion of the Ising model
- High-temperature expansion of the Ising model
- Duality of the square-lattice Ising model
- Self-duality and the exact critical point
- Duality beyond the square lattice
- Duality mapping to Z2 gauge theory in 3D
- Elitzur's theorem: no spontaneous breaking of local gauge symmetry
- Wilson loop as a non-local order parameter
- Confinement and asymptotic freedom from Wilson loop behavior
- High-temperature expansion of Ising partition function
- Gas of non-intersecting vs. phantom loops
- Counting random walks via transfer matrix
- Diagonalising the connectivity matrix by Fourier transform
- Spin–spin correlation function from walk counting
- Divergence of correlation length at the critical point
- Equivalence to the Gaussian (free-field) model
- Fractal dimension of random walks and the upper critical dimension
- Ising model partition function and graph expansion
- Phantom loop approximation and its failure
- Corrected loop sum with no-U-turn and crossing sign rules
- Whitney's theorem: crossing parity via tangent winding
- Oriented walk matrix with phase factors
- Explicit 4×4 one-step transfer matrix T*
- Fourier diagonalization to block-diagonal form
- Partition function as determinant integral
- High-temperature graphical expansion of Ising model
- Phantom loop approximation and its failure
- Exact loop expansion with no-backtrack and crossing sign
- Transfer-matrix and Fourier diagonalization
- Exact Ising partition function and its singularity structure
- Kramers–Wannier duality and the critical temperature
- Logarithmic divergence of the heat capacity (α = 0)
- Critical exponents of the 2D Ising model
- Fermionic (Grassmannian) interpretation of the 2D Ising model
- Low-temperature expansion and Goldstone modes in n-component models
- n-component unit spin vector model
- Ground state and Goldstone modes
- Integration measure and constraint on spin components
- Non-linear sigma model Hamiltonian
- Continuum limit and gradient expansion
- Temperature-ordered perturbative expansion
- Momentum-space Fourier representation and propagator
- Perturbative renormalization group procedure
- Diagrammatic evaluation of mode elimination
- Renormalization of the coupling constant K
- Physical interpretation: order vs. disorder in 2D
- Non-linear sigma model and spin field
- Transverse fluctuations and Goldstone modes
- Renormalization group procedure for spin models
- RG flow equation for coupling K and temperature T
- Fixed points and the 2+epsilon expansion
- Thermal and magnetic scaling exponents
- Correlation length divergence in 2D Heisenberg model
- Mermin-Wagner theorem and the n=2 puzzle
- Spin-spin correlation functions: high vs low temperature
- Topological defects (vortices) in the XY model
- Vortex-antivortex binding and the KT transition
- 2D XY model and its partition function
- Topological defects and vortices
- Decomposition of gradient into regular and topological parts
- Coulomb interaction between topological defects
- Core energy and single-defect partition function
- Grand canonical Coulomb gas partition function
- Dielectric screening by bound vortex pairs
- Renormalization group recursion relations for k and y
- XY model and low-temperature spin correlations
- Topological defects (vortices) in the XY model
- Energy and entropy balance for a single vortex
- Coulomb gas representation of many vortices
- Renormalization group (RG) flow equations for the Coulomb gas
- RG flow diagram and the KT phase transition
- Universal jump in superfluid density at the KT transition
- Experimental verification via superfluid helium films
- Essential singularity of the correlation length above Tc
- Two-dimensional melting and dislocation unbinding
- 2D elastic solid and strain tensor
- Translational order parameter and quasi-long-range order
- Dislocation unbinding and melting of translational order
- Orientational order parameter and bond angles
- Orientational correlations decay to a constant in the solid
- Hexatic phase with quasi-long-range orientational order
- Disclinations and orientational order melting
- KTHNY two-transition melting scenario
- Langevin equation and dissipative dynamics
- Time-dependent Landau-Ginzburg equation
- Critical slowing down and dynamic relaxation times
- XY model vs. isotropic solid analogy
- Goldstone modes and symmetry breaking
- Elastic energy and elastic moduli
- Fourier-space representation of elastic energy
- Displacement fluctuation correlators
- Long-range order and the Mermin–Wagner theorem
- Power-law correlations in 2D and the KT transition
- Lattice periodicity and the displacement ambiguity
- Density-wave order parameter ρ_G
- Landau-Ginzburg free energy functional
- Dissipative dynamics and Brownian motion analogy
- Time-dependent Landau-Ginzburg equation
- Linearization and Fourier mode decomposition
- Mode relaxation times and critical slowing down
- Relationship between correlation length and relaxation time
- Dynamic critical exponent z
- Conserved versus non-conserved order parameter dynamics
Syllabus
Lectures
- 1. Collective Behavior, from Particles to Fields Part 1
- 2. Lec 1 (continued); The Landau-Ginzburg Approach Part 1
- 3. The Landau-Ginzburg Approach Part 2
- 4. The Landau-Ginzburg Approach Part 3
- 5. The Landau-Ginzburg Approach Part 4
- 6. The Scaling Hypothesis Part 1
- 7. The Scaling Hypothesis Part 2
- 8. The Scaling Hypothesis Part 3
- 9. Perturbative Renormalization Group Part 1
- 10. Perturbative Renormalization Group Part 2
- 11. Perturbative Renormalization Group Part 3
- 12. Perturbative Renormalization Group Part 4
- 13. Position Space Renormalization Group, Part 1
- 14. Position Space Renormalization Group, Part 2
- 15. Series Expansions Part 1
- 16. Series Expansions Part 2
- 17. Series Expansions Part 3
- 18. Series Expansions Part 4
- 19. Series Expansions Part 5
- 20. Continuous Spins at Low Temperatures Part 1
- 21. Continuous Spins at Low Temperatures Part 2
- 22. Continuous Spins at Low Temperatures Part 3
- 23. Continuous Spins at Low Temperatures Part 4
- 24. Dissipative Dynamics
- 25. Continuous Spins at Low Temperatures Part 5
- 26. Continuous Spins at Low Temperatures Part 6