Statistical Physics (2017)
Statistical mechanics enables us to probabilistically model the behavior of macroscopic systems, which are made up of large numbers of identical microscopic constituents for which we only have incomplete description. It bridges the disconnect between mechanics which requires complete knowledge of initial conditions, and the real world where such information is not available. These ideas therefore find widespread application.
This page will be updated regularly with course-related information. Please check frequently.
Any comments and/or suggestions about special interests/requests, pre/during/post-course are highly welcome. I am available over email (ALWAYS include the tag "SP2017" in the subject line to ensure my spam filter doesn't reject it). You can send anonymous emails if you prefer. No promises to act on any of them unless I think it will be useful for a majority of the class.
Administrivia
Time: 11:30 AM, Tuesdays and Thursdays
Venue: AG 69
First lecture: Thursday, 2 Feb 2017
Credit policy: 25% from 5 problem sets + 25% from mid-semester exam + 50% from end-term exam
Instructor: Basudeb Dasgupta
Tutors: Subhajit Ghosh (DTP) and Mayank Narang (DAA)
Target Audience
This is the core course SP-1 or P-204 in the TIFR graduate school. Students who have joined after their B.Sc. or M.Sc may both take this course.
Course Contents
1. Preliminaries: Motivation and review of thermodynamics (3 lectures)
2. Probability and statistics: Counting, distributions, large numbers (3 lectures)
3. Kinetic theory and approach to equilibrium (5 lectures)
4. Classical statistical mechanics: Formalism and simple systems (4 lectures)
5. Classical statistical mechanics: Interactions, approximations, phase transitions (4 lectures)
6. Quantum statistical mechanics: Formalism, ideal Bose/Fermi gases, phase transitions (6 lectures)
7. Beyond SP-1 (1 lecture)
+ 4 problem solving sessions & review lectures
References
1. Statistical Mechanics of Particles, Kardar (Main text, but very terse. The videos are highly recommended.)
2. Statistical Mechanics, Huang (I personally find it most readable)
3. Statistical Physics (Berkeley Physics Course Vol.5), Reif (easier than others)
4. Statistical Mechanics Part-I (Course of Theoretical Physics Vol.5), Landau and Lifshitz
5. Lecture notes by David Tong, Cambridge Univ. (Kinetic Theory, Statistical Mechanics)
6. Statistical Mechanics, R. P. Feynman (especially for solids, density matrices, and the later chapters)
Problem Sets
PS1 (Thermodynamics) (on 7 Feb, due 21 Feb)
PS2 (Probability and Kinetic Theory) (on 21 Feb., due 21 March)
PS3 (Classical Stat. Mech.) (on 21 March, due on 11 April)
PS4 (Interacting Classical Stat. Mech.) (on 11 April, due on 4 May)
PS5 (Quantum Stat. Mech.) (on 27 April, due on 23 May)
Exams
1. Drop-test on 11 Feb (10 AM, A 304)
2. Mid-term on 1 April (2 PM, AG 69)
3. End-term on 27 May (2 PM, AG 69)
Lecture Summaries
Lecture 1 (2 Feb): Orientation
Syllabus
Logistics
Calibration
Lecture 2 (7 Feb): PS1 handed out. Thermodynamics I
Motivation
Definitions and basic notions in thermodynamics
0th Law: Statement; Consequence = T exists; Application = Thermometer
1st Law: Statement = E exists if walls adiabatic, and Q defined by energy conservation
Lecture 3 (9 Feb): Thermodynamics II
2nd Law: Kelvin and Clausius statements. Equivalence.
Carnot cycle, Carnot theorem
Clausius theorem
Definition of entropy S
Potentials and how to get appropriate derivatives
Extensivity (Gibbs-Duhem relation between intensive variables) and Maxwell relations
Applications: dmu/dP|_T = V/N or dv/dN|_T,P ; dS/dJ|_X = dX/dT|_S etc.
