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Vorlesungsnotizen/Lecture Notes:
Quantenfeldtheorie I/Quantum Field Theory I
Prof. Michael G. Schmidt
Bücher/Literature
Inhalt/Contents
- Introduction
- Short repetition of quantum mechanics
- Observables
- Time evolution and Heisenberg equation
- Field equations
- Heisenberg uncertainty relation
- Interactions and Feynman graphs
- Perturbation theory
- The free electromagnetic field, coherent states
- Coherent states for harmonic oscillator
- Coherent states and classicality
- Coherent states are overcomplete
- Operators in the coherent state representation
- The free electromagnetic field (without sources)
- The hamiltonian for the electromagnetic (EM) field
- Naive quantization of the EM field
- Induced emission/absorbtion, spontaneous emission
- Electromagnetic waves in coherent state representation
- Exercise 1
- Exercises 2 and 3
- Canonical formalism for the wave equation (Klein-Gordon equation)
- Field equation
- Klein-Gordon equation
- Klein-Gordon equation for massive particles
- Quantization
- The Hamiltonian in the N-representation
- Maxwell's equations in the Lagrange Formalism
- Maxwell's Lagrangian in the Coulomb gauge
- Schrödinger equation in the language of field quantization ("2nd quantization")
- Lagrange formalism for the Schrödinger equation
- Heisenberg equation for the second quantized `wave function'
- The number and momentum operators
- The Hamiltonian in the second quantized formalism
- Multiparticle Schrödinger equation
- Construction of multiparticle states
- Interactions in the second quantized formalism
- Fermions and the Fermi-Dirac statistics
- The Fock space for fermions
- Multiparticle fermionic states
- Relativistic covariance; the Lorentz and Poincaré group
- Properties of symmetry transformations
- Lie algebra of a symmetry group
- Relativistic invariance/covariance; Lorentz transformation
- Lorentz transformation of the metric tensor and vectors
- Lorentz group
- Lorentz algebra
- Lorentz boosts and the small group (rotations)
- Poincaré group
- Relativistic particles as unitary representations of the Poincaré group
- Representations of the small group
- Plane waves and Lorentz transformation
- Covariant field equations and their quantization
- A general solution of the Klein-Gordon equation
- Canonical quantization of the Klein-Gordon (scalar) field
- Hamiltonian of the Klein-Gordon field
- Canonical quantization of a complex scalar field
- Charge conjugation
- Charge conjugation in scalar electrodynamics
- Microcausality
- Transition to the nonrelativistic theory
- Transition to the nonrelativistic theory (cont.)
- The Dirac equation and its quantization: 0. Spinor representation of Lorentz group
- The Dirac gamma matrices
- Direct construction of the representation matrices in spinor space
- Lorentz boosts in spinor space
- Dirac spinors in terms of Lorentz representation matrices
- Transformation of the Lorentz spinor by the spinor representation matrices
- The Dirac field equation
- Representations of the Dirac algebra: Weyl or chiral representation
- The Dirac-Pauli representation
- Relativistic covariance of the Dirac field equation
- Charge conjugation C
- More on charge conjugation
- Projection operators onto positive and negative energy states
- The Lagrange and Hamilton functions for the spinor fields
- Quantization
- The creation and annihilation operators and the Fock space
- Charge conjugation revisited
- Clifford algebra and bilinear covariants
- Quantum mechanical interpretation of the Dirac equation and its nonrelativistic limit; the Foldy-Wouthuysen transformation
- Positive and negative energy solutions
- Nonrelativistic limit
- The Pauli equation
- The Foldy-Wouthuysen transformation
- The Foldy-Wouthuysen transformation in presence of a constant electromagnetic field
- The Darwin term and the Thomas factor
- The hydrogen atom
- The hydrogen atom and the Foldy-Wouthuysen transformation
- Symmetries and conservation laws
- Noether theorem
- Translation invariance and energy-momentum tensor
- Energy momentum tensors for the Klein-Gordon, Dirac and Maxwell fields
- Invariance under Lorentz transformations
- The orbit-angular momentum and spin density tensor
- Discrete symmetries: space inversion (parity)
- Discrete symmetries: time reversal
- Discrete symmetries: charge conjugation
- CPT theorem
- Interacting fields, vacuum expectation values, S-matrix
- Interaction of particles in QFT and S-matrix
- The Yang-Feldman equation
- The Yang-Feldman equations and the in and out states
- The two-point functions (propagators)
- The retarded and advanced propagators
- The spectral representation of the commutator vev; the
Kaellen-Lehmann bound on Z
- The LSZ reduction formalism
- The LSZ reduction formalism (continuation)
- The LSZ reduction formula for bosonic fields
- The LSZ reduction formula for fermionic fields
- Generating functional for the scattering operator
- X. Invariant perturbation theory. 1) Dyson expansion
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- 2) Wick Theorem
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- 3) Feynman graphs
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- 4) Back to S-matrix elements
- 4)
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- 5) Feynman rules for other interacting theories (a) Complex scalars
- 5) (b) Yukawa coupling
- 5) (c) Quantum electrodynamics
- 6) A simple example in Yukawa theory
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- 7) From S-matrix to the Cross Section
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