Methods of QFT in Condensed Matter Physics

TMP-TA4, WiSe-2014/15

 

Lecturer: Dr. Oleg Yevtushenko,    Tutor: Dennis Schimmel

 

Lecture topics:

1)          Introduction: From classical field theory to effective field theory of lattice vibrations.

 

                              PI in quantum mechanics, tunnelling – instanton solution

 

2)          Derivation of the Feynman path integral (PI) for the evolution operator.
 

3)          Quantum tunnelling: the Instanton solution – Part I (substitution by Dennis Schimmel).

4)          Quantum tunnelling: the Instanton solution – Part II (substitution by Dennis Schimmel).

         Useful notes for Lect-s. No.3 & 4 (by Prof. A. Nersesyan) can be found here.

5)          ϕ4-theory for the classical Ising model vs. quantum tunnelling. Linear response theory, response functions (operator approach).

 

                              Correlation functions, many particle systems, from PI to FI

6)          The PI for correlation functions, source fields, generating functionals. QFT-Stat.Phys. correspondence.

7)          Coherent States (CS) for fermions and bosons, Grassmann variables. How to express the partition function as the FI over CSs.

         Useful notes about CSs and Gaussian integrals (kindly provided by Lode Pollet) can be found here.

8)          FI for the generating functional, boundary conditions for fermionic/bosonic fields; Gaussian integrals. Free energy of a non-interacting gas.

                              Interacting fermions: normal metals and superconductors

9)          Basic properties of the Fermi liquid, life-time of single particle excitations; free energy of weakly interacting fermions from FI.

10)          Selection rule for the loop-diagrams, free energy in the RPA, polarization operator, screening, plasmons.

11)          Hubbard-Stratonovich transformation, 3 interaction channels. The density channel: the MF approximation.

12)          RPA from fluctuations around the MF. Superconductivity: basic properties, the BCS model.

if you do not remember basics of theory of superconductivity you may look at the lectures notes from Mesoscopics, SoSe-2013

13)          The Cooper channel, ladder diagrams, the Cooper instability; the BCS GS, the BCS theory as the MFA.

14)          FT for superconductors: matrix GFs, the gap equation from the saddle-point. The Ginzburg-Landau theory from FI.

15)          Fluctuations in the GL theory; spontaneous symmetry breaking and Goldstone modes, action for the phase.

16)          Part 1 of L-16: Londons’ equations.

               Luttinger Liquid, Abelian bosonization

16)        Part 2 of L-16: Non-FL effects, peculiarity of low-dimensional systems; 1D: Tomonaga-Luttinger model (1d massless fermions).

17)        Dzyloshinkii-Larkin diagrammatic solution: loop cancellation, effective interactions; the Ward identity, non-FL GFs; Bosonization.

18)        Bosonization from FI: alternative proof of loop cancellation, gauge transformation and Jacobian, effective bosonic action.

19)        Luttinger Liquid: chiral & dual fields, correlations functions, LDoS and ZBA, LL with a potential scatterer, RG method.

 

FT on the closed time-contour, NEGFs, kinetic equation

 

20)        Real-time formulation of FT for arbitrary systems, closed time contour. Example of a Bose gas: partition function, discretized time and 4 GFs.

21)        Keldysh rotation, independent GFs, continuous limit, causal structure, FDT, source fields, cumulants in discretized-/continuous representations.

22)        FT for a Fermi gas on the closed contour: GFs, causality, source fields. Matrix structure of the polarization operator, causality, FDT.

23)        Action for interacting systems, the matrix Dyson equation; scale separation, the Wigner transform, derivation of the semiclassical kinetic equation.

24)        Screening, the structure of the interaction propagator and of  in the RPA; calculating . Collision integral for interacting fermions, in-/out- terms.

 

Additional 4 lectures

               Introduction to the FT of disordered systems & Integer Quantum Hall effect (if time permits)

 

Last update: 27.01.2015