Lecture 4 (14 Feb): Thermodynamics III
Third Law: Weak and Strong Statement, Justification, Consequences (dS/dX,C,etc vanish)
Relations from equilibrium (T,P,mu,.. same)
Relations from stability (Second derivatives of S are negative)
Application: Critical point in PV plane of real gas (dP/dV, d^2P/dV^2 is zero, Third derivative -ive, Maxwell construction for van der Waals EOS)
Clausius-Clapeyron equation for P(T)
Gibbs Phase Rule: # of intensive variables needed = N_work + 1 + C_components - P_phases
Lecture 5 (16 Feb): Probability I
Definitions of probability: objective (occurrence frequency) and subjective ("reasonable" expectation)
Counting methods (Basic, Permutation, Combination, Partition, Generating function)
Bayes theorem p(A&B) = p(A|B)p(B) = p(B|A)p(A)
Lecture 6 (21 Feb): PS1 due. PS2 handed out. Probability II
CPF, PDF, expectation, CF = characteristic function as the Fourier transform of PDF, moments from power series of CF = MGF, cumulants from power series of log(CF) = CGF
Graphical trick relating cumulants and moments
Explicit computation for Gaussian, Binomial, Poisson PDFs
Lecture 7 (23 Feb): Probability III
Probability distribution of many variables
CPF, PDF, CF, MGF, CGF, Conditional and Unconditional PDFs of many variables
Graphical trick for many variables
Joint Gaussian ~ Product of gaussians
Statement of Weak law of large numbers, Statement and Proof of Central Limit Theorem (without assuming iid) ~ sum of random variables has Gaussian PDF
Sum of exponential(N*x) ~ exp(N*x_max)
Saddle point approximation to integrals and Stirling's approximation
Entropy as information in a PDF
Information I[{p_i}] = ln(M) - S, and Entropy of a PDF S[{p_i}]= - sum_i p_i ln(p_i)
Maximum Entropy Method as a formalization of subjective assignment of probability.
Claude Shannon and encoding info (See Shannon's 1950 paper on information and language. See also page 12-14 of his 1948 paper)
Lecture 8 (28 Feb): Kinetic Theory (Hamiltonian dynamics)
Last bit of Probability theory: Saddle point, Shannon information and entropy, MEM
Macrostates and microstates
Hamilton's equations
Lecture 9 (2 Mar): Kinetic Theory (BBGKY)
rho(p,q) as the full 6N dimensional probability dist. for N-particles
measurement O as an expectation value
Liouville's theorem: uncompressibility of rho
Consequences: T-reversal, evolution of O, equilibrium exists and is defined by rho = rho(E)
1 particle density, s-particle density
BBGKY hierarchy for N particles with pairwise interactions
Lecture 10 (7 Mar): Kinetic Theory (Route to Equilibrium I: BBGKY to Boltzmann eqn.)
BBGKY -> Boltzmann equation using dilute approx. + molecular chaos + coarse-graining + separation of scales
Interpreting the Boltzmann equation and irreversibility
Lecture 11 (9 Mar): Kinetic Theory (Route to Equilibrium II: H theorem, local equilibrium, Hydrodynamics)
Statement and proof of H theorem, Loschmidt paradox, Poincare recurrence
See this Article by Cedric Villani (much of it is easy to read) on the mysteries of the Boltzmann equation
Local equilibrium for all except conserved qtys.
Properties of local equilibrium (Boltzmann-like but position and time dependent)
Approach to full equilibrium (f_2 -> f_1*f_1 at intrinsic time-scale, local equilibrium at t_mfp, global equilibrium at t_eq >> t_mfp, e.g., t_ballistic^2/t_mfp)
Hydrodynamic equations for collisionally conserved quantities
Deriving the hydrodynamic equations (Continuity, Navier-Stokes, Heat-flow)
Physical meaning of the terms in the equations
Lecture 12 (14 Mar): Kinetic Theory (Route to Equilibrium III: Hydrodynamics)
Zeroth order: Sound waves, but no dissipation, Shear, Heat-flow
First order: Shear, Heat-flow
Global equilibrium
Lecture 13 (16 Mar): Problem solving and review
Steady Atmosphere
Benford's Law
Lecture 14 (21 Mar): PS3 handed out. PS2 due. Classical Stat Mech (Foundations, Microcanonical)
From Hamilton's eqns to Phase space: Recap
Volume in phase space, introduce 1/h^3N, number of microstates W, density of states
Ergodicity and Mixing
Fundamental Postulate of Statistical Mechanics and its justification via i) MEM, ii) Dynamics
Lecture 15 (23 Mar): Classical Stat Mech (Microcanonical)
Macrostate = M(E,X,N), microstate = mu(p,q)
p(mu) = 1/W(E), where W(E) = # of microstates within energy E and E-dE
1/T=dS/dE|_V,N
Derivation of 0th, 1st, 2nd Law
Ideal gas thermodynamics and "microscopic" info
Fixing non-intensive mu, Mixing entropy using 1/N! factor
2 level systems and negative temperatures (Observation of Negative T)
Holiday (Gudi Padwa) (28 Mar)
Lecture 16 (30 Mar): Problem solving and review
Midterm Exam (1 April): AG 69, 2 PM onwards. Open book.
Score Distribution
Lecture 17 (4 April): Classical Stat Mech (Canonical)
Canonical Macrostate M(T,X,N), microstate = mu(p,q)
p(mu) = exp(-E/kT)/Z
Canonical Partition Function Z = W(E) exp(-E/kT) sum over E
E -> F = E - TS and Z = exp(-F/kT) sum over F
Energy fluctuations in CE: Why E_most-prob = <E> + O(1/sqrtN)
Z_N = Z_1^N ; include 1/N! if indistinguishable
Ideal gas and variations in D, dispersion relation, multiple dofs
Lecture 18 (6 April): Classical Stat Mech (Gibbs and Grand Canonical)
Gibbs Canonical Macrostate = M(T,J,N), microstate = mu(p,q)
E -> G = E - TS - JX, and Z = exp(-G/kT) sum over G
Ideal gas in isobaric ensemble
Grand Canonical Macrostate = M(T,X, mu), microstate = mu(p,q)
Number fluctuations in GCE
Ideal gas in GCE
Lecture 19 (11 April): PS4 handed out. PS3 due. Approximations (Cumulants)
Interacting systems and approximation techniques
Series expansions / perturbation theory
Cumulant expansion and failure for hard core type interactions
Lecture 20 (13 April): Approximations (Cluster)
Cluster expansion
Virial series for P
Comments
Lecture 21 (18 April): Approximations (Mean field)
Mean Field Theory of Condensation
Proof & Meaning of Maxwell Construction
The search for Universality
Lecture 22 (20 April): Approximations (Critical Phenomena and Monte Carlo)
Weiss Mean Field Theory for Ising Model
Critical Exponents, Universality, and Heuristic Justification
Ordinary Monte Carlo and its Failure
Basic Markov Chain Monte Carlo
Metropolis Algorithm
Lecture 23 (25 April): Problem solving and review
Lecture 24 (27 April): PS5 handed out. Quantum Stat Mech (Old QM)
Issues with Classical Stat Mech
Quantization a la Old Quantum Mechanics
Vibrations, Rotations, and Blackbody Radiation
Lecture 25 (2 May): Quantum Stat Mech (Formalism and Density matrix)
From classical to quantum: microstates, macrostates, probability density (matrix)
The ensembles: microcanonical and canonical
Canonical density matrix of 1 particle
Interpretation in terms of classical and quantum uncertainty
Lecture 26 (4 May): PS4 due. Quantum Stat Mech (Anti/Symmetrization and multi-particle states)
Exchange symmetry of wavefunction of 2 identical particles
Hilbert space of N identical particles and normalization
See this link for a nice primer on quantum mechanics of many particles
Canonical density matrix of N particles
Lecture 27 (9 May): Quantum Stat Mech (Canonical and Grand Canonical Ensembles)
N particle Hilbert space, density matrix, product state basis, entangled states, reduced density matrix
Interpretation of canonical density matrix in terms of statistical attraction/repulsion
Grand Canonical Ensemble
Lecture 28 (11 May): Quantum Stat Mech (Ideal Quantum Gas at High T)
Ideal gas in GCE
High T limit of ideal gas and virial expansion
Lecture 29 (16 May): Quantum Stat Mech (Degenerate fermions)
Sommerfeld expansion in small T limit, i.e. z >> 1
Why fermions are simple: Fermi surface
mu, P, E, C_v, etc.
Lecture 30 (18 May): Quantum Stat Mech (Degenerate bosons)
Why z cannot exceed 1 : Bose Einstein condensation
What happens to mu close to z = 1?
mu, P, E, C_v, etc.
Lecture 31 (23 May): PS5 due. Beyond SP-1
More examples, interactions, bands, superfluidity
Lecture 32 (25 May): Problem solving session and review
27 May: Endterm exam (AG 69, 2 PM onwards. Open notes) and End of Course
Grades and Break-Up into Assignment, Midterm, and Endterm
Congratulations